METHOD OF PROCESSING, ANALYSING AND DISPLAYING MARKET INFORMATION

Abstract: Method of interactive user controlled processing of graphical images for financial data analysis, by means of a data processing system and software including the steps of: acquiring financial parameter data on a financial parameter to be analysed in digital or electronic format; calculating and depicting on a screen one or a plurality of broken lines, representative of the evolution of the financial parameter and drawn in such a way that when each new point of said broken line is plotted, its coordinate along a first axis (T-axis) is always incremented by tau and its coordinate along a second axis (R-axis) is always changed either by +<i>r</i> or by -<i>r</i>, where one of said tau or <i>r</i> values has to be specified by the user.

Description: Method of Processing, Analysing and Displaying Market Information BACKGROUND This invention relates to a method of processing, analysing and displaying information, in particular market information, to assist traders and investors in analysing and forecasting the movement of stock market values based on recorded historical information. The analysis of stock market values or other parameters based on historical information is a specialist field of activity called "Market Technical Analysis", or simply "Technical Analysis". The ultimate goal of performing technical analysis is usually to assist the trader or investor in deciding whether to buy or sell market values, for example currencies, shares or values related to market indexes. Conventional technical analysis is typically performed by an analyst studying charts of historical parameter changes presented on a computer screen, for example, and applying his experience and knowledge to determine possible trends or trend changes. The parameter is a price or index value for example, selected over certain time frames, such as hourly, daily, weekly, monthly, etc. The technical analyst uses certain tools to help analyse the information, for example he may draw "support" and "resistance" lines through low and high peaks respectively to determine the band within which the parameter fluctuates. If the analyst considers that the lines drawn are very representative of the market trend, a drop of the value below the "support" line may be an indication of the trend reversal suggesting a sell decision, and conversely, a rise above the resistance line would tend to indicate a buy decision. A technical analyst will probably look simultaneously at different time frames to distinguish between larger and shorter term trends. Knowledge of "market psychology" and the company or value to which the parameter relates will strongly influence the analyst's perception of the information he is analysing. The conventional analyst thus primarily bases his forecast on intuition and experience, the information analysis tools at his disposition being graphical aids of a very simple nature. It would be a distinct advantage for an investor or trader if market values could be analysed in a more systematic and structured manner, relying less on intuition and guesswork than the present methods. SUMMARY OF THE INVENTION An object of this invention is to provide a method and a set of tools therefor to assist a technical analyst, trader or investor in analysing and forecasting the movement of market values in a more structured and systematic manner than prior to this invention. Another object of this invention is to provide a technical analyst, trader or investor with electronically calculated and generated lines on top of a chart, such as possible support and resistance lines and parameter development trajectories that assist the analyst in forecasting movements or waiting for clearer market situations. Objects of the invention have been achieved by providing a method of processing, analysing and displaying information according to the independent method claims, or as set forth in the following description. Objects of the invention have been achieved by providing software program modules according to the independent program module claims or as set forth in the following description. Advantageous aspects of the invention are set forth in the dependent claims or will be apparent from the following description and drawings. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a graph of the daily bar of the exchange rate Euro / US Dollar over the period April 20, 1998 to January 28, 2000 ; Fig. 2 is a graph of the section P1a-P1b of Fig. 1 after parameter-normalization in Increment-Change Space according to the invention, whereby the vertical axis represents the amplitude of the exchange rate stated as the number of measurement increments r where r - 0.005, and the horizontal axis represents the number of successive registered measurement steps ; Fig. 3 is a detailed view of a portion of the trajectory of Fig. 2 ; Fig. 4 is a graph showing five different parameters after transformation by parameter-normalization and superposition by aligning their starting points; Fig. 5 is a graph showing a curve representing the average of the five trajectories of Fig. 4 ; Fig. 6A is a detailed graph of a portion of the real curve of Fig. 1 ; Fig. 6B is a graph in parameter-normalized Increment-Change Space of a beam of two trajectories based on the curve of Fig. 6A ; Fig. 7A is a graph in Increment-Change Space of the section P1a-P1b of Fig. 1 after transformation to a beam comprising two trajectories representing the same section, but where the starting point of one trajectory relative to the other has been phase-shifted by r/2 ; Fig. 7B is a graph showing a beam-average curve in Increment-Change Space representing the average of the two trajectories of Fig. 7A; Fig. 7C is a graph showing a beam-average curve in Increment-Change Space representing the average of the 200 trajectories as derived from the section P1a-P1b of Fig.l Fig. 8A is a graph of the same portion of curve as Fig. 6A ; Fig. 8B is a graph in time-normalized Increment-Change Space of a beam of two trajectories based on the curve of Fig. 8A ; Fig. 9A is a graph in Increment-Change Space of the section P1a-P1b of Fig. 1 after time-normalized transformation to a beam of two trajectories, the phase shift being τ - r/c-2 days; Fig. 9B is a graph showing a beam-average curve in time-normalized Increment-Change Space representing the average of the two trajectories of Fig. 9A ; Fig. 10 is a graph of a trajectory in parameter-normalized Increment-Change Space of the section P a-P1b of Fig. 1 , whereby r= 0.02 ; Fig. 11 is a graph of the ratio of the calculated parameter localization error ΔR and the experimentally measured value ΔR exp of the trajectory sections of Fig. 10 ; Fig. 12 is a graph of the line slop 1/n as a function of the measurement increment value r of point P1b of Fig. 1 after transformation in Increment- Change Space with different measurement increment values r ; Fig. 13A is a scheme view showing a section of a trajectory in parameter- normalized Increment-Change Space illustrating a possible direction of the compatible trend; Fig. 13B is a scheme showing a section of a trajectory in parameter-normalized Increment-Change Space illustrating a possible direction of the compatible trend. Fig. 14 is a graph in parameter-normalized Increment-Change Space over the period from October 1999 to January 2000 of the Dow Jones Industrial Average index (DJIA) where the measurement error r= 50; Fig. 15 is a graph in time-normalized Increment-Change Space of sections P1a- P1b of Fig. 1 where rl c = 2 days; Fig. 16 is a graph in parameter-normalized Increment-Change Space of the exchange rate Euro / US Dollar of the sections P1a-P1b of Fig. 1 , where r = 0.005; Fig. 17 is a graph in parameter-normalized Increment-Change Space of the DJIA index since its conception to the year 2000, where r = 500; Fig. 18 is a graph similar to the first part of Fig. 17 (from the starting point until point 71), but with the value r= 300; Fig. 19 is a graph in parameter-normalized Increment-Change Space of the DJIA index since conception with three different trajectories representing trajectories where r = 300, r= 400, and r= 500, respectively, the horizontal axis representing the number of measurement increments and the vertical axis representing the number of measurement values r (such that the DJIA value is different for each trajectory at the same number of measurement steps, for example at number 5 on the vertical axis, the DJIA values for the trajectories are 1500, 2000 and 2500, respectively); Fig. 20 is a graph of the square of the mean values of the trajectories of Fig. 19 ; Fig. 21 is a graph of the relation between the square of the parameter and t/τ for the trajectory of Fig. 9B in time-normalized Increment-Change Space with τ = 2 days ; Fig. 22 is a graph in Increment-Change Space depicting the Euro/USD rate over the period April 20, 1998 to January 28, 2000 (as in Fig.1) after parameter- normalization with Λ=0.0206. Starting from point 2 a beam comprising 100 trajectories is obtained. The beam-average curve B22 is shown together with the fastest trajectory F22. The support and resistance lines are superimposed on the graph. Fig. 23 shows the same graph as Fig. 22. Starting from point 2 the smoothing procedure is applied to the fastest trajectory F22 from Fig. 22. Both the trajectory F23 and beam-average curve B23 smoothed are shown. The number of smoothing iterations is equal to 4. Four quantum lines with n=1 , n=2, n=3 and n=4 are plotted from point 2. Fig. 24 is a graph of the USD/CHF rate obtained over the period from April 15, 2001to May 12, 2001. Each point represents the average quote for 10 minutes bar (data supplied by Reuters). Fig. 25 shows the graph from Fig. 24 after parameter-normalization in Increment-Change Space with increment value r=0.003. The variants of the support (S25a, S25b, S25c) and resistance (R25a, R25b, R25c) lines are shown. The development equation curve D25 is drawn starting from point 5 with the value of q equal to q max =3.36. Starting from point 6 both the fastest trajectory F25 and the beam-average curve B25 are also shown after the application of ten smoothing iterations. The 7 quantum lines are shown for point 6. Fig. 26 is a schematic view of the overall structure of a data processing system according to the invention. Fig. 27 is a flowchart describing one from many possibilities to calculate the recommended minimum value of increment r. The program module is part of the software developed. Fig. 28 is a flowchart describing the transformation of real market data into a trajectory in Increment-Change Space. The program module is part of the software developed. Fig. 29 is a flowchart describing the smoothing procedure applied to a trajectory in Increment-Change Space. The program module is part of the software developed.. Fig. 30 is a flowchart describing the plotting of trend lines. The program module is part of the software developed. Fig. 31 is a flowchart describing the calculation of the value of q max . The program module is part of the software developed. Fig. 32 is a flowchart describing the calculation and drawing of the second trend line on the basis of the first line chosen. The program module is part of the software developed. Fig. 33 is a flowchart describing the splitting of real market data into a beam of trajectories in the Increment-Change Space. The program module is part of the software developed. Fig. 34 is a flowchart describing the determination of the fastest trajectory for the beam in the Increment-Change Space. The program module is part of the software developed. Fig. 35 is a flowchart describing the calculation of the beam-average curve in the Increment-Change Space. The program module is part of the software developed. Fig. 36 is a flowchart describing the drawing of quantum lines in the Increment- Change Space. The program module is part of the software developed. Fig. 37 is a flowchart describing the drawing of the development equation curve in the Increment-Change Space. The program module is part of the software developed. DETAILED DESCRIPTION OF THE INVENTION I. THEORY UNDERLYING THE INVENTION The invention is based on a new theory of evolution proposed by the inventor, particularly as applied to the evolution of market parameters. The inventor's premise is that the movement of market prices or other market parameters can be described by the laws of physics, and specifically the laws of motion of material objects. The inventor postulates the following: The principle of universality: The laws governing changes in measured material parameters are universal, recurring laws true for all types of matter, material objects and measuring instruments. 1. 1) Fundamental laws of evolution From a conceptual point of view, one may consider that an observer receives information on the material world by registering changes in material parameters, and the observer registers changes in material parameters by taking measurements by means of instruments. The process of observing material parameter changes is objective and is carried out by taking measurements. The measurement produces a number. The number that reflects a material parameter cannot be exact. The measuring process inevitably entails a measurement error which can be greater or smaller and which depends on the method of measurement and the instrument used. Parameter changes with an amplitude smaller than the measurement error will not be registered. Let us assume that the measurement error appears as a scale unit of the instrument used. The scale unit may therefore be considered to be the increment change that is detected and therefore registered by the instrument used. Thus, any material parameter can be represented as a pair of numbers, where R is the value proper and r is a measurement increment. Each time one registers a new parameter value that differs from the preceding one, the registered parameter change will be equal to the discrete measurement increment such that the value of any material parameter can be represented by an integer number multiplied by a measurement increment r. The scale of change determined in this way and calibrated in integer numbers does not depend on the instrument and complies with the principle of universality. The inventor thus proposes the following: First law of evolution: Registered change is always a measurement increment. What this in fact means is that the world that we are cognizing is "discrete". No one will ever be able to observe the continuous (non-discrete) changes of material parameters. Thus, the process of change can be described as a sequence of changes of integer numbers in time. On the premise that the theory described herein is universal and therefore true for all material objects without exception we shall consider a particular case and extend it to all others. If one records the change in spatial coordinate of light with an appropriate instrument, the motion will be composed of identical steps, each equal to a discrete increment of distance. If one redefines "time" as a number of registered changes (hereinafter "Evolution Time"), the clock will always be constructed of the same form of matter as that to which the parameter under examination belongs. On the basis of the principle of universality, the inventor extends this definition of time to all forms of matter and material objects as his second law. Second law of evolution: The length of time of change is proportional to the number of successively registered changes. This means that "Evolution Time" stands still if the amplitude of changes in the real parameter is less than the specified measurement increment r. One can construct a two dimensional space for which the universality principle holds true, with one coordinate axis representing the parameter value (for example price) as a number of measurement increments r, and the other coordinate axis representing Evolution Time as the number of successively registered changes. A change in parameter is registered when the difference between the last registered parameter and the newly measured parameter equals the chosen value of the measurement increment r. We shall hereinafter call this two- dimensional space "Increment-Change Space". It may be noted that the aforesaid Increment-Change Space is dimensionless, since the Y-axis is a sequence of integers representing a number of measurement increments, and the X-axis is also a sequence of integers representing a number of successively registered changes. A parameter in Increment-Change Space is often relative in a double sense: first, it is frequently used as integer and, second, it is often convenient to set its starting point to zero. In the present application, notions derived from the quantum theory are used to describe the movement of a market parameter in Increment-Change Space. In other words, the movement of a market parameter in Increment-Change Space is considered analogous to the motion of a wave-particle (electron, photon...) and subject to physical laws applying to wave-particles. By analogy, the following terms describing the value of a market parameter over time, after transformation in Increment-Change Space, will be used in this application: - parameter change trajectory, or simply "trajectory": shall mean the curve or line plotting the movement of a market parameter in Increment-Change-Space - mass: shall mean a fictive mass given to a parameter change particle or particles - parameter change particle: shall mean a point following a single trajectory in Increment-Change Space - parameter change trend, or simply "trend": shall mean the average linear direction of a trajectory in Increment-Change Space - parameter change beam, or simply "beam": shall mean a plurality of trajectories in Increment-Change Space, each representing the same parameter at the same measurement increment r but with shifted real starting points - phase shift: shall mean shifting the starting measurement point when transforming a real parameter curve to a trajectory in Increment-Change Space - velocity: shall mean the rate of change of the parameter, as represented by the slope of the trend in Increment-Change Space. Considering the above, changes of a market parameter (for example the price of a share on the stock market) over real time can be expressed in Increment- Change Space by applying the following system of equations and inequalities: Registration of a new parameter value in Increment-Change Space takes place if the following condition is met: where: ^ is the current va ue o the parameter in real space; is a value IR I < r which meets the condition ' /! , chosen in such a way as to facilitate splitting into a beam or effecting a "phase shift"; ώfel is the current (latest) registered value of the parameter in Increment-Change Space; the term appearing in the left-hand part of the inequality diminishes abruptly each time a new parameter value is registered; and d ^ m is the parameter value by which the parameter scale in Increment-Change Space is shifted in relation to the parameter scale in real space; this makes it possible to combine the starting R = 0 point of the trajectory with the start (zero point) of the coordinates s in D _ n Increment-Change Space. The starting point ^ is often used for convenience. At the same time nothing is changed in principle if the starting point is fixed by some other value. The values of the parameter ώfe allowed in Increment-Change Space are determined in accordance with the following equation: where: / = 0, 1, 2, 3... is a series of integers, and r > 0 is the increment or the absolute value of the difference between any two adjacent parameter values successively registered in Increment-Change Space. The time interval ^ ώfe in Increment-Change Space is also a discrete sequence of values where: N = 0, 1, 2, 3... is the number of registered changes of the parameter in Increment-Change Space during the time interval ^ ώfe , and τ > ° is the constant time interval between any two adjacent parameter values successively registered in Increment-Change Space. The transformation described above is termed by the inventor "parameter- normalization" since the changes in the market parameter are registered at every change of the parameter by increment r. It is however also possible to effect a transformation from real space to Increment-Change Space by considering real time as the parameter and the real parameter as successive increases or decreases in registered changes. This transformation is termed by the inventor "time normalization" and is governed by the system of equations and inequalities set out below. The registration of a new parameter value in time-normalized Increment- Change Space is determined by the equation: where t?Mϊ is the current time value in real space at the moment of registration of the parameter in time-normalized Increment-Change Space (any interruptions in the de facto existence of the parameter in real space, e.g. non- working days, are left out of account if they impede the regular reflection of the real-time data in Increment-Change Space); recW is the initial moment of time in real space (corresponds to N = 0 ); N = 0, 1, 2, 3... is the serial number of the parameter change registered in time-normalized Increment-Change Space; r > ° is the time interval between any two adjacent parameter values successively registered in time-normalized Increment-Change Space; and f is a value which meets the condition , chosen in such a way as to permit splitting into a beam or effecting a "phase shift". Every change in the value of the parameter in time-normalized Increment- Change Space is determined in accordance with the formula: rM real (v) ΔR duka ' \∞ where ^ is the change in the parameter when its new value is registered in Increment-Change Space relative to the preceding value in time-normalized Increment-Change Space (if ΔR reo/ = 0 , then M& equals its preceding value, or else it is determined by some other reasonable method chosen at will); r > 0 is the absolute value of the difference between any two adjacent parameter values successively registered in time-normalized Increment-Change Space; and ^^ is the parameter change in real space during the time that has elapsed since the preceding registration. Finally, the scale of permitted time values in time-normalized Increment-Change Space appears as follows: where: t& * s - is the scale of the permitted time values in time-normalized Increment-Change Space, and dlΛoi0) is the time value set at N = 0, which makes it possible (if desired) to combine the starting point of the trajectory with the zero point of the time count (or any other point fixed as the starting one) in time-normalized Increment-Change Space. The pattem of change of any market parameter in Increment-Change Space appears as a broken line in which the segments have the same angle of inclination with respect to the time axis. A physical analogue with which we are familiar is the trajectory of the motion of a light ray along one axis, subject to the condition that "U-turns" are possible only at "specially marked" points on this axis, i.e. points located at identical intervals equal to the value of the increment of measurement. This analogy is somewhat idealized but extremely useful for our further investigations. Following the principle of universality, we can extend the physical laws of motion of a light ray to the change of market parameters. Since the physical analogue we have determined can exist in a stable manner in the conditions described above only as a wave with a length equal to double the measurement increment r, in Increment-Change Space we shall interpret the motion of any parameter as a wave process with the same wavelength. By doing so we establish the basis for applying techniques and methods of wave mechanics when analysing the process of change of parameters in Increment- Change Space, and this represents the third law of evolution. Third law of evolution: The process of change may be described as a material wave-particle motion in which the wavelength is equal to double the measurement increment r and the rest mass is equal to zero. Thus the motion of a market parameter in Increment-Change Space is physically similar to the motion of light, but it is not light. It is important to understand that the properties of a trajectory describing changes of a market parameter in Increment-Change Space are related to the value of the measurement increment r, which can take any value in the range from zero to infinity. In other words, waves describing the process of change of parameters in Increment-Change Space (hereinafter "parameter change wave", or simply "wave") theoretically have an unlimited spectrum of wavelengths, whereby for any wavelength a shorter one can be found in which the representation of the process of change will be more precise and detailed. Thus, the length of a wave is not an absolute characteristic - it is always relative, as is the pattern of the process of change at that wavelength. The essential point here, however, is that development of the process of change at any possible wavelength in the infinitely wide range must be governed by universal laws and must be independent. This independence means that development processes at different wavelengths do not influence each other. Nevertheless the pattern of changes at shorter wavelengths always supplements and determines the corresponding pattern of long waves. I. 2) Application of Physical Laws Considering the above, in the following section the laws of Physics shall be applied by analogy to the process of change of a market parameter plotted in Increment-Change Space. The wavelength λ and frequency v of a parameter change wave can be expressed as follows: (1) i (2) v = 2τ where τ = r/ c t where c is the maximum possible velocity of change in Increment-Change Space, τ thus represents the time in Increment-Change Space that it takes to register each change of the parameter by the increment value r. In the following development, we shall apply, by analogy, the laws of Quantum Mechanics Theory, which describe the behaviour of wave-particles, to the process of change of market parameters in Increment-Change Space. The momentum P of a parameter change wave at a selected wavelength equals h h (3) λ 2r where h is an analogue of the Planck constant. Considering further that P = M (4) where M and V are, respectively, the mass and the velocity of the parameter change particle. We may thus express the law of conservation of momentum as follows: h (5) P = — = MV = const 2r Applying Einstein's law, the following is true for the effective mass of the particle: £ (6) c A where E represents the energy of the parameter change particle. Moreover, according to Planck, energy can take only the quantum values S = fήv (7) where n = 1, 2, 3 ..., and where the parameter change wave frequency is connected with the wave length of the parameter change wave by the known ratio λv = c (8) Taking expressions (5), (6) and (7) into consideration we arrive at k nkvV s (9) — = =*- = const x ' 2r c 2 where H is the velocity of the parameter change particle corresponding to the quantum number n. The rule of the quantization of the velocity of the parameter change particle follows there from. V n = - (10) n , where n = 1, 2, 3 ... We should therefore meet the effect of quantization of the velocity of the parameter change particle, and therefore of the trajectory describing the evolution of a market parameter in Increment-Change Space. This shall be verified further on when concrete examples are discussed. One of the consequences of accepting the quantum hypothesis is the applicability of the Heisenberg uncertainty principle: ARAP x h (11) where A ? stands for the uncertainty of the coordinate of the parameter change particle and therefore of the trajectory describing the motion of the particle (localization of the parameter) and Λ-° the uncertainty of the parameter change particle momentum. Let us consider an experiment designed to determine . Given that in practice we can measure only the trajectory velocity, let us concentrate on the determination of V and A .it is understood that AP js functionally related to them. As a consequence of p = MY , we may express as follows: AP = ^M 2 AV 2 + AM 2 V 2 ( 12 ) The mass of the parameter change particle is expressed through V as a consequence of equation (5) u- 2rV (13) From which it follows that: \dM kAV (14) Δ = AV = dV 2rV* Let us insert equations (13) and (14) in equation (12) Applying the law of quantization of velocities, we can write: By combining expressions (16), (15) and (10) we derive From which, by inserting the result in equation (11), we obtain the uncertainty relation for the parameter change particle in the following form: R - -&2L (18) It remains to determine ra . As we know that n is a discretely changing quantum number, it is determined in advance that Aw w j|| be close to unity. We cannot, however, state with absolute certainty that Δ« = l . Accordingly, on the understanding that ra j s a number of the order of unity, we introduce the numerical coefficient q ^/Δn _ yyj tn tn j s coe ffj c j en t ι the uncertainty relation can be stated in more convenient form: Λ D * qrn = - — (I 9 ) ' 2 This formulation also automatically eliminates the question of the coefficient which, generally speaking, may be put in front of h in expression (11). By tacit assumption we took it to be equal to unity. Even if it is not equal to unity, however, the coefficient q introduced by us successfully "absorbs" this awkwardness and seems to dispose of it completely. Furthermore, by using the parameter q we avoid yet another awkwardness. We are not entitled to claim that the formula for the momentum localization (expression 12) is exclusive. For example, that formula can either be written in linear form ΔP = MAV + AM V 0 r expressed in other ways. But the difference between these approaches entails the emergence of a numerical factor of the order of 1. Clearly this factor can also be absorbed by q. The precise definition of q in each particular case is one of the major practical problems of the theory of evolution. Later we shall explore this question in more detail, but for the time being we shall use the value q = ^ . It should also be noted that here and further on n must be taken to mean, not a discrete series of integer values, but a continuously changing average value. In fact, by assuming a non-zero rø t we are obliged to acknowledge the existence of the scatter of n, i.e. a certain quantum number distribution. Even though it is an integer value distribution, the mean value of n is changing continuously. The expression (19) thus establishes a direct connection between the wavelength at which the trajectory is observed, the quantum number of the trajectory and the vertical distance ΔR between the borders of the band within which the trajectory moves. Since we are conducting the trajectory analysis in Increment-Change Space we must pay attention to the error in the determination of ΔΛ . The measurement unit here is r , i.e. half the length of the parameter change wave. Let us assume that we determine the length of a section of a parameter change trajectory between two points as ΔS = R, -R s Then the error of the result will be related to the errors of the measurements of the coordinates δR { = δR 2 = r in the following way: SAR = (SRι + (SR 3 = r-f2 ( 20 ) This enables us to estimate the relative error of the measurements: SAR 1 (21) Hence it can be concluded that in the range of low n, where the error is of the order of 100%, it is unrealistic to expect quantitative correspondence from the measurements. Conversely, we may expect the analysis of concrete examples to yield sound, stable results in the high n range, where the error diminishes as 1 / n, as we will see when we verify the various results of this theory in the examples section further on. The uncertainty relation has an important property which can make it easier to conduct its experimental verification. Since the geometrical representation of the parameter localization error AR is represented by the distance between the high and low peak values of the parameter change trajectory measured as the distance in the direction of the parameter axis (i.e. Y-axis), between upper and lower lines R10a, R10b, S10A, S10B traced through extreme points as illustrated in Fig. 10, then at » » 1 , when the measurement error of AΛ is small the following must be true: Α , r * Δ& »„,r « cons ,tant , ( λ 22) ' Where ΔR π , r and ΔR n ', r ' are the magnitudes of the parameter localization for different values r and r' of the measurement increment respectively. In other words, the value of ΔR is substantially independent of the choice of the measurement increment rfor a large number of measured changes. Compliance with this requirement is more easily verified by the rule of transformation of the quantum number n of the trajectory points when passing from one Increment-Change Space in which the value of the measurement increment is r, to another in which the value of the measurement increment is r' different from r, whereby m w r' B'M i v ~ constant (23) This rule is confirmed by experimental verification as we shall see further on. In concluding this section it is useful to add the following. A correlation interconnecting the magnitudes of the measurement increment r and the quantum number π on the scale of the real space parameter/time chart can be derived from expression (23) by means of a simple transformation. To this end it is necessary to turn to the substitution » = (tfτ)f(Rfr) an d «'= (t /r)' /(R/r') . Here τ and τ' stand for the average intervals in real time taken up by single changes of the parameter r or r" as the case may be. After the substitution we cancel out t and R, which do not depend on the choice of the measurement increment because they are coordinates in real space, and we obtain the following invariant relation: r 2 1 'τ « (r'Ϋ I r'« inv » const. II. EXPERIMENTAL VERIFICATION OF THE THEORY II. 1) Quantum Effect The properties of a parameter change trajectory will now be defined and described. Consider a chart as shown in Fig. 1 representing the changes of a market parameter in real time. In this particular example, the market parameter is the quoted exchange rate of the Euro to the US dollar (i.e. the ratio of Euros per USD) from April 20 th 1998 to January 28 th 2000, on a daily bar basis, the data being provided by Aspen Research Group. Fig. 2 shows the section P1 a-P1b (from October 8 th 1998 to January 28 th 2000) of the chart of Fig. 1 in Increment-Change Space, i.e. the real parameter information has been transformed by applying the expressions (i) to (iii) for parameter normalization. In so doing, the absolute real parameter scale along the vertical axis in Fig. 1 has been transformed into the relative parameter scale (expressed as a number of measurement increments r) along the vertical axis in Fig. 2. Moreover, the real time (in days) along the horizontal axis in Fig. 1 has been transformed into Evolution Time along the horizontal axis in Fig. 2 (as described in the above section "First Law of Evolution") and expressed as a number of registered changes N as defined in expression (iii). In this example of transformation into Increment-Change Space, r was given the value 0.005. According to expression (iii), the number of registered changes N is expressed as a number of τ units. It is to be noted that the values along the vertical axis representing the real space market parameter (e.g. price, exchange rate, etc..) shown in Fig. 1 corresponds essentially to the values along the vertical axis representing the relative parameter in Increment-Change Space, as shown in Fig. 2, except that the latter is expressed in number of measurements steps (i.e r units) and the origin is set at zero. The horizontal axes of the charts of Figures 1 and 2 however do not correspond. Looking at the pattern of motion as depicted by the trajectory T2 in Fig. 2, the existence of a quantum effect is not apparent due to the fact that, for the visual observation of quantum properties, simple graphical plotting of the trajectory of one parameter change particle is not sufficient. It will be shown below that the rule of quantization of the velocity (10) of the parameter change trajectory (V n = c/n, where the quantum number ? = 1 , 2, 3 ...) is met when examining the changes of a set of parameters (hereinafter called a "beam") in Increment- Change Space, that is to say the manifestation of the quantization or quantum effect has a statistical character. Independently of discussing exclusively the statistics of a coherent beam, such quantization must be typical even for the statistical drift in space of one parameter change particle if the drift is taking place at a stable average velocity. Fig. 3 shows, at an enlarged scale, the section as delineated by means of dashed lines F3 in Fig. 2. As can be seen in Fig. 3, the average velocity V n of the trajectory between points P3a and P3b is defined by the slope of the line L3 which is equal to R n /t n . The maximum velocity c is equal to rlτ , thus, λ may be determined at will by the value of r chosen. If τ is given the same magnitude as r, such that c = 1 , then the quantum value n of the line L3 is equal to 1/V n according to expression (10), in other words: n = t n /R π . In this particular example, t n = 16τ and R n = 8r, such that n = 2 and V n = 0,5. Fig. 4 shows the image obtained as a result of the superposition of 5 different trajectories in Increment-Change Space. It includes trajectories which appear to be unrelated with one another : the trajectory T4a represents, by means of open circles, the ratio EUR/USD, with r = 0.005, i.e. the first 100 points of Fig. 2 starting from initial point P1a the date of which is 08/10/1998 ; the trajectory T4b represents, by means of stars, the Dow Jones Industrial Average or DJIA index, with r = 50, from October till November 1999 ; the trajectory T4c represents, by means of open triangles, the DJIA index, with r = 300, from the moment of DJIA birth until 1998 ; the trajectory T4d represents, by means of "*", the GBP/USD ratio, with r = 0.0009, from 21st of May till 27th of May 2001 ; the trajectory T4e represents, by means of open crosses, the USD/CHF ratio, with r = 0.0025, from 17th May till 31st May 2001. The starting points of each of these trajectories are aligned (for example, set to zero) in Increment-Change Space, where the relative parameter (expressed as the number of measurement increments r) along the vertical axis is equal to the half of the wavelength, as expressed by equation (1), and the evolution time measurement unit is the value τ, redefined as * " = ri c _ as expressed in section 1.2). A slope (i.e. velocity), set at will, was chosen as "c" for all the graphs thus aligned. Some of the trajectories pointed downwards in real space ; accordingly, their direction was reversed before alignment. Fig. 5 shows beam-average curve B5 determined by averaging, at each point along the Evolution Time axis, the value of the Relative Parameter (i.e. the average of the vertical coordinates) of the five trajectories T4a to T4e shown in Fig. 4. We shall call "average" the value defined substantially or approximately by calculating an arithmetical mean. For example, it could be a weighted mean (where the weighting coefficients can be user-defined), or any other averaged value which application does not distort the idea of the method. It is to be noted that the beam-average can be obtained for any type of trajectories in Increment-Change Space by calculating the average of parameter for each Evolution Time. The indication of velocity quantization in accordance with expression (10) may be observed in the beam-average curve B of Fig. 5. One can see that the beam-average curve B seems to have sections P5a-P5b, P5c- P5d, P5e-P5f and P5g-P5h that stick to quantum lines n = 1 , 2, 3, 4 and 5, respectively. The aforegoing indicates the existence of the effect of quantization of velocities in a randomly composed (i.e. incoherent) beam of trajectories. Although these trajectories are completely unrelated and refer to different market parameters and historical periods, by operating in dimensionless Increment-Change Space, we have been able to combine in one beam what seemed to be incompatible. We remind you again that this beam includes the DJIA index trajectory which has been in existence almost a century, the EUR/USD currency correlation over a period of about a year and a half, and a brief spurt, lasting only a few days, of the British pound in relation to the dollar. We draw particular attention to this factor just to emphasize the importance and universality of the results obtained. Since recognition of the quantum effect is a cornerstone of the theory developed herein, let us cite here the results of another experiment. Let us verify the existence of the quantum effect in a coherent beam of trajectories, as opposed to the quantum effect in a randomly composed beam of trajectories T4a to T4e as shown in Fig. 4. The coherent beam can be obtained by splitting one initial trajectory into a beam of two or more coherent trajectories. According to the properties of Increment-Change Space, whereby all points on the real parameter curve that differ from the last registered change by a value less than the measurement increment r will have the same formal coordinate in Increment-Change Space, it is possible to transform one curve in real space into two or more trajectories in Increment-Change Space, i.e. to create a coherent beam of trajectories each with the same wavelength λ as expressed in equation (1) and coinciding points of emission. It is sufficient merely to "shift" the measurement starting point on the parameter axis of the real curve by a value less than the measurement increment r. An example of the aforementioned beam transformation will now be described with reference to Figures 6A and 6B. A coherent beam B6B in Fig.δB consisting of two trajectories T6Ba and T6Bb is obtained by transforming one real curve C6A as shown in Fig. 6A, where r was given the value 0,01, where the first trajectory T6Ba is phase shifted by r/2 with respect to the second trajectory T6Bb. For example, the round dots 1-16 in Fig. 6A are used to plot the first trajectory T6Ba in Fig. 6B and the triangular points 1'-12' in Fig. 6A are used to plot the second trajectory T6Bb in Fig. 6B. Fig. 7A shows the beam transformation with a phase shift of r/2, as explained above, of the section P1a - P1b of the real curve shown in Fig. 1. Quantum lines n=1 to n=11 have been superimposed on the two trajectories T7Aa and T7Ab. It is interesting to observe that many of the market rebounds occur when the trajectories touch or are very close to quantum lines, for example at points P7Aa, P7Ab and P7Ac, which would tend to confirm the existence of a quantum effect. Fig. 7B shows a beam-average curve B7B which is the "centre of mass" (i.e. the average relative parameter) of the two trajectories T7Aa and T7Ab of Fig. 7A. It is clear that the beam-average curve can be obtained for any number of trajectories. The meaning of "beam-average curve", "centre of mass of trajectories" and "trajectory of centre of mass" is absolutely equivalent. As it was mentioned above the quantum effect has a statistical character. But even from the averaging of two trajectories it can be seen that the quantum directions roughly followed by the beam-average curve B7B are the quantum lines n=5 and n=8. Fig. 7C shows a beam-average curve B7C for 200 trajectories obtained by the phase shift r/200 for the same section P1a-P1b of the real curve shown in Fig.l Thus, Fig.7C differs from Fig.7B only by the number of trajectories used and the manner of presentation. Fig. 7B is drawn mainly to explain the principle of construction of a beam-average curve while Fig. 7C is a real example of the graph that will be used in market analysis. This Fig. 7C is obtained by using the software which main components are described below. The quantum effect can be seen much more clearly in Fig 7C than in Fig. 5. This difference can be explained by two factors: much higher number of trajectories (two hundred used in Fig. 7C in comparison to only five used in Fig. 5), and independent character of the trends (see Fig. 4) used for averaging in Fig. 5. Due to the much smoother character of its fluctuations the curve B7C subsequently follows the quantum line n=1 in the section P7C1-P7C2, line n=3 in the section P7C3- P7C4, line n=6 in the section P7C5-P7C6, line n=5 in the section P7C7-P7C8, briefly follows line n=8 in the section P7C9-P7C10 and, finally, the line n=7 in the section P7C11-P7C12. The Increment-Change Space transformations discussed earlier were based on a fixed measurement increment r of the market parameter (e.g. price, exchange rate, etc) axis (parameter-normalization), but one can also effect a transformation in time-normalized Increment-Change Space as set forth in expressions (iv) - (vi) that may be described as follows: if the market parameter (e.g. stock market closing price) is measured at equal time intervals τ (for example one day), then irrespective of real rise or fall of the market parameter, the corresponding rise or fall in Increment-Change Space is a set at a constant value r. In other words, only the direction of change of the market parameter is reflected. If the change is a rise, the fixed value r is added to the preceding Y coordinate; if it is a fall, the fixed value r is deducted. Of course such a transformation will considerably distort the price axis, but what matters is that motion in such space must obey the same universal laws. In the same way as shown in Fig 9A, 9B, it is possible to verify the existence of the quantum effect in a coherent beam of trajectories as in the time-normalized Increment-Change Space. It is possible to transform a curve in real space into two or more trajectories in time-normalized Increment-Change Space, i.e. to create a coherent beam of trajectories with the same wavelength λ as expressed in equation (1) and coinciding points of emission. It is sufficient merely to "shift" the starting point on the time axis of the real curve by a value less than the measurement increment τ. An example of such splitting may be described by referring to Figures 8A and 8B. The coherent beam B8B in Fig. 8B is obtained by transforming the real curve C8A shown in Fig. 8A, where τ is given the value 2 days and the phase shift is τ/2 (one day) into two trajectories T8Ba and T8Bb as shown in Fig. 8B. Points 1-12 in Fig. 8A are used to plot the first trajectory T8Ba in Increment-Change Space, respectively points 1'-12' in Fig. 8A are used to plot the second trajectory T8Bb in Increment-Change Space as shown in Fig. 8B. Fig. 9A shows the time-normalized transformation as explained above, as applied to the section P1a - P1b of the real curve shown in Fig. 1. The second trajectory T9Ab is phase-shifted by τ/2 with respect to the first trajectory T9Aa. Fig. 9B shows a beam-average curve B9b which is the "centre of mass" (i.e. the average relative parameter) of the two trajectories T9Aa, T9Ab of Fig. 9A. It can be clearly seen in this example that the beam-average curve BΘBfollows closely, along sections thereof, respective quantum lines n=1 to n=4. II. 2) Uncertainty of the Increment-Change Space Trajectory Coordinate: Parameter Localisation ΔR Fig. 10 shows a trajectory T10 corresponding to the section P1a-P1b of the chart of Fig. 1 after transformation in parameter-normalized Increment-Change Space with a measurement increment of r = 0.02. The experimental parameter localization ΔRexp for the trajectory section from point P10-1 to point P10-13 is measured as the vertical distance between the support and resistance lines S10a and R10a, respectively. The support and resistance lines S10a and R10a are parallel to the average trajectory line T10a and pass through the outermost points P10-5 and P10-7, respectively. In a similar manner, the experimental parameter localization ΔRexp for the whole trajectory from point P10-1 to point P10-36 is measured as the vertical distance between the support and resistance lines S10b and R10b, respectively. The support and resistance lines S10b and R10b are parallel to the average trajectory line T10b. The average trajectory lines T10a and T10b are linear approximations of the trajectory sections P10-1 to P10-13 and P10-1 to P10-36 respectively, obtained for example by using the least square method. The equation of the average trajectory line T10a is Y = -0.55 X + 0.15 and the equation of the average trajectory line T10b is Y = -0.28 X - 1.88. The slops of the average trajectory lines T10a and T10b are thus equal to -0.55 and -0.28, respectively. As discussed above with reference to Fig. 3, where the maximum velocity c is chosen as equal to 1 , the slope of a line in Increment-Change Space is equal to 1/n. We can therefore conclude that, for example, 1/n is equal to 0.55 for the average trajectory line T10a and to 0.28 for the average trajectory line T10b. Fig. 11 shows the ratio ΔR / ΔRexp of the trajectory shown in Fig. 10 for respective trajectory sections defined from the initial point to each current point. To avoid a hundred percent uncertainty which arises according to (21) for n=1 , the first five current points are not taken into account. The parameter localization error ΔR is calculated according to expression (19) where r is the known measurement increment, q is given the value of the square root of 2, and the quantum number n is the inverse value of the slope of the average trajectory line of the corresponding section of trajectory of Fig. 10. For example, to determine n for point P11-13 in Fig.11 the trajectory section from origin to point P10-13 in Fig. 10 is taken and the average trajectory line T10a is obtained as described above. The slope of this line gives the value of 1/n. For each measurement point along the Evolution Time axis, ΔRexp is measured as the vertical distance between the support and resistance lines, determined as mentioned above. As may be seen in Fig. 11 , the ratio ΔR /ΔRexp varies around the level of unity, except in the field of low quantum numbers n where these variations are, as expected, greater than at the right-hand portion of the graph, where the value of n increases. Therefore, for the determination of ΔR exp , we excluded the first five points of Fig. 10 for which there is an uncertainty. Due to the fact that ΔR / ΔRexp varies around the level of unity for n » 1 , ΔR / ΔRexp ~ 1 and we can conclude that expression (19) is met. Fig. 12 shows the value of 1/n for points P1b, P1c and P1d of the curve of Fig. 1 after transformation into Increment-Change Space. 1/n is given by the slope of the respective lines extending from the origin of the Increment-Change Space chart to points P1b, P1c and P1d, respectively, for transformations of the section P1a - P1b of Fig. 1 for different values of the measurement increment r. As can be seen from the graph, in the range 1 / n < 0.4 (or n > 2.5), there is a substantially linear relation between 1 / n and r, which confirms the theoretical properties of Increment-Change Space discussed above, in particular the validity of expression (23), whereby r ■ n remains substantially constant independent of r used. As could be expected, in the area 0.4 < 1 / n < 1 (or 1 < n < 2.5), the errors are increasing. Precisely because, according to expressions (20) and (21), any assertion in Increment-Change Space can be correct only with some degree of uncertainty, we used the symbol "«" instead of "=" in expressions (22) and (23). III. DEVELOPMENT OF INFORMATION ANALYSIS TOOLS III. 1) Possible Market Development Directions Let us now consider one of the main practical applications of the theory developed hereinabove. As is well known, forecasting of market trajectories is the principal concern of millions of investors. The information analysis tools described hereafter are to assist investors in improving their forecasts. Fig. 13A shows a model section of a trajectory in Increment-Change Space. Let us suppose that marked rebounds occurred at points 1 and 2 and that we wish to determine the direction in which the trajectory will proceed. Let us also assume that point 2 is the base point through which the support line of a new trajectory will later be drawn - either in the same direction as n but with a higher quantum number (i.e. at lower velocity) n(+), or in the direction opposite thereto n(-). Point 1 will determine the resistance lines R(+), R(-) of the future trajectory, parallel to the corresponding support lines S(+), S(-). Let us see if we can find the quantum numbers (i.e. the velocities or the slopes) for the two possible directions of the future trajectory. From a formal point of view, the problem may be defined as follows. For two different points in Increment-Change Space, we need to determine the quantum numbers of the trends localized by the support and resistance lines passing through those points. According to the terms of the problem, these trends should be physically compatible with the space coordinates of this pair of points. Let us designate the quantum numbers of these trends as n(+) and n(-), where (+) corresponds to the trend pointing in the same general direction as n, while (-) designates the opposite general direction. As seen in Fig. 13A, localization of such trends is determined in the following way : ΔR M(+ = R H -^ W (28.1) ΔS.^ - Λ.+ ^. j (28.2) By the introduction of a coefficient z = ±I , these two equations can be reduced to a general form. ΔR_ W - *Λ W < 29 > Here z = 1 takes into account the same direction as the I → 2 trajectory, while R = \R — R I z = -1 takes account of the opposite direction. Furthermore, s I f - 3 J n and t n = t (2) -t (1) , where (R (1) ,t (1) ) and (&{2)> t (2)) are the coordinates in Increment-Change Space of points 1 and 2, respectively. Given that έ * = R ^ , and bearing in mind expressions (10) and (19), the condition of physical compatibility we have formulated may be expressed as the following compatibility equation: q s m 2 = R n [n ∑ - zn] (30) Here #* means that in a general case q may depend on the direction. Subsequently, to simplify the designation of #* we propose to use the same value of q for both directions. At the moment, for the sake of simplicity we accept q∑ = q = ^ 2 . It should be noted, however, that this may not always be a sound assumption - a problem that will be treated in detail further on. In view of the foregoing, the solution of the physical compatibility equation may be expressed as follows: ,_ (31) The result obtained from this calculation has important practical implications. First of all, there cannot be more than three compatible solutions. For ease of distinguishing between these three possible Increment-Change Space trends, the inventor has assigned a certain letter to each. First, at z= -7 (direction opposite to I → 2 ) a solution always exists and it is always the only one, as the second solution is negative and, by definition, n∑ . Thus, at any value of n and ^ there is a possible future trajectory in the opposite general direction which endeavours to reverse the current trajectory. The quantum number n(-) -n a 0 f sucn a trajectory is determined in the following manner: We shall call this solution "alpha". But if we are considering solution (31) at z = 1, i.e. if we are looking for the quantum number of the trajectory moving in the initial general direction, then several variants present themselves. They are determined for positive values of the expression standing under the root, i.e. if n < — — (33) 4qr then there are two solutions, which we shall call "beta" with a high quantum number, and "gamma" with a lower number, respectively. Λ. : (34) ■ + R nβ = 2qr 4q"r Λ qr A single positive trend solution, which we shall call "abc", exists when the "beta" and "gamma" Increment-Change Space trajectories coincide. It takes place at n = R " / 4ctr and may be expressed as follows. n aic = 2 ,n = — Z» (36) 2qr In the event of the "abc" solution the expression for n& can be simplified. Substitution of the condition in (32) gives the following result. n & = 2n(l +42) = ξϊ- (l + 2) (36'1) 2qr This n a bc solution also has a special physical meaning, which we shall consider later. On the other hand, a positive trend solution cannot exist if 4qr Let us emphasize that for all expressions (28-37) the following occurs: c(t - t {1) ) (38) R * = \ R(2) - R(i) \ a nd n Here are the coordinates in Increment-Change Space of points 1 and 2, respectively. In addition, for any n \ it is assumed that (39) n \ = — > ^ where / is: z, α,β,γ,αbc, e t c In the context of putting into effect the idea of constructing physically compatible trends, it would be useful to indicate some other possible scenarios of calculating their quantum numbers. For instance, it might be useful to consider a situation where - unlike in the case shown in Fig. 13A - the base points 1 and 2 are located at opposite and resistance lines respectively as shown in Fig.13B. By analogy with what we wrote in formula (28.2), let us formulate the compatibility equation: AR -R + t s V s(Σ) (40.1) The difference from (28.2) consists in the minus sign placed before R n . In the light of (40.1) we can also rewrite the general form of the compatibility equation (29) as follows: AR = +/? + f V (40.2) Here any combination of plus and minus corresponds to one of the scenarios of the compatibility problem. After substituting all the necessary variables into (40.1) we obtain the solution in the following form: The solution "with a minus sign" can obviously be discarded at once, given that n is a positive figure. On the other hand, n must (by definition) be greater than unity. Hence all solutions less than unity must be ruled out. Bearing in mind the above, we arrive at the following definitive formulation of the solution for same- direction alpha trend: 2qr y 4πq 2 r7 2 + qr It is very interesting to consider what happens to the alpha-solutions when R„ = 0. This corresponds to a situation where both base points are located on the same horizontal straight line. The substitution of R n = 0 in (40.4) as well as in (32) leads to the disappearance of the addend in front of the root and of the first addend under the root. As for the second addend under the root, since n = clV n = (t τ)l(R n Ir) after the substitution and cancellation of R„ it is, precisely, this addend that determines the solution for symmetrical alpha trends: Now we must look into what it actually means if a solution to the physical compatibility equation is or is not available. According to formal logic, the absence of a solution should be interpreted as the impossibility of drawing two parallel lines through points 1 and 2 of the trajectory of Fig. 13A or Fig. 13B, which could be taken as, respectively, the resistance and support lines R, S of a trajectory in Increment-Change Space. One solution means that such a pair of straight lines can be drawn in only one way. But the availability of two or three solutions means that these lines can be drawn in two or three different ways respectively. It may be stressed once again that the criterion adopted for the possibility of drawing the parallel lines localizing the trajectory through points 1 and 2 in Fig. 13A is the applicability of the Increment-Change Space uncertainty relation according to expression (19). The total number of variants of the Increment-Change Space trajectory limited by lines passing through points 1 and 2 is then at most three and at least one. Of several competing solutions - alpha, beta and gamma - real motion must, in the long run, choose only one and even then merely in order to reject that direction, too, in favour of a new one (or new ones). The motion thus described is an infinite sequence of rectilinear trajectories, constantly passing into one another, which are limited in space by certain bands. Without going too deeply into the causes of the change in the Increment- Change Space trajectory which, in formal language, can be reduced to some impact on the corresponding wave packet or particle, we will concern ourselves here only with those physical states into which a motion occurring prior to an impact can be transformed after that impact. According to this approach the Increment-Change Space motion represents a broken line of a certain thickness (depending on the slop) where disturbing shocks of the market correspond to the kinks between the rectilinear sections, while "inertial" motion is represented by the rectilinear sections, which may also be very short. In a sense, this concept can even be considered as somewhat deterministic. Indeed, if the future stems from the known past, then this is really so. It is also a symmetrical concept, in that our knowledge of the "future" makes it possible to restore the "past". As with any quantum theory, however, its determination goes only as far as the limits of the correlation of uncertainties, beyond which all certainty disappears without a trace. The correspondence between the approach we have described and the experimental data may be illustrated by the following examples. Fig. 14 shows the behaviour of the DJIA index, from October 1999 to January 2000, in Increment-Change Space for r = 50 on which are superimposed support and resistance lines calculated according to expression (31) for each of the selected sections P14a-P14b, P14c-P14d, P14e-P14f, P14f-P14g and P14g-P14h, more particularly "alpha" and "beta" support and resistance lines respectively calculated according expressions (32) and (34). One can see that the solutions to the compatibility equation, which is constituted by two parallel lines creating the resistance and support lines, limit the trajectory development over a certain length. For example, the beta-solution Rab, Sab of the P14a- P14b section limits the trajectory development from point P14a up to point P14d, and the beta-solution Red, Scd of the P14c-P14d section defines the trajectory development starting from point P14C up to point P14e. It is clearly seen that for similar trend sections such as P14a-P14b and P14c-P14d, the corresponding beta-solutions are comparable. It is interesting to note that at points P14g and P14h, the alpha-solution Rfg, Sfg of the previous section P14f- P14g passes into the beta-solution Rgh, Sgh of the next section P14g-P14h. Thus, the general behaviour of the current trajectory section is defined by the previous one. Fig. 15 shows the section P1a-P1 b of Fig. 1 after time-normalization transformation in Increment-Change Space, where the time measurement increment is r/c = 2 days. It is clearly seen that it is the beta-solution R, S that limits the trajectory development. Fig. 16 shows the development of the same section P1a-P1b of Fig.1 after parameter-normalization transformation in Increment-Change Space with the measurement increment r=0.005. It is an example of trajectory development inside the beta S β , R β and gamma S γ , R γ solutions. It can be seen that when the trend overcomes the resistance line R γ of the gamma-solution, at point P16a, its development is restricted by the beta-solution support line Sβ. Figures 14 to 16 confirm the usefulness of the solutions of the physical compatibility equations to determine resistance and support lines of market parameter trajectories in Increment-Change Space. These solutions can thus be used to perform the analysis of evolution of the market parameters. It is to be noted that if a certain straight line is the support or resistance line of the Increment-Change Space trajectory, then a parallel resistance or support line must also exist, due to the Increment-Change Space uncertainty relation (expression 19). The distance between this second border line and the first one is determined by this relation. In other words, when drawing any straight line we must also draw, at the appropriate distance, its parallel travelling companion. Consider for example Fig. 17 which shows the DJIA Increment-Change Space trajectory from the moment of its "birth" till the year 2000, where r = 500. The resistance line R17 is clearly visible at the top. Points used to draw this resistance line are marked by black circles. The support line S17 can be drawn by plotting a line parallel to the resistance line R17 and passing through the point P17a. Moreover, as mentioned above, for each registered change along the Evolution Time axis, the experimental parameter localization ΔR is approximated as the vertical distance between the support and resistance lines, i.e. is determined by measuring the vertical distance separating the support and resistance lines S17 and R17 in Fig. 17, which in this example is approximately equal to 6 r units (in other words 3000 DJIA points). The value n is the inverse of the slope of the average trajectory line (or of the support S17 and resistance R17 lines) of the whole trajectory of Fig. 17. One can see in Fig. 17 that t17b - t17c = 56 - 40 = 16 and R17b - R17c = 23 - 19 = 4, such that n = 16/4 = 4. Considering the equation (19) according to which ΔR « qrn, if we choose q as the square root of 2, the product qrn of this example, as expressed in r units, is equal to l x 4, which is approximately 6 r units. This therefore corresponds to the experimental value of ΔR exp . Thus, we can conclude that the equation (19) expressing the uncertainty relation as ΔR ~ qrn is once again experimentally verified in this example. III. 2) General Market Development Equation Curve Let us analyse more closely the development of the parameter from its historical starting point towards the future. As the measurement error r is a finite value, then in all cases where the value R of the market parameter is less than the measurement increment r (i.e. R < ή, the parameter will simply be equal to zero. The first registered change for the observer will occur at the moment when its value exceeds that of the measurement increment r.. We have already seen an example of such a graph in Fig. 17, which shows the evolution of the industry of the Dow Jones Industrial Average (DJIA) from its birth until the year 2000. Everything that happened before R = r = 500 is, in our case, concentrated in one point, R = 0. The graph therefore represents the complete history of the development of Dow Jones Industrial Average to the year 2000. Fig. 18 shows the DJIA in parameter-normalized Increment-Change Space for the measurement increment r = 300. The trajectory of the curve is slightly more detailed than in Fig. 17, where r = 500. One may observe from this graph how the US economy, in the process of its development, gradually "worked off' the quantum magnitudes of its velocity. When the two graphs of Fig. 17 and Fig. 18 are compared, notwithstanding their different scales (r = 500 for Fig. 17 and r = 300 for Fig. 18), it may be noted that they are approximately the same. Despite the non coincidence in real space-time, approximately equal parameter values measured in the number of units of the measurement increment r correspond to the same number of registered changes in Increment-Change Space, which means that in dimensionless Increment-Change Spaces, these two trajectories coincide to some extent. Thus, on both graphs, the value of the relative parameter R corresponding to the Evolution Time coordinate 56 is R = 23 r (see point P17b in Fig 17, and point P18a in Fig. 18), although in real space, these points are decades apart from each other, and their real DJIA values differ almost by a factor of two. The notion of similarity forms part of the possible consequences of the universality principle. Different-scale graphs of the same trajectory in dimensionless Increment-Change Spaces should roughly coincide. If the number of particles in the beam is increased to infinity, the trajectory of its centre of mass will ultimately approximate a relatively smooth trajectory. Let us define the equation of this trajectory R(t) as the ideal equation of development. Considering the theoretical trajectory of part of a trajectory in Increment- Change Space as shown in Fig. 13A, let the starting point of the trajectory coincide with point 1 , while point 2 is any point of the trajectory R(t). A single line localizing the parallel trajectory can be drawn through point 2 such that this localizing line will coincide with the tangent of the trajectory R(t). It was shown earlier that a single parallel solution with the quantum number n abc can exist only subject to meeting the following condition (see expression (36)). R x = 4q (41) According to the demonstration made with connection to Fig. 3, n = t n /R n (the maximum velocity c, which is chosen at will, being equal to unity), where t n is expressed in τ units and R n is expressed in r units. Expressing n as (t/τ)/(R/r) in equation (41), one obtains the following expression for the equation of the development equation curve in Increment-Change Space: The thick solid line D18 in Fig. 18 is the development equation curve of the trajectory T18 in accordance with (42). The differentiation of the equation of development at any point of the trajectory leads, in its turn, to the ABC-solution according to expression (36). That is to say that at any point of the development equation curve D18, the tangential line is in fact the quantum line corresponding to the quantum number r? ajt , c . The physical significance of the ABC-solution is thus determined. Its trajectory coincides with the line tangential to the ideal equation of development. Since real motion is always "scattered" around the ideal trajectory, in practice one rarely has only one solution of the compatibility equation for the parallel trajectory. Nevertheless, even where two solutions are formally available, it is useful for the analyst to draw an additional n at>c -\\r\e because it is unlikely to be breached. It is steeper than the beta-line but less steep than that of the gamma-solution. In Fig. 19, three Increment-Change Space DJIA trajectories T19a, T19b and T19c with different measurement increment rvalues (r is equal to 300, 400 and 500, respectively) are superimposed on one another in Increment-Change Space. This image is a good illustration of the universality principle. At this stage, we may confirm experimentally that the curve of averaged trajectories really tends towards the development equation curve according to expression (42). The graph in Fig. 20 shows the mean relative parameter R squared of the three trajectories T19a, T19b and T19c represented in Fig. 19 as a function of Evolution Time. By way of example, the R value of point P20 at time coordinate 41 in Fig. 20 is equal to the average value of the three R values of the three points P19a, P19b and P19c in Fig. 19, which is equal to (19 + 21 + 16)/3 = 18,7. The value of R 2 is thus approximately 350, as shown in Fig. 20. By considering the relative parameter R squared (i.e. R 2 ) as a function of evolution time, the development equation curve according to expression (42) becomes a straight line, as shown in Fig. 20. It is clearly seen that the experimental development line L20 exp represented by black squares calculated in the same manner as for point P20 discussed above, fluctuates around the ideal development line L20, showing a good enough agreement between the experimental and ideal development equation curves. It is important to mention that the development equation curve can be obtained for a section of the trajectory starting from some initial point of the trend in real space. For example the graph of Fig. 21 shows the time dependence of the relative parameter squared R 2 for the beam-average curve B9b shown in Fig. 9B obtained for section P1A-P1 B in Fig.l The difference between Fig. 21 and Fig. 20 is that the starting point in Fig. 21 is not the historical starting point of the parameter contrary to Fig. 20. The line D21 is the ideal development equation curve as calculated according to equation (42). Once again, a good enough agreement is observed between the experimental development equation curve D21 exp and the ideal development equation curve D21 IV. PRACTICAL EXAMPLES OF INFORMATION ANALYSIS TOOLS IV. 1) General Principle In the following section, we shall describe, with reference to examples, the method of processing and analysing market parameters, that may be implemented by means of computer software, to aid an analyst, investor or trader (hereinafter "user") in making a buy, hold, sell and many other types of decisions and recommendations. Computer software for practical implementation of the invention ensures iterative processes of the following type: - Request (instruction) by the user - Request handling and information delivery in appropriate graphical or any other form suitable for the user - New request (instruction) by the user on the basis of analysis or received information - Handling of the new request (instruction)... etc, which will end, for example, when the user judges he has enough information to make a buy, hold, sell or other type of decision and recommendation; or when the user achieves the understanding of the market situation that he judges sufficient for his purposes. The user has the possibility to exit from the process at any moment. This iterative process allows the user to accumulate useful information concerning the evolution of a market parameter being analysed, for example to accumulate intersection signals of the trajectory with a support line or a quantum line. Due to the fact that several signals in favour of the same market direction reinforce each other, the risk of human error when taking final decision can be minimized. The success of market forecasting or speculation significantly depends on the way in which the aforementioned technical analysis method is applied. It relies on the capacity of an experimented user to make a judicious choice of analysis parameters, such as the measurement increment rand the coefficient q, and of the analysis tools to be used, such as the support and resistance lines, the development equation curve, the creation of a beam and the quantum lines. The user must then perform a pertinent analysis of the plotted results in a relatively short time since the market is continually changing, and to continue analysis or to take a decision. The information and information analysis tools available to the user and that can be acted upon with the assistance of a data processing system and software, are as follows : - a real market data database - a method of transformation of a real curve to a trajectory in Increment- Change Space - one or more trajectories in an Increment-Change Space Chart - a data smoothing or noise fluctuations filtering method - a method for calculating and/or selecting and/or proposing the q coefficient (in relation with the compatibility equation) - a method for calculating and drawing by superposition on the Increment- Change Space Chart analysis lines such as support and resistance lines, quantum lines, development equation line(s), beams, beam-average curves, the fastest trajectories and variations thereof. The above information and information analysis tools will be discussed hereinafter. IV. 2) Information and Information Analysis Tools IV.2)-a The real market database First of all and before starting the analysis, the user will need to select the real market database on which he wishes to work so that it will be as close as possible to an "ideal" database. The term "ideal database" should be understood as a continuous record of all without exception consequent values of the changing parameter, which is also free of any defects, recording gaps, distortions, etc ... In practice, it is difficult to fulfil this criterion, even if such fulfilment is seen as the ultimate goal. Moreover, with the purpose of reducing the amount of data stored and transmitted over data networks, a simplified (shortened) format is used in practice. Stock market information for quoted share prices, stock market indices, exchange rates etc. are commercially available from various suppliers of such data, via the internet or by direct telecommunication access to the suppliers' database server network. In case of stock market data, a set of periodical characteristic prices is most often chosen as the appropriate format, for example the quotes for open, close, minimum and maximum prices. Also indicated is the standard duration of the interval, its start time or end time, and sometimes the volume of transactions within the interval. The required speed of data transmission and possibility of their storage in a compact format is usually achieved by dividing the real time axis into standard intervals and characterizing such intervals with a finite set of parameters. If the dynamics of the parameter change in real time is represented in such reduced format (and this is the true for the vast majority of cases) it is not an ideal method of representing and displaying data. Gaps between characteristic points (for example, between maximum and minimum prices) define the degree of error attributable to the data which defines the smallest meaningful value for the choice of the measurement increment r. IV.2)-b The transformation step in Increment-Chanαe Space The user can select the measurement increment r himself, seek an automatic recommendation on the optimal measurement increment from the data processing system, or select it while being guided by a recommendation from the system. As has been discussed above, the optimal values of r are greater or equal to the average amplitude of the difference between the maximum and minimum quotes within a standard time period. It is possible to configure the system so that it adds all average amplitudes relating to the selected data with which the user is working, divides the resulting answer by the number of added terms, and communicates the calculated average difference amplitude to the user to help him in optimising the choice of r, in particular to assign a value greater than the average amplitude. Once the measurement increment r is determined, the transformation of the real curve to a trajectory in Increment- Change Space is effected as previously described herein. We shall call this trajectory "main trajectory". It is also possible, as previously described, to transform the real curve into a beam of two or more trajectories and, if desired, to calculate the beam-average curve thereof, which may be superposed on the main trajectory, or analysed separately. There are many ways of presenting the aforesaid transformation in Increment-Change Space, and of processing the main trajectory or the trajectories of a beam to provide useful information for analysing market trends, as will be seen in the examples described below. IV.2)-c Example of processing a beam of trajectories in Increment-Change Space A particularly useful way of analysing the trend of a market parameter is by splitting the main trajectory into a beam of trajectories, and therefrom plotting the centre of the mass thereof to give the beam-average curve, as previously discussed in relation to Fig. 7A, 7B and 7C, and additionally plotting the fastest beam particle trajectory, which is obtained as described below. By way of example, if we refer to the beam consisting of two trajectories T7Aa and T7Ab shown in Fig. 7A, one observes that the end points P7Ae, P7Af of the trajectories have different values along the Evolution Time axis while having the same relative parameter. If we plot a beam consisting of a larger number of trajectories, their end points will have the same coordinate on the relative parameter axis and differing coordinates on the Evolution Time axis. The beam trajectories thus gradually "slide apart". The fastest trajectory is the trajectory (T7Ab in the example of Fig. 7A) that reaches the end coordinate (which will often be the current market parameter value) in the shortest evolution time interval. The slowest trajectory (T7Aa in the example of Fig. 7A) reaches the end coordinate in the longest Evolution Time interval. If the general trend of the beam is downwards, as is the case in Figure 7A, the point P7Ad of the slow trajectory with the same Evolution Time coordinate as the last point P7Af of the fast trajectory. If a beam consists of more than two trajectories, then all other trajectories will also cross this vertical straight line passing through the Evolution Time coordinate of the end point of the fast trajectory above the point P7Af. This property of the end point of the fast trajectory can also be expressed differently : the end point of the fast trajectory is positioned in front of the center of mass of the beam's trajectories. This means that in case of a downward trend, the end point of the fast trajectory should be located below the beam's centre of mass and for an upward trend, the end point of the fast trajectory is usually above the centre of mass of the beam trajectories. It is convenient to apply such property of the fast trajectory to identify the direction of the trend. To facilitate a user's decision making, it is useful to display (on the monitor) the beam-average curve and the fast trajectory of the beam. It is important to mention that the trajectories can exchange their relative positions, the fast trajectory becoming the slow one and vice versa. In case of a large number of trajectories their position in the beam relative to each other is constantly changing. The faster trajectories slow down, while the slower ones accelerate. For this reason the inventor suggests re-defining the fastest trajectory for each registered change in parameter. For the currently identified fast trajectory, we must find the coordinate of its end point, plot it on the graph and repeat this operation for every new change in parameter. The resulting sequence of end points will form a special trajectory, which will be the fastest of all the beam trajectories. At the same time, the fastest trajectory may also be used as a main trajectory for developing support and resistance lines, quantum lines and development equation curves. However, the main property of the proposed trajectory is that it is always "ahead" of the beam's centre of mass and can thus be used to more clearly identify market trend direction changes, for the purposes of market forecasting. IV.2)-d Real data noise fluctuations Filtering out Process Independently of the choice to proceed on with one or more trajectories in Increment-Change Space, it may be useful for the purpose of facilitating analysis to smooth out the peaks of the trajectories. This data noise fluctuations filtering out process could be done with the traditional method of technical analysis known as the "moving average", but this method averages, for example, an N number of subsequent quote values to derive only one average point and therefore shortens the resulting trajectory by Λ/-1 points. Instead of this method and according to the properties of Increment-Change Space, it is recommended to use a smoothing method which is the moving average method, whereby the averaging period is equal to two points. It is to be noted that the important advantage of smoothing is its application to two points (taken with any user-defined weight coefficients) in Increment-Change Space. At the same time, the smoothing method itself is not so important. In practice, any smoothing procedure (not only the moving-average method) can be used. Consequently, the resulting trajectory is not shortened. Generally a one-off averaging does not result in the desired elimination of "roughness". It is suggested to repeat such method of smoothing a number of times by averaging every subsequent result. The repetitions are stopped when the curve becomes sufficiently smooth to permit the analysis of the resulting image. The corresponding number of times smoothing was applied can be considered as optimal (sufficient). By experience of the inventor, it is suggested that the optimal number lies between four and ten. lV.2i-e The q Coefficient Correct definition of the coefficient q is an important practical task, since it influences inter alia the value of the parameter localisation ΔΛ , i.e. the relative parameter distance between the support line and the resistance line. Its value has been earlier defined as being approximately equal to the square root of two. In practice, the choice of the value for q allows certain deviations from this value. First, it is necessary to point out that q is approximately equal to a constant which is close to the indicated value only in the case where the user has available an "ideal" database. We'll suppose this condition is met. Experience of the inventor suggests that in case of sufficiently large values of the measurement increment r, for example, when r is considerably larger than the average amplitude that characterizes the degree of error of the curve in real space (the case of an ideal database), better results are achieved by using any value of q between the square root of two and two, and sometimes slightly greater. The choice of the concrete value of q from the optimal range depends on the trading tactics preferred by the user. For example, the solutions for the physical compatibility problem lead to the decrease of the quantum number, and thus an increase in velocity, with the rise of q. Therefore, by choosing the value of q closer to the upper limit of the optimal range (q=2), the user will be looking at a more "aggressive" picture - the support and resistance lines will be steeper. This means that with large q, the user will receive an earlier signal to change his trading position. Thus, the problem of choosing a precise value of q becomes to some extent the issue of trading tactics. There are two more factors that need to be taken into account while assigning a value for q. The greater the value of q, the lower the probability of having beta- and gamma-solutions (see expression (34) and (35) for tracing support and resistance lines. In the proximity of q=2, such solutions are rarely available, facilitating significantly the interpretation of support and resistance lines being drawn on the graph because the user obtains only one alpha-solution. This makes the information on the Increment-Change Space simpler and less ambiguous for the user, which facilitates the process of making a trading decision. Secondly, when the maximum value is taken for q, the equation curve becomes the external envelope of all trajectories, such that the parameter trajectory which is touching the development equation curve or coming in its proximity provides a strong trading decision signal. Due to the fact the ideal conditions essentially concerning the original database are not always achievable, it is useful to put forward a practical method for deriving the value of the q coefficient under conditions that are not ideal. Let us look at the interpretation of the q coefficient in the general case. This value has been introduced as a number coefficient while deriving the uncertainty relation (19). The uncertainty relation is used to define parameter localization in Increment-Change Space, which equals the vertical distance between the support and resistance lines of the trajectory. If the lines pass through the outermost points of the trajectory, this corresponds to the maximum value of q. In turn, such interpretation of q means that the development equation curve becomes the outermost envelope of the trajectory in Increment- Change Space. From this, it follows that experimentally, we can derive the maximum estimation for the value of q from the equation of the development equation curve, under the condition that the development equation curve is drawn from the initial point of the trajectory through its outermost point. Accordingly, the following method for deriving q may be considered as the easiest one. The user chooses a pair of points on the graph such that one of them is the point of the start of the trend, and the other - an point of the trajectory. Then, for example using the mouse cursor, the user inserts into the computer the coordinates of these points, after which the value of q is calculated employing the expression (41) as q=Rn/4rn, where R n signifies the difference between the coordinates of the selected points on the parameter axis, r is the measurement increment and n is the quantum number defined by equation (38). After defining the value of q for several points, the resulting solutions may be compared to choose the maximum one. The proposed method can be automated. To this end, the section of the trajectory in Increment-Change Space is scanned. A point on the graph is identified, which is the starting point of the data (for example the origin of the graph). Subsequently this point is considered in pair with every remaining point that belongs to the trajectory. For each such pair, the q coefficient is calculated as described above. All resulting solutions are compared and the one with the maximum value is chosen. Then, the next point is fixed and then paired with all remaining points. For each pair we define the q coefficient. These values are then compared to chose the one with the highest value, and then compared with the maximum of the preceding cycle, after which the absolute maximum for both cycles is chosen. This iteration may be continued until all possible combinations of points have been made and the maximum value of the q coefficient has been selected. The discussed examples of methods for defining the coefficient q are based on the principle that any pair of identifiable points in one-dimensional space unambiguously defines the development equation curve, starting from the first point and passing through the second one. And, as we know, the value of the q coefficient enters the equation of development. Let us consider another example. Using the mouse cursor, the user fixes the point of the start of the trend and the position of the second point through which the development equation curve is automatically drawn. The coefficient q corresponding to such curve is depicted next to the curve. By manipulating the mouse, the user can achieve the required position of the development equation curve (for example such that it passes through the outermost point of the trajectory), and then fix the corresponding value of q. To complete the series of examples of defining the maximum value of the q coefficient in practice, we have to consider one other interesting method. Let us refer once again to the equation of development (41). The expression includes the quantum number n, that corresponds to the line connecting the two points selected from the graph. If n=1, we have q= R n /4r. From this, it follows that to calculate the maximum value of q, all that is needed is to find the longest rectilinear segment on the graph depicting the changing parameter in Increment-Change Space and divide its vertical projection by four. Under rectilinear segment, we mean a rectilinear part of the trajectory without any "turns", i.e. a segment of the trajectory exactly from one turn to the next turn. Thus, we have demonstrated several different examples of practically defining the maximum value of the q coefficient. Let us repeat again, that the convenience of choosing the maximum value is due to three factors. Firstly, the support and resistance lines plotted according to the highest value of q will also be characterized by the highest velocity, so that they will produce the earliest signal of the change in the trajectory's general direction after being intersected by the trajectory. Secondly, the compatibility equation is left only with the family of alpha-solutions which significantly facilitates the process of making a trading decision. Thirdly, when the maximum value is chosen for q, the development equation line becomes the external envelope of any trajectory. This implies that if the trajectory crosses the development equation curve, a strong trading decision signal is given. To determine an average value of q, it is possible to approximate the trajectory with the average development equation curve passing through the "middle" of the points of the trajectory. The term "middle" allows for multiple interpretations. There is a plentitude of standard methods for minimizing the approximation error but the standard least square method is recommended. IV.2)-f Information Analysis Lines The system is organized so that, just after the definition of the q coefficient, the user can enter the coordinates of two points which, in the user's opinion, belong to the support and resistance lines. After receiving these coordinates, the system automatically determines the angle of inclination of the line joining these two points, which provides the quantum number n used to calculate and plot the support and resistance lines. As soon as the trajectory exits the corridor defined by the support and resistance lines, the crossing of which can be interpreted as a signal of a trend reversal and as a possibility to change the trading position, the user can enter into the system a new pair of points to plot new support and resistance lines. Nevertheless, the signal of a trend reversal obtained as a consequence of the fact that the parameter change trajectory exits the corridor defined by the plotted support and resistance lines, as just mentioned, is not always sufficient information to take a reasonable decision. The support and resistance lines constitute the main analysis lines, but to reduce the risk of error, the user should seek additional confirmation signals, in other words, the user should consider other analysis lines, since several signals of the same trend reinforce each other. The user can collect complementary information by superimposing complementary analysis lines, for example quantum lines, development equation curves, beam-average curves, fast trajectories, on the main analysis lines. The system is configured in such a way as to allow the user to enter the coordinate of the point from which quantum lines are to be drawn. If the user detects a rebound of the trajectory from a quantum line, according to the conclusions drawn from the theory, it can be a signal that the market parameter may change direction, i.e. a signal of a trend reversal. It is to be noted that the number of the quantum lines can be set as default by the system or can be requested by the user. The development equation curve, is of a great importance. As above mentioned, when the q parameter is chosen so that it is equal to a maximum value, the development equation curve becomes the external envelope of any trajectory and this implies for example that the trajectory should not cross the development equation curve. Therefore, the user can anticipate, for example, that the market parameter is likely to make a downward correction after an upward movement makes the trajectory reach the development equation curve. The data processing system and software is developed in such a way that the user may enter the coordinate of the point from which the development equation curve is to be drawn. It is to be recalled that, optionally, the user can choose to draw the fastest beam trajectory and the beam-average curve and also carry out the smoothing of any trajectory. IV. 3) Practical Examples In order to further illustrate how the above-described information analysis tools could be used in practice by a user (an analyst, trader or investor), two further practical examples will now be discussed with reference to Figures 22 to 25. Figures 22, 23 and 25 represent a computer screen view of charts in Increment- Change Space, while Fig. 24 shows real market data. On those figures the horizontal axis is always Evolution Time, the vertical axis on the right is the relative parameter in Increment-Change Space, while the vertical coordinate on the left is a real market parameter. Fig. 22 is a chart in Increment-Change Space of the Euro/USD rate shown in Fig. 1 for the period April 20, 1998 to January 28, 2000 after transformation with a measurement increment of r = 0,0206, further splitting into a beam, and subsequently calculating and plotting the fastest beam trajectory F22 and the beam-average curve B22. As previously discussed, in the case of a downward trend, the fastest trajectory is located below the beam-average curve, and vice- versa, for an upward trend. While applying such property of the fastest trajectory to identify the direction of the trend the user can simultaneously employ other tools such as support and resistance lines of the trend, the development equation curve, etc. To this end, the user must decide upon the value of the coefficient q that will be used for the calculation of the distance between the support line and the resistance line. The value of q that ensures the simplest interpretation of graphical information is q ma x - the maximum of all values of q corresponding to a specific range of analyzed data as previously described. It is important to keep in mind that the support and resistance lines plotted according to this value of q maχ will be characterized by a high velocity, so that they will produce an early signal of the change in the trend direction after being intersected by the trajectory in the Increment-Change Space. Moreover, the choice of the maximum value q maχ results in that the compatibility equation is left only with the family of alpha- solutions, which facilitates the process of making a trading decision, and in that the development equation curve becomes the external envelope of any trend trajectory. This implies that the parameter change trajectory should not cross the development equation curve. The system is organized so that, just after the definition of the coefficient q as guided by the system (in both Fig. 22 and 23, q max = 1.75), the user can enter the coordinates of the two points that, in the user's opinion, could belong to support and resistance lines. For example the user chooses points 1 and 2 as such points in Fig. 22. After receiving these coordinates, the data processing system automatically defines the slope of the support and resistance lines S22a, R22a and subsequently plots them. It is to be noted that, although the downward trend has not yet manifested itself in a visual manner in the vicinity of point 2, application of the method developed by the inventor allows the user to already foresee its direction and width by means of support and resistance lines S22a, R22a. After point 3 one may observe that the fastest trajectory goes upward but not enough to exit the corridor formed by lines S22a, R22a. Once again the general downward trend in Fig. 22 can be confirmed by plotting downward-sloping trend lines from points 1 and 2. Just after point 3, there are a number of intersections I22 of the fastest beam trajectory F22 and the beam- average curve B22. However all those intersections lie above the support line S22b of the upward-sloping trend, which is drawn through points 2 and 3. Therefore, if the user closed the position bargaining on the downward trend ("short position") at the first intersection point within the I22 interval, he does not react to subsequent intersections. Only at the moment where the fast trajectory intersects the beam-average trajectory in the last point of the I22 section and subsequently intersects the support line drawn from point 3 does the user reopen his short position. Another method to improve analysis and avoid overreacting at each of these intersections I22, is to apply a filter of trajectory smoothing. As previously stated, the optimal number of repetitions of the smoothing process to obtain curves sufficiently smooth has been proposed as lying between four and ten (although this does not exclude the use of any other numbers). The fastest beam trajectory F23 and beam-average curve B23 shown in Fig. 23 represent the fastest beam trajectory F22 and beam-average curve B22 respectively of Fig. 22 after ten consecutive smoothing iterations. One may observe that the curves of the fastest trajectory F23 and the beam-average curve have been considerably smoothed. The intersection at point 123 of the two curves F23, B23 after smoothing provides a clearer signal for considering a possible change of trading position. As previously discussed, several signals of the same trend reinforce each other. To identify in a more precise manner the general trend, it is helpful to plot support and resistance lines, as well as quantum lines and a development equation curve. Fig. 23 shows the support lines S23a and resistance lines R23a, drawn through points 1 and 2 respectively (exactly as S22 and R22 in Fig. 22). The user can also decide to plot quantum lines n=1 to n=4 from point 2 by entering into the data processing system the coordinates of this point. The quantum lines are lines along which the trajectory in Increment-Change Space develops, jumping from time to time from one quantum line to the other. It is to be noted once again that analysis of trajectories with the quantum lines is more effective when smoothing is applied. For example, due to smoothing, it is easy to determine point P23a as being the intersection of the fastest trajectory F23 by the quantum line n=2 right after point 3. The intersection at point P23a is an important signal indicating that the trajectory can "jump" higher towards the next quantum line or reverse the trend direction altogether. To obtain confirmation that the signal received at point P23a does in fact signify the beginning of a upward market correction, the user can also draw the lines of the possible upward trend through points 2 and 3, for example, the support line S23b and the resistance line R23b. Since point P23a lies above the support line S23b the user can conclude that the upward correction has indeed started. On the other hand the intersection of the same support line S23b in the opposite direction in point P23b will signal the end of market correction. Thus, by analysing points 3, P23a and I23a, the user may identify three signals : first of all, point 3 is the point where a trend reversal can be supposed to begin ; secondly, point P23a, which is the intersection of the fastest trajectory by the second quantum line, seems to confirm the supposed trend reversal ; thirdly, point I23a, which is the intersection of the fastest trajectory by the mass centre trajectory, confirms the opposite trend (upward-sloping). The three signals reinforce each other substantially. The user can interpret these three signals as being the moment to react and change his position for a short-term gain speculating on the upward movement. Finally, after the re-intersection of the support line S23b in point P23b and the intersection of the fastest trajectory by the beam-average curve at point 123b located inside the downward-sloping trend, restricted from the top by the resistance line R23a, the user concludes that the quote's fall has resumed. Decision that could be taken on the basis of this analysis was indeed confirmed in practice: after these signals the Euro declined by another 15 percent. To refine even more his analysis, the user can obtain further information from other information analysis tools, such as the development equation curve. Referring to Figures 24 and 25, an example of use of a development equation curve will be described below. Fig. 24 shows a real chart of the US dollar Swiss franc (USD/CHF) exchange rate over the period from April 15 to May 12, 2001, as provided by Reuters, based on ten minute USD/CHF quotes. Carrying out a transformation in Increment-Change Space with a measurement increment r = 0.003 the trajectory T25 displayed on the computer screen is plotted in Fig. 25. As shown in Fig. 25, the zone of stagnation between points 1 and 2 offers the user the possibility to obtain on the chart the support and resistance lines S25a, R25a, which is the unique abc-solution to the compatibility equation by confirming the choice of the coefficient q max calculated by the data processing system for selected points 1 and 2 for example with a mouse curser. Right after point 4 where there is a sharp reversal of the general trend and the trajectory crosses the resistance line R25a, the user receives a clear signal to consider changing his trading position. The user may then also enter into the system the coordinates of points 3 and 4 to plot new support and resistance lines S25b, R25b. At point 5, the quote bounces off the support line S25b.ln accordance with the invented method the user has an indication long before the emergence of point 5, that there is a possibility of market reversal upon the approach of the support line S25b by the trajectory T25 and he can prepare himself in advance to take the necessary actions. After point 5, the user could speculate on an upward movement, but to be cautious, he could request the system to plot the development equation curve D25 with coefficient q = q max from point 5 upwards. Due to the fact that q = q max , the development equation curve D25 becomes the external envelope of any trajectory. Therefore, the user may speculate that approaching point 9, the market should start a correction since at this point, the trajectory T25 has reached the development equation curve. Taking that into account, the user can temporarily exit the position or even open a short term position at least until point 6, where the trajectory bounces off the support line S25b again. To widen our illustration of other tools that can be applied, let us assume that at point 6, the user has requested the transformation of the real curve into a beam with the number of trajectories equal to 100. Let him request the system to carry out the smoothing from the same point, with the number of cycles equal to 10, and plotting of the quantum lines n=1 to r?=3. Let us consider the sequence of events that follows. Having reached the local high at point 7, the fastest trajectory F25 intersects the beam-average curve B25, which signal a downward trend. At this point, a risk-averse user can temporarily close the position, but at point 8 he may speculate in re-opening the long term position, because the fast trajectory F25 has bounced upwards off the second quantum line r/=2. It is important to note that the upward bounce took place above the resistance line R25c of the possible downward trend drawn from points 6 and 7. Right after the bounce, the user receives additional confirmation of the open long term position as the fastest trajectory F25 intersects and outstrips the beam-average curve B25. The user may for example speculate to keep his position until the moment of the intersection of the beam-average curve by the fastest trajectory in the opposite direction. Before ending our series of examples we should touch on one more issue. There exists another simple but useful method of applying the development equation curve. In his research the inventor established the critical value of the q coefficient as being equal to q max /4. The position of the trajectory in relation to the development equation curve corresponding to this value of the coefficient is a conventional criterion of whether there is a directional market trend or whether it has already been dispersed. If the trajectory outstrips this development equation curve or follows alongside it, then there exists a directional trend. If the trajectory intersects this line and falls behind, it means that the trend has been dispersed, i.e. it doesn't exist any more. Of course, in comparison to the ones used previously, the proposed criterion is not a precise tool and can give the user only a conventional signal, which is however simple and useful. That is why the inventor recommends to organize the system in such a way that it offers the user a choice between several values of q which are most interesting from the point of view of practical applicability. It makes sense to include among them at least two values. One of them is equal to q max and the other one is equal to q ma χ/4. IV.4i-a Overall Structure Referring to Fig. 26, a data processing system 1 is connected via communication lines 2, such as the internet or any other type of communication lines, to external data sources 3 for supplying real market data, and one or more user computers or terminals 4 via communication lines 5, that may for example be part of a global computer network, such as the internet or any other type of communication lines. The data processing system 1 comprises for example a central server 6 (or a group of spread servers performing the functions of a central server) with an information storage section 7 and an information processing section 8. The information storage section 7 is used in particular for storing data bases of market data received from the external sources 3, such as for example by commercial market information suppliers, or private (own) data sources. The various market data received and stored in the system 1 may for example be currency quotes, equity prices, and any other market values. Other information may also be received and stored, for example the history of trading operations and user accounts. The information processing section 8 comprises software for processing and displaying market information in real space and Increment- Change Space, comprising various algorithms and processing modules for generating the various information analysis tools of the invention that had been described previously. This software further comprises programs for interactive communication with users, providing the information analysis tools and means of their control and monitoring. The processing of information comprises for example data selection from the database storage section 7. It may be noted that the processing of data may be also run on the user computer by downloading the processing software from the central server, or by software already installed on the user computer. The storage and processing of market data can be organised with different degrees of centralization or decentralization of database storage and information processing systems without parting from the scope of this invention. The software comprises a number of programs, algorithms or calculation modules for performing the transformation of real data into Increment-Change Space and for generating the various information analysis tools according to this invention. By way of example, the structure of some of the software programs or modules for generating information analysis tools according to this invention will now be described with reference to Figures 27 to 37. IV.4)-b Software Programs/Modules IV.4)-b1 Calculation of r def As mentioned above, real market data inherently present a degree of error attributable to the spread of quoted values. The average spread of quoted market values are used to estimate the value of rjdef which determines the smallest useful value of the measurement increment r. Fig. 27 illustrates of a program module to calculate r_def. In step S27a, the data processing system receives from the information storage means 7 real market data as a real data array Rreal[], i.e. as the array containing the maximum and minimum real values (Rreal ma χ[] and Rreal m i n []) corresponding to the each real point in the real market database. In step S27b, the system initialises variables and arrays necessary to carry out the calculation of rjdef. The variable initialisations concern three variables : imax, that is the number of the last point of the real data array; an iterative counter / ' , that is the ordinal number of a real point in the real data array, its starting value being 0 and its final value being equal to i max ; and a variable "Average", that accumulates the average difference between the maximum and the minimum real values, the starting value of which is 0. The array initialisations concern the two above mentioned arrays Rreal ma x[] and Rreal min []. In step S27c, for each value of / ' , i.e. in an iterative manner, the variable "Average" is calculated in a cumulative way. It has to be mentioned that the "Average" is substantially or approximately determined by calculating an arithmetic mean. For example, a weighted mean (where the weight coefficients can be user-defined) or another averaged value can be applied. In step S27d, the counter / is incremented by one. In step S27e, a decisional test is executed to determine if the counter / is less than its maximum value, i.e. imax- If the answer to this test is "yes", i.e. if the counter / has not yet reached its maximum value, then the flow goes back to step S27c. If the answer is "no", i.e. if the counter / has reached its maximum value, then there is no more data in the real data array and the Average value as calculated is equal to r_def, i.e. the recommended minimum value of the measurement increment r for the transformation step. In case the system acquires new on-line data, the variable i max takes a new higher value and the calculations are resumed until the new "no" reply to the test in block-scheme S27e. If the analysed data do not contain the minimum and maximum values for each point and are represented only by a single value for each point, for example open price, then r_def is defined as the average absolute value of the difference between the values of two neighbouring points, i.e. as the average distance between all pairs of the neighbouring points in the array. IV.4)-b2 Transformation from Real Space to Increment-Change Space Fig. 28 illustrates a flowchart describing the operations of a program module to transform the real market data into a trajectory in Increment-Change Space. In step S28a, the system receives real data from the information storage means 7. It can be real-time market data, delayed market data, archived market data or any other type of real market data. In step S28b, the user can select the measurement increment r himself, choose as r the optimal increment r_det 'from the system or select the increment r while being guided by the recommended value r_def from the system. It is to be recalled that though the method is applicable to any range of r, it has been demonstrated that the optimal values of r are greater or equal to the average amplitude r_def. In step S28c, the system initialises variables and arrays necessary to carry out the tranformation. The variable initialisations concern two variables : a first iterative counter / ' , that is the ordinal number of a real point in the real data array and a second iterative counter j, that is the ordinal number of the point in Increment-Change Space, both starting values equal to 0. The array initialisations concern two arrays, RrealQ and Rincr[], i.e. the real data array and the Increment-Change Space data array, both of which are initialised at 0 respectively for / = 0 and j = 0. In step S28d, the counter / is incremented by one. In step S28e, a decisional test is executed for current / value to determine if the absolute value of the difference Rreal minus Rincr is less than r, i.e. in an iterative manner. If the answer to this test is "yes", the corresponding real point / ' is not selected to fix the next Increment-Change Space point and the flow goes to step S28f where it is verified if all real points have been treated. If it is not the case, the flow goes back to step 28d. If it is the case, the flow goes to a step 28i where the values of Rincr for all the Increment-Change Space points j are calculated according to the expressed formula, the constant being chosen in such a way that the values Rincr[] are integers. If the answer to the decisional test at step S28e is "no", the corresponding real point / is selected to fix a new Increment-Change Space point and the flow goes to step S28g where the countery is incremented by one. Then, in step S28h, the vertical coordinate of the new selected point in Increment-Change Space is calculated by adding +/-r to the vertical coordinate of the previous selected point. For every point in Increment-Change Space, i.e. for every j, the "+" or "-" sign is chosen in such a way that the point in Increment-Change Space moves in the direction of the current real point. As the main result the parameter-normalized trajectory is obtained in the Increment-Change Space. In step S28j, the user can optionally select the q max value calculated by the system. This optional step is outlined separately in the hereunder-described section entitled "calculation of q max ". In step S28k, the user can choose to visualize the trajectory in Increment-Change Space. IV.4)-b3 Smoothing method Fig. 29 illustrates a flowchart of a program module to carry out the smoothing method, i.e. a method to remove excessive "roughness" of a trajectory in Increment-Change Space. It is to be recalled that the smoothing has to be repeated until the curve becomes sufficiently smooth to facilitate the analysis of the resulting image. By experience of the inventor, it has been established that a such optimal number of repetitions usually lies between four and ten. However, this range is by no means exclusive; moreover, any other stopping criteria can be used. In particular one can exit the repetition loop while the latest change of the smoothed out parameter is less than a certain value. In step S29a, the system has at its disposal a trajectory in Increment-Change Space. This trajectory can be the parameter- or time-normalized trajectory as considered above, the fastest trajectory, the beam-average curve or any other trajectory in Increment-Change Space. In step S29b, the user chooses the number of smoothing repetitions, i.e. z, and the starting point for the smoothing procedure. In step S29c, the system initialises variables and arrays necessary to carry out the smoothing. The variable initialisations concern two variables, i.e. an iterative counter j, that is the ordinal number of the smoothing, the starting value of which being 1 , and iincr, i.e. the number of the last point in Increment-Change Space for the trajectory R[], with respect to the starting point of smoothing. The array initialisation concerns Rsmooth[], i.e. the vertical coordinate array of points on the smoothed trajectory. The initial element Rsmooth[ ] is initialised as Rsmooth[0]=R[initial point], where R[initial point] is R[] in the starting point of the trajectory to be smoothened. The counter / is the ordinal number of the point of the smoothed out trajectory with respect to the chosen starting point of smoothing. At step S29d the initial counter / is initialised to 0. In step S29e, for every point / on the chosen normalized trajectory, Rsmooth is calculated as being the average mean between its own value and its previous value. In step S29f, a decisional test is run to determine if / < i max , i.e. if the ordinal number of the current point on the trajectory is less than the number of the last point in Increment-Change Space for this trajectory, always with respect with the starting point of smoothing. If the answer to the test is "yes", i.e. if the last point on the trajectory is not yet reached, then at a step S29g, the value of / is incremented by one and the flow goes back to step S29e. If the answer is "no" in step S29f, the flow goes to step S29h where it is verified if the ordinal number of the current smoothing is less than the number of repetitions of the smoothing method as defined in step S29b. If the answer is "yes", i.e. if the number of repetitions is not reached, then the flow goes to a step S29i where the ordinal number of the smoothing is incremented by 1 and the flow goes to a step S29j where a reassignment of the array RsmoothQ into the array R[] is made. Then the flow goes back to step S29d. If the answer is "no" at step S29h, i.e. if the number of repetitions of smoothing as selected by the user is reached, the running of the smoothed method is finished and the smoothed out trajectory is displayed for visualisation in step S29k if required by the user. IV.4)-b4 Trend line plotting Fig. 30 illustrates a flowchart describing the operations of a program module to carry out the trend line plotting, i.e. the plotting of the support and resistance lines. The calculation of parameters for support and resistance lines are based on the solution of the compatibility equation (30), described in detail in section 111.1). In step S30a the user selects two points of the trajectory in Increment-Change Space, defines the coefficient q by himself or guided by the data processing system as described in the next section IV.4)-b5. He also defines the type of trend to be plotted, i.e. alpha, beta, gamma or abc and its direction. In step S30b the system defines the quantum number n for the line connecting the points specified by the user (according to formulae (38) and (40.2). In step S30c the system analyses expression (33) to make a decision on the possible types of existing compatible solutions. If condition (33) is fulfilled, it is possible to define alpha- beta- and gamma-solutions (using formulae (32), (34), (35), (40.4) or (40.5) from section 111.1)). If the user chose q_max as the value of q only alpha-solutions exist. Corresponding quantum numbers of the compatible trend are calculated using the formulae (32), (40.4) or (40.5). After calculating the specific value of the quantum number of the compatible trend, the line slops for the trend's support and resistance lines are defined. Lines with such angles of inclination are drawn through the points specified by the user. In step S30d the system produces a visualization of the support and resistance lines. This function is optional. IV.4)-b5 Calculation of q max Fig. 31 illustrates a flowchart describing the operations of a program module to carry out the calculation of qjmax, i.e. the maximum of all values of q corresponding to a specific range of analysed data. Details of different ways of defining q_max are discussed in section IV.2)-e. This method can be optionally performed before the trend line plotting procedure described above in section IV.4)-b4, to assist the user in choosing the value of q. In step S31a, the system has at its disposal a trajectory R[] in Increment- Change Space and its measurement increment r. In step S31b, the program initialises variables necessary to carry out the calculation of qj ax. The variable initialisations concern four variables: i max , the number of the last point of the trajectory; two iterative counters / and j that define the scanning of the trajectory, that is the ordinal number on the Evolution Time coordinate axis of a point on the trajectory, their starting values being 0 and their final values being equal to and qjmax the starting value of which is equal to 0. In step S31c, a decisional test is executed to determine if the counter / ' is less than its maximum value, i.e. i max . If the answer to this test is "yes", i.e. if the counter / has not yet reached its maximum value, then the flow goes to a step S31d where the value of the counter / plus one is set as the value of the counter j. If the answer is "no", i.e. if the counter / has reached its maximum value, then there are no more points on the trajectory and the program produces the qjmax value as calculated. In step S31f, a decisional test is executed to determine if the counter; is less than its. maximum value, i.e. i max . If the answer to this test is "no", i.e. if the counter; has reached its maximum value and there are no more points on the trajectory, then the flow goes to step S31g where the counter / is incremented by one and the flow goes back to step S31c. If the answer is "yes", i.e. if the counter ; ' has not yet reached is maximum value, then the flow goes to a step S31 h where q is calculated for the points / and j as expressed. Then the flow goes to a step S31i where the current value of qjmax is compared to the obtained value of q. If qjnax is less than q, then the flow goes to a step S31j to set q as qjnax, i.e. the new qjnax again has the maximum value. If qjmax is greater than q, the flow goes to a step S31k where the counter; is incremented by one, then the flow goes back to step S31f. As the determination of qjmax requires large resources, it can be carried out not for every new point but upon the receipt of a defined number of new points. To speed up the calculations, it is also possible to form an array of the inflection points of the trajectory (these are the points where the trajectory's direction changes). The number of such points is smaller than the number of all points of the trajectory. Thus, using the array of inflection points to calculate the current value of q lowers the amount of resources and time needed to carry out the calculations. IV.4)-b6 Drawing the second trend line Fig. 32 illustrates a flowchart describing the operations of a program module for drawing a second trend line (i.e. the complementary support or resistance line) in Increment-Change Space, after a first one has been drawn by the user. In step S32a, the user draws by using the mouse or any other means the first straight line in Increment-Change Space with increment r, defines q by himself or is guided by the system that calculates qjmax or chooses automatically qjmax. The user also indicates the direction of the shift to draw the second trend line. In step S32b, the system defines the quantum number n for the first drawn trend line and in step S32c, it calculates the trend's localisation ΔR between the first drawn trend line and the second trend line to be drawn. In step S32d, the system defines the equation of the second trend line, which is parallel to the first one and shifted by ΔR in the direction as indicated by the user in step S32a. In the final step S32e, the system produces a visualisation of the second trend line, if required by the user. IV.4 -b7 Splitting into several trajectories Fig. 33 illustrates a flowchart describing the operations of a program module for transforming (splitting) the curve in real space into several trajectories in Increment-Change Space. The splitting method is illustrated in Fig. 5A, Fig. 6B and Fig. 8A, Fig. 8B and discussed in section 11.1). In step S33a, the system has at its disposal data of a curve in real space. In step S33b, the user defines the number of splittings w he wishes, i.e. the number of split trajectories to obtain, and the starting point from which he wants the program to begin its splitting process. It is to be noted that in practice, it is convenient that the user specifies the starting point in Increment-Change Space, and the program automatically identifies the corresponding point in real space. In that case the increment r is already defined; however, if the starting point is chosen differently the value of r needs to be specified as well. In step 33c, the program initialises variables and arrays necessary to carry out the splitting process. The variable initialisation concerns one iterative counter / that defines the ordinal number of a split trajectory, the starting value of which is equal to 1. The value of the first starting point of the real trajectory will be used for splitting Ri[0]=R[initial] which is equal to the value of the initial point of the trajectory in real space. In step S33d, the program calculates the first split trajectory in Increment-Change Space. This operation is described above in section IV.4)-b7. In step S33e, a decisional test is executed to determine if the ordinal number of the current split trajectory is less than w, i.e. if the number w of splitting steps as defined by the user is reached or not. If the answer is "yes", i.e. if the number of wished split trajectories is not yet reached, the iterative counter / is incremented by one in step S33f. If the answer is "no", i.e. if all the w split trajectories have been calculated, the flow goes to a step S33i where an optional visualisation of the w split trajectories in the Increment-Change Space is carried out. It is to be noted that, depending on the user's objectives, the system offers the capability to depict at the step S33i only a part of the derived trajectories or only the borders of such trajectories. In step S33g, the program calculates, as expressed, for each splitting step / ' , the current starting point of the real trajectory, which will be used to obtain the current split trajectory. These starting points are stored into the one- dimensional arrays R|[0]. It is to be noted that it is possible to use R-,[0] = Rι[0] - (i-1) * (r/w) as well as other methods of defining Rj[0] instead of the one proposed in step S33g, lying within R^O] +/- r. It is to be recalled that all starting points of the w split trajectories in Increment-Change Space are superposed. In step S33h, the system calculates the i-th split trajectory in Increment-Change Space. Then the flow goes back to step S33e. IV.4)-b8 Determination of the fastest trajectory Fig. 34 illustrates a flowchart describing the operations of a program module for drawing the fastest trajectory (see section IV.2)-c and IV-3)). In step S34a, the system has at disposal a real data array, the beam's starting point in real space and the number of splitting steps w. In step S34b, the program initialises a single variable necessary to carry out the splitting process, i.e. the variable / which is the ordinal number of every point in the real data array, calculated from the starting point (the point of splitting into a beam). The initial value of / is 0 and its maximum value is i max , i.e. the ordinal number of the last point in the real data array. In step S34c, the section of the real data array from / = 0 to the current value of / is split into w trajectories in Increment-Change Space. In step S34d, for every point / ' , the program searches for the fastest trajectory (-ies) among the w split trajectories. The fastest trajectory is the same as the shortest trajectory. It is to be noted that there can be several fastest trajectories and that in any case, the choice by the system of a particular trajectory among them does not affect the final result. In step S34e, the program defines the coordinate of the last point of the fastest trajectory and stores it into the array of points of the fastest trajectory. In step S34f, a decisional test is executed to determine if the current value of / is less than i max , i.e. if the last point in the real data array is reached or not. If the answer is "yes", i.e. if the last point of the array is not yet reached, then the flow goes to a step S34g where the current / value is incremented by one. If the answer is "no", i.e. if the end of the real data is reached, the system produces a visualisation of the fastest trajectory. This function is optional. IV.4)-b9 Determination of the beam-average curve Fig. 35 illustrates a flowchart describing the operations of a program module for drawing the beam-average curve. Detailed discussion on how the beam- average curve is calculated can be found in section IV.2)-c. In step S35a, the system has at its disposal the beam of w trajectories R[ ][ ] and its starting point in Increment-Change Space. In step S35b, the program calculates the fastest trajectory of the beam and defines the number i max of its last point. During the process of data handling i max can increase if new data are obtained. In step S35c, the program initialises variables and arrays necessary to carry out the determination of the beam-average curve. The variable initialisation concerns two iterative counters The counter / ' defines the ordinal number of every point in the data array R, calculated from the starting point, the starting value being equal to 0, while the counter ; ' defines the ordinal number of the trajectory, the starting value being equal to 1 The array initialisation is an initialisation at 0 of the value Rave[i] for all /, Ravefi] being the array of points of the beam-average curve. In step S35d, for every / ' , Rave[i] is calculated as expressed. In step S35e, a decisional test is executed to determine if; is less than w, i.e. if the ordinal number of the trajectory is less than the number of trajectories. If the answer is "yes", i.e. if the number of trajectories w is not yet reached, then the current value of; is incremented by one, then the flow goes back to step S35d. If the answer is "no", a decisional test is executed at a step S35g to determine if the current value of / ' is less than the number i max of the last point. If the answer is "yes", i.e. if the last point is not yet reached, then, at a step S35h, the current value of / is incremented by one and the ordinal number of the trajectory ; ' is reset to one. If the answer is "no" in step S35g, i.e. if the last point on the current trajectory is reached, the system produces a visualisation of the beam- average curve. The last function is optional. IV.4)-b10 Drawing quantum lines Fig. 36 illustrates a flowchart describing the operations of a program module for calculating and drawing the quantum lines. The ways how they can be used in analysis are described in section IV.2)-f. In step S36a, the user selects a point in Increment-Change Space, the direction - upward or downward - according to which quantum lines are to be drawn, and the maximum number i max of those quantum lines. It is to be noted that instead of the maximum number of quantum lines, it is possible to specify selected quantum numbers. In step S36b, the program initialises the single variable necessary to carry out the drawing of the quantum lines, that is / which defines the ordinal number of the quantum line n,, the starting value being equal to 1 In step S36c, the system solves the quantum line equation for the current quantum line n; which is equal to / ' . In step S36d, a decisional test is executed to determine if / is less than i max , i.e. if the maximum number of quantum lines is reached or not. If the answer is "yes", i.e. the maximum number of quantum lines is not yet reached, the flow goes to a step S36e where the current value / is incremented by one. If the answer is "no", i.e. if the maximum number of quantum lines is reached, the system produces a visualisation of the quantum lines as defined by the system. This function is optional. IV.4)-b11 Drawing the development eguation curve Fig. 37 illustrates a flowchart describing operations of a program module for calculating and drawing the development equation curve. The ways how it can be used in analysis are discussed in section IV.2). In step S37a, the user selects the value of q. It is to be noted that if the user chooses q as q = q max , the development equation curve will become the external envelope of all trajectories. In step S37a, the user also selects the starting point for the development equation curve to be drawn and its direction. In step S37b, the program calculates the coordinates along the time axis of the points on the development equation curve by using the formula (42). In step S37c, the system produces a visualisation of the development equation curve. This function is optional.

Claims: Claims Method of interactive user controlled processing of graphical images for financial data analysis, by means of a data processing system and software comprising the steps of: acquiring financial parameter data on a financial parameter to be analysed in digital or electronic format; calculation and depicting on a screen one or a plurality of broken lines, representative of the evolution of the financial parameter and drawn in such a way, that when each new point of said broken line is plotted, its coordinate along a first axis (T-axis) is always incremented by τ and its coordinate along a second axis (R-axis) is always changed either by + r or by -r , where one of said ror rvalues has to be specified by the user. Method according to claim 1 wherein each new point on the broken line is added if the absolute value of the difference between the current value of the financial parameter and the R coordinate along the R-axis of the current point on the broken line appears to be equal or bigger than r; whereby for a positive said difference the increment r of the coordinate along the R-axis is positive and for a negative difference the increment r is negative . Method according to claim 1 wherein each new point on the broken line is added for each time increment r of a financial parameter, whereby the sign of r increment corresponds to the sign of the financial parameter change within said increment τ of time. Method according to any one of claims 1 to 3, further comprising the calculation and depiction on a screen of a curve substantially defined or approximated by a result of averaging of the R coordinates of said plurality of lines for any coordinate along the T-axis after a point specified by the user as the starting point for the plurality of lines. Method according to claim 4, wherein if the user specifies the value of r , individual broken lines of said plurality of lines are obtained by shifting the financial data values or said starting point by values smaller than the value of the increment r . Method according to claim 4, wherein if user specifies the rvalue, individual broken lines of said plurality of lines are obtained by shifting the financial data time coordinate or said starting point by values smaller than the value of τ . Method according to claim 5 , wherein an end point of one of said plurality of broken lines having the smallest coordinate along said first axis (T-axis) is plotted on the screen, aforesaid step being repeated for subsequent financial parameter data to obtain a line of said end points. Method according to any one of claims 1 to 7 comprising the further step of smoothing at least one of said broken lines by substituting the coordinate of every point with a new value defined substantially or approximately by the average of the coordinate of this point and the preceding point. The method according to claim 8 wherein the smoothing step is repeated one or more times to the curve resulting from the previous smoothing step. The method according to any one of claims 1 to 9 wherein two substantially parallel straight lines defined substantially or approximately by the equations ' R^ = A iTλ + C „ x and , (Rλ = A IT^ + C '-2 where R defines the r y τ j r ) τ j coordinate along the R-axis and T defines the coordinate along the T-axis, A is a coefficient related to the distance between said straight lines | C - C 2 \ according to the equation A \ C x - C 2 1= q , where q is a numerical coefficient chosen by the user or defined by the data processing system and software. The method according to claim 10 wherein the user specifies two points through which said two straight lines are to be drawn, or one of said two straight lines are to be drawn and further indicates whether two points belong to the same line or whether they belong to two different lines. The method according to claim 11 wherein the user also defines the direction in which said straight lines are to be drawn, and in the case where two points belong to the same (first) straight line, selects whether the second trend line is to be drawn higher or lower than the first trend line. The method according to any one of claims 1 to 9 wherein a plurality of straight lines intersecting a point specified by the user are drawn , said lines δ being calculated or approximated by equation fT \ + C where R \ r J defines the coordinate along R-axis, T defines coordinate along the T-axis, n is a positive integer excluding zero, δ = ±l , and C is selected in such a way that the straight lines pass through the specified point. The method according to any one of claims 1 to 9 wherein a curve substantially defined or approximated by equation IS plotted on the screen, where R'= R -R 0 , T'= T-T Q and R 0 ,T 0 are the coordinates along the R-axis and T-axis respectively of a point defined by the user, δ = ±l and q is a numerical coefficient chosen by the user or defined by the data processing system and software. The method according to any one of claims 1 , 2, 5 or 7 - 14 wherein the data processing system and software calculates or approximates r, defined as the average absolute value of the difference between neighbouring values of said financial parameter data obtained as an array of values. The method according to any one of claims 1 ,2,5 or 7-14 wherein the data processing system and software calculates or approximates the value of r as the average difference between maximum and minimum values of an array of values of said financial parameter data, when said data comprises minimum and maximum values for regular time intervals. The method according to any one of claims 1 to 16 wherein the data processing system and software calculates or approximates values of coefficient q defined for pairs of two different points of said broken line according to the equation q = ± 1 — - , where ΔR and AT are the 4*|ΔΓ| difference of R and T coordinates of said pair of points along the R-axis and T-axis respectively . The method according to claim 17 wherein the values of the coefficient q are determined for every pair of points of the broken line , and a maximum value q max is retained by the system. Method of processing financial parameter data comprising the steps of - acquiring real financial parameter data on a financial parameter to be analysed in digital or electronic format; and - transforming, with the assistance of a data processing system and software, the real financial parameter data to Increment-Change Space, said transformation comprising the operations of - defining a measurement increment r - defining and registering a starting value of the financial parameter - registering successive values of the financial parameter every time the value thereof differs from the preceding registered value by the measurement increment r - registering the number of successively registered change of the parameter - defining and recording two-dimensional coordinates of evolution of the financial parameter in Increment-Change Space, a first coordinate parameter representing a registered relative financial parameter value as a number of measurement increments r and a second coordinate parameter representing Evolution Time as the number of successively registered changes. Method according to claim 19, wherein said transformation operations are repeated for one or more iterations for a starting value of said financial parameter different from the starting value used for the previous transformation, by a value smaller than the measurement increment r. Method according to claim 20, wherein the average value of the first coordinate parameter is calculated and recorded for each value of the number of successively registered changes. Method according to claims 19, 20 or 21 , comprising the further steps of plotting and displaying on a computer screen a trajectory or trajectories of recorded two-dimensional coordinates on a two-dimensional chart with a first axis having a scale of numbers representing the relative value R of the financial parameter as a number of measurement increments r and a second axis having a scale of numbers representing Evolution Time as a number N of successively registered changes. Method according to claim 22, including the further steps of - selecting two points of the trajectory - setting a first point of said two points as an origin of a curve - plotting on the screen a development curve from said first point as origin and passing through a second point of said two points, said curve substantially following the relation R(t)/r = 2jql , where R(t) is the value of the curve coordinate along the first axis as a function of Evolution time, t is Evolution Time, and q is a coefficient that may be determined by entering the coordinates of the second point in the relation. Method according to claim 23, including the further steps of - selecting a point of the trajectory - plotting on the screen a development curve from said point, set as an origin, said curve substantially following the relation R(t)lr = 2s qt , where R(t) is the value of the curve coordinate along the first axis as a function of Evolution time, t is Evolution Time, and q is a numerical coefficient. Method according to claim 22, including the further steps of - selecting two points of the trajectory - calculating and drawing on the screen substantially parallel resistance and support lines respectively through first and second points of said two points, said lines satisfying the equations Rι(t)/r = b * t + c-1, R∑(t)/r= b * t +c 2 where Rι(t) and R 2 (t) are the values of said line coordinates along the first axis as a function of Evolution time, t is Evolution Time, b is substantially equal to qr/AR, ci, c 2 are calculated such that said lines pass through said first and second points, q is a numerical coefficient, r is the measurement increment, and ΔR is the difference in the relative parameter value of the first point with respect to the second point. Method according to claim 22, including the further steps of - drawing or defining by a user a first support or resistance straight line satisfying the equation R(t)/r = b*t + c, where R(t) is the value of the line coordinate along the first axis as a function of Evolution time, t is Evolution Time, and b,c are numerical coefficients. - calculating coefficients b,c of the first support or resistance line. - calculating and drawing on the screen a substantially parallel complementary resistance or support line at a distance ΔR along the relative parameter axis from the first line, whereby ΔR is substantially equal to k -q- r n where q is a numerical coefficient, r is the measurement increment, k - ±1 and π is the inverse of the coefficient b of the first support or resistance line. Method according to claim 22, including the further steps of - selecting two points of the trajectory - calculating and drawing on the screen substantially parallel resistance and support lines respectively through first and second points, said lines satisfying the equations R (t)/r = b - t + c , R 2 (t) /r = b -t + c 2 where R-ι(t), R 2 (t) are the values of said line coordinates along the first axis as a function of Evolution time, t is Evolution Time, and b is equal to 1/r/β or 1/r or \ln a or Mn abc or 1/n t whereby r/ p , n Y ι n α , n abc , n t are approximately or substantially determined by the following relations: 0.5 n β = AR/2 qr + (AR 2 /4q 2 r 2 - ΔR n/qr) n γ = AR/2 qr - (AR 2 /4q 2 r 2 - ΔR n/qr) α 5 n a = ±AR/2 qr + (AR 2 /4q 2 r 2 + ΔR n/qrj 05 r/ aϋc = ΔR/2 qr where q is a numerical coefficient, r is the measurement increment, ΔR is the absolute value of the difference in the relative parameter value of the first point with respect to the second point, Δ7 " is the absolute value of the difference in Evolution Time coordinate of the first point with respect to the second point, and 1/n is the slope of the straight line joining two selected points; ci, c 2 are calculated such that said lines pass through said first and second points. Method according to claim 22, comprising the steps of selecting a point of the trajectory - calculating and plotting on the screen one or more quantum lines starting from said point and having line slope equal to Mn where n is an integer. Method according to any one of claims 24 to 28, wherein the coefficient q is determined by - selecting a first point of the trajectory as being a starting point - selecting a second point of the trajectory - calculating or approximating the difference ΔR between the first axis coordinate of the selected first and second points - calculating or approximating the difference AT between the second axis coordinates of the selected first and second points - calculating or approximating q as (AR/ή 2 / 4AT. 30. Method according to claim 29, wherein a new second point of the trajectory is selected and - repeating said calculating or approximating steps of claim 29 - repeating the above iteration with the remaining points of the trajectory and selecting a maximum value of the coefficient q. 31 Method according to claims 29 and 30, wherein a new first point of the trajectory is selected and the steps of claims 29 and 30. are iterated until all points of the trajectory have been selected as first points, selecting the maximum value of the coefficient q of all the iterations. 32. Program module for calculating a measurement increment r for transforming financial parameter data as set forth in the method according to claim 19 adapted to perform the steps of : a) receiving real financial parameter data from an information storage means as a real data array Rreal [ ] comprising maximum and minimum real values (Rreal max [ ] and Rreal m j n [ ]) ; b) initialising variables, i max , i and "Average", i max being the number of real points in the real data array, / being the ordinal number of a real point in the real data array, initially set at 0 and "Average" being a variable that accumulates the average difference between the maximum and the minimum real values, initially set at 0 ; c) calculating the variable "Average" in a cumulative way according to the formula Average = (Average * / + | Rreal max [i] - Rreal min [i] \)/(i + 1) ; d) incrementing / by one ; and e) executing a decisional test to determine if / ' is less than i m ax whereby if the answer is "yes", going back to step c) and if the answer is "no", the measurement increment r is set at the value of "Average". 33. Program module for transforming real financial parameter data into a trajectory in Increment-Change Space according to claim 19, comprising the steps of : a) receiving real financial parameter data from an information storage means as a real data array, Rreal [ ] ; b) selecting or receiving a value of a measurement increment ; c) initialising an ordinal number / of a real point in the real financial parameter data and an ordinal number; of a point in Increment-Change Space at 0 and initialising a first value Rincr [0] of an Increment-Change Space data array Rincr [ ] as being equal to a first value Rreal [0] of said real data array Rreal [ ] ; d) incrementing / by one ; e) executing a decisional test to determine if the absolute value of the difference of a value Rreal [i] minus a value Rincr ] is less than the measurement increment r and if the answer is "no", incrementing ; ' by one, calculating the new coordinate value Rincr [j] along the relative parameter axis of a new point; in Increment-Change Space by adding or substracting the measurement increment r to the previous coordinate value Rincr 0-1], and returning to the beginning of this step, and if the answer is "yes", verifying if all real points have been treated and if the answer is "no", going back to step d) ; f) calculating the value of Rincr 0] or the Increment-Change Space point ; corresponding to the real point / according to the formula Rincr 0] = Rincr 0] /r + constant, the constant being chosen in such a way that the values Rincr 0] are integers. 34. Program module for smoothing a trajectory in Increment-Change Space according to claim 33, comprising the following steps : a) receiving a trajectory in Increment-Change Space ; b) selecting the number of repetitions z of the smoothing program module and the coordinates of the starting point for smoothing; c) initialising the ordinal number; of the smoothing at 1 and the number of the last point of the trajectory in Increment-Change Space i incr with respect to the starting point of the smoothing program module, and equalizing to each other R[0] and Rsmooth [0], i.e. the coordinates, along the number of measurement increments axis, of the starting point of the trajectory and of the smoothed trajectory ; d) initialising the ordinal number of the current point on the trajectory / at 0; e) calculating Rsmooth as being the average between its own value and its previous value ; f) executing a decisional test to determine if / < i incr and if the answer is "yes", incrementing i by one and going back to step e), and else then g) verifying if the ordinal number of the current smoothing ; ' is less than the number of repetitions z of the smoothing program module as defined in step b) and if the answer is "yes", incrementing the ordinal number ; " of the smoothing by 1 and reassigning the array Rsmooth [ ] into the array R [ ] then going back to step d), and if "no", the smoothing program module is finished. 35. Program module for plotting trend lines according to claim 26, comprising the following steps : a) selecting two points in Increment-Change Space, defining the coefficient q and selecting the direction of line's shift. b) calculating parameters of the first trend line drawn through the said points c) calculating the distance ΔR according to the method as set forth in claim 26 d) calculating parameters of the second trend line 36. Program module for trend line plotting according to claim 27, comprising the following steps : e) selecting two points in Increment-Change Space and defining the coefficient q. f) selecting the type of trend to be plotted, i.e. alpha, beta, gamma, abc or t and defining its direction. g) executing a decisional test to verify whether the solution of the corresponding equation for the selected type of trend quantum number exists, and, if the answer is "yes", h) calculating the quantum number n according to the method as set forth in claim 27 for the line connecting the points selected in step a). i) calculating parameters for support and resistance lines according to the method as set forth in claim 27 37. Program module for calculating the value of a coefficient q max , comprising the following steps : a) receiving a trajectory in Increment-Change Space and its measurement increment r ; b) initialising the number / max of the last point of the trajectory, two iterative counters / and ; ' that define the scanning of the trajectory, that is the ordinal number on the Evolution Time axis of a point on the trajectory, at 0, their final values being equal to i max , and the starting value of q max at 0; c) executing a decisional test to determine if / is less than i max and if the answer is "no", the program module if finished ; d) if the answer at step c) is "yes", ; ' is set at / plus one ; e) executing a decisional test to determine if ; ' is less than i max and if the answer is "no", incrementing / by one and going back to step c) and else, then calculating q for points i and j as q = ((R[j] - R[i])/ή 2 /(4*\j-i\), R[i] and R//7 being the coordinates of points / and ; ' along the number of measurement increments axis ; f) if q ma χ is less than q, then storing q into q max , incrementing ; ' by one then going back to step e). 38. Program module for splitting a trajectory of financial parameter data as described in claim 21 , comprising the following steps : a) receiving a trajectory ; b) selecting the number of splitting steps w and the coordinates of their starting point ; c) initialising the ordinal number / of every split trajectory at 1 and the starting point of the first split trajectory in Increment-Change Space R-i [0] at O ; d) calculating a first split trajectory in Increment-Change Space ; e) executing a decisional test to determine if i is less than w and if the answer is "no", the program module is finished and else, incrementing / by one ; f) calculating a starting point, along the number of measurement increments axis, of the current split trajectory R/ [0] = R [0] + (i-1) * (r/w) ; g) calculating the /-th trajectory in Increment-Change Space then going back to step e). 39. Program module for drawing a fastest trajectory, comprising the following steps : a) receiving a trajectory representing real financial parameter data as defined in claim 21 , a starting point and a number of splitting steps w ; b) initialising at 0 the ordinal number / ' of every point on the trajectory, calculated from the starting point, its maximum value being / max ; c) splitting a section of the trajectory from / = 0 to the current value of / into w trajectories in Increment-Change Space ; d) searching for a fastest (shortest) trajectory(ies) among the w split trajectories ; e) defining a coordinate, along the number of measurement increments axis, of the last point of the fastest trajectory and storing it into an array of points of the fastest trajectory ; and f) executing a decisional test to determine if / is less than i ma χ and if the answer is "yes", then incrementing i by one and going back to step c). 40. Program module for drawing a beam-average curve, comprising the following steps : a) receiving a beam of w trajectories R[ ][ ] and its starting point in Increment- Change Space ; b) calculating a fastest trajectory of the beam according to claim 38 and defining the number / max of its last point ; c) initialising the ordinal number / of every point in the data array R, calculated from the starting point, at 0, the ordinal number ; ' of the trajectory at 1 , and Rave [i] for all i at 0, Rave [i] being the array of points of the beam-average curve ; d) calculating the value of the beam-average curve coordinate along the number of measurement increments axis Rave [i] as Rave [i] = (Rave [i] * 0-1) + RID DM \ ™<* e) executing a decisional test to determine if ; ' is less than w and if the answer is "yes", incrementing; by one and going back to step d) and else, executing a decisional test to determine if / is less than N and if the answer is "yes", incrementing / by one and resetting; to one. 41 Program module for drawing quantum lines as defined in claim 28, comprising the following steps : a) selecting a point in Increment-Change Space, a direction - upward or downward - according to which quantum lines are to be drawn, and a maximum number / ' max of those quantum lines ; b) initialising the ordinal number / of a quantum line at 1 ; c) defining a quantum line equation for the current quantum line / ' ; d) executing a decisional test to determine if / is less than i ma χ and if the answer is "yes", then incrementing / by one and going back to step c) and else, the program module is finished. 42. Program module for drawing a development curve as defined in claim 22 or 23, comprising the following steps : a) selecting the coefficient q, a starting point for the development curve to be drawn and a direction thereof ; and calculating the coordinates along the Evolution Time axis of points on the development curve by using the formula Rlr = 2 qt .

Inventors: DUKA ANDREY, DUKA, ANDREY
Applicants: DUKA ANDREY, DUKA, ANDREY
Application year: 2001
Main classification: G06F17
IPC codes: G06Q10, G06Q40, G06T11