METHOD AND OPTICAL MEANS FOR IMPROVING OR MODIFYING COLOUR VISION AND METHOD FOR MAKING SAID OPTICAL MEANS

Abstract: Method and optical means for improving or modifying human colour vision by applying a colour filter with a spectral transmission tau ( lambda ) so that it compensates, in three wavelength ranges around maximum values of spectral sensitivity curves of protos, deuteros and tritos receptors of a human eye with normal colour vision, differences between spectral sensitivity P*( lambda ), D*( lambda ), T*( lambda ), as determined, of corresponding receptors of the eye with colour vision to be modified and spectral sensitivity P( lambda ), D( lambda ), T( lambda ) of corresponding receptors of a human eye with normal or desired colour vision. The optical means may be realized as an eyeglass, a contact lens or an intraocular lens, or by any other optical implement placed between the eye and the object to be viewed.

Description: Method and optical means for improving or modifying colour vision and method for making said optical means TECHNICAL FIELD The invention relates to a method and means for improv¬ ing or modifying colour vision, and a method for making said optical means. BACKGROUND ART The human eye is able to detect electromagnetic radia¬ tion in the wavelength range of visible light which extends approx. from 380 nm to 780 nm. The light efficiency of human vision in dependence of wavelength is defined by the so-called visibility curve. In the human eye there are three orthochromatic receptors (pigments) assuring colour vision, called protos, which is sensitive to red, deuteros, which is sensitive to green, and tritos, which is sensitive to vio¬ let. Sensation of the yellow colour is aroused by simulta¬ neous stimuli of the protos and the deuteros. Simultaneous stimuli of the tritos and the deuteros causes the vision of the colour turquoise, while simultaneous stimuli of the tritos and the protos leads to the sensation of the colour purple. Other transitional shades of colours are produced by simultaneous stimuli of the three receptors with different intensities. Diagrams of spectral sensitivity of the protos, the deuteros and the tritos for people having normal (average) colour vision are well known. Fig. 1 illustrates the visi¬ bility curve V (\) for normal human eye and the sensitivity curves P( ) , D(λ) and T Qc) of protos, deuteros and tritos, respectively, for normal human colour vision. The spectral sensitivities of receptors in the eye can be determined by individual measurements (W.B. Marks, .H. Dobbelle, E.F. Mac Nichol: Visual Pigments of Single Primate Cones, Science, Vol. 143, March 1964). Rushton performed microspectrographic measurements on eyes of living human beings and monkeys (Rushton: Visual Pigments and Color Blindness, Scientific American, March 1975) . In the micro¬ spectrographic method, a thin monochromatic light beam is imaged on the retina through the pupil of the eye to be tested, the size of the light beam - when reaching the retina - does not exceed that of each receptor (protos, deuteros, tritos). The intensity of the light beam is con¬ tinuously measured prior to emission and also after being reflected from the receptor. The difference of the two corresponds to the intensity of light absorbed by the given receptor, which is characteristic of the receptor's sensi¬ tivity in the given wavelength. By altering the wavelength of the testing light beam, the spectral sensitivity curve of the given receptor can be determined (Leo M. Hurvich: Color Vision, Sinauer Associates Inc., Sunderland, Massachusetts, U.S.A., 1981, pp. 121-122). There is another method for determining the spectral sensitivity curves of receptors by a mathematical method from results of colour mixing measurements (K. Wenzel and G. Szasz: Numerical method for determining simultaneous functions having been measured with an indirect measuring method (in Hungarian), Finommechanika-Mikrotechnika, 1985, Vol. 24, No. 8/9, pp. 250-252). Results obtained by this computing method are in agreement with the results of said microspectrographic measurements. It is well known that people do not have exactly the same colour vision. So, e.g. the so-called colour blind people see only two basic colours instead of three. If there is a lack of protos receptors, the colour blind person is called protanop, in lack of deuteros receptors, we speak about a deuteranop person, and if tritos receptors are missing, the person is called tritanop. Additionally, people with anomalous colour vision are also known, and although they have all the three receptors, they see the colours in a different way than normal people. The most frequent form of anomalous colour vision appears as red-green parachromatism. People suffering in red-green parachromatism do not recog¬ nize pseudoisochromatic tables (known in practice as dotted figures) and they are not able to distinguish between red, yellow and green signals used in traffic control. Different types of parachromatism are described on pages 222 to 269 in the textbook of Leo M. Hurvich quoted above. Anomalous colour vision is an inherited characteristic and it does not change over the life-span of a person, except of colour blindness caused by certain diseases and unless the effect is temporarily caused by some poisonous materials, e.g. alcohol. As much as approx. 2.1 % of the entire population is colour blind (protanopy is approx. 1 %, deuteranopy is approx. 1.1 % and tritanopy is approx. 0.01 %) . Approx. 6.3 % of the population have anomalous colour vision (protanomaly is approx. 1 %, deuteranomaly is approx. 5.3 % and tritanomaly is approx. 0.01 %) . This means that about 8.4 % of the entire population do not see colours properly. The above data refer to male population of the Caucasian (European) group of people, while for other groups of people and for woman population investigations resulted in smaller values. Generally, colour blind persons, or people with para¬ chromatism cannot have a driver licence, they cannot be employed as typographers, industrial designers and electri¬ cians, they cannot work in textile, cosmetic and ceramic industries etc. There are more than 100 occupations which are not recommended for persons suffering in parachromatism. Attempts have already been made to correct the error of colour vision by colour filters placed in front of the eye. The solutions described in US patents 3,586,423, 3,701,590 and 4,300,819, by using a colour lens for one eye and a transparent one for the other, ensure some rough colour distinguishing ability for colour blind people, however, they do not provide any improvement for people suffering in parachromatism. In US patent 3,731,993 a colour filter was recommended for correcting parachromatism which includes colour filter components placed as a mosaic side by side corresponding to the three basic colours (red, green, blue) . The spectral transmission factor of colour filter components is inverse¬ ly proportional with the corresponding colour sensitivity of a person with anomalous colour vision. In US patent 3,877,797 an optical filter combination improving the colour distinguishing ability was recommended, which filters the light arriving into the eye in two bands, that is in the vicinity of 490 nm and 580 nm. These solutions, by diminishing the light intensity in some range of the spectrum through filtering, only achieve the result of virtually reducing amplitudes of the spectral sensitivity curve of some of the colour-sensing receptors, but, according to experiences, this approach is not suitable for correcting parachromatism. Until now, there is no implement on the market that would be able to correct parachromatism. DISCLOSURE OF INVENTION By creating the invention, it has been intended to find a solution for correcting parachromatism. Thus, a first objective of our invention is to elaborate a method by which anomalous colour vision could be corrected. A second objective is to create means suitable to improve colour vision and to modify the same, respectively. In most cases parachromatism is caused by the fact that spectral sensitivity curves of receptors of an eye with anomalous colour vision are different from the corresponding sensitivity of an eye with normal colour vision. As to parachromatism we have recognized that sensitivity curves of such an eye may be displaced along the wavelength inde¬ pendently from each other and in both directions in compari¬ son to the corresponding sensitivity curves of an eye with normal colour vision, and that there may also be some dif¬ ferences in the shape of the sensitivity curves and, there¬ fore, for a given eye spectral sensitivity curves of the protos, deuteros and tritos receptors must be analysed separately for determining the type and extent of para¬ chromatism in order to improve colour vision. We have recognized that anomalies in sensitivity curves of the receptors can be corrected by appropriately selected colour filters as, in most cases of parachromatism, the displacement of any sensitivity curve along the wavelength is of an extent that the reduction in light intensity caused by colour filters can largely be compensated for each receptor by the adaptation of human eye. E.g. the applica¬ tion of a colour filter with a transmission of 10 % causes a very little reduction in light perception owing to the logarithmic sensing characteristics of the eye. We have also recognized that, by using special colour filters, any person having normal or anomalous colour vision can be endowed with a special colour vision and, in such a manner, his colour distinguishing ability can be increased for special purposes, e.g. for recognition of plant para¬ sites, treating of foodstuffs and pharmaceutical products, detection of counterfeits, etc. Thus, on the one hand, the invention is a method for improving or modifying colour vision, in the course of which the vision of an eye of a person is modified by applying a colour filter. According to the invention the method is characterized by determining spectral sensitivity of colour-sensitive protos, deuteros and tritos receptors of the eye with colour vision to be modified, and applying a colour filter with a spectral transmission so that it com¬ pensates, in three wavelength ranges around maximum values of spectral sensitivity curves of protos, deuteros and tritos receptors of a human eye with normal colour vision, differences between spectral sensitivity, as determined, of corresponding receptors of the eye with colour vision to be modified and spectral sensitivity of corresponding recep¬ tors of a human eye with normal or desired colour vision. On the other hand, the invention relates to optical means for improving or modifying colour vision of a human eye, comprising a colour filter which has a spectral trans¬ mission so that it compensates, in three wavelength ranges around maximum values of spectral sensitivity curves of protos, deuteros and tritos receptors of a human eye with normal colour vision, differences between spectral sensitiv¬ ity, as determined, of corresponding receptors of the eye with colour vision to be modified and spectral sensitivity of corresponding receptors of a human eye with normal or desired colour vision. The invention further relates to a method for making optical means for improving or modifying colour vision of a human eye, in the course of which an optical body is formed, said optical body comprising a colour filter. According to the invention the spectral transmission of the colour filter is chosen so that the colour filter compensates, in three wavelength ranges around maximum values of spectral sensi- tivity curves of protos, deuteros and tritos receptors of a human eye with normal colour vision, differences between spectral sensitivity, as determined, of corresponding receptors of the eye with colour vision to be modified and spectral sensitivity of corresponding receptors of a human eye with normal or desired colour vision. Preferred embodiments of the present invention are described in sub-claims attached to this specification. It is an advantage of the invention that it allows eliminating or reducing parachromatism, which has been impossible so far, by optical means that are relatively simple, can be produced by technology per se known in op¬ tics, and are suitable for applying in ophthalmologic prac¬ tice. It is a further advantage that by the use of the inven¬ tion not only parachromatism can be eliminated, but a colour vision, being more selective in some respect than that of a normal eye, can also be assured. BRIEF DESCRIPTION OF THE DRAWINGS Hereinafter, the invention will be described by means of preferred embodiments shown in the drawings, where Fig. 1 is a diagram depicting visibility curve of a normal human eye and spectral sensitivity curves of colour-sensitive receptors thereof. Fig. 2 is a diagram depicting normalized spectral sensitivity curves of colour-sensitive receptors of a normal human eye, Fig. 3 is a diagram showing spectral sensitivity curves of colour-sensitive receptors of a normal human eye and those of a human eye exhibiting colour vision anomaly, Fig. 4 is a diagram showing spectral transmission characteristic of a colour filter according to the invention for improving the colour vision of an eye exhibiting the anomaly as of Fig. 3, Fig. 5 is a diagram depicting wavelength shifts of a set of lenses comprising colour filters according to the invention. Figs. 6 to 8 are diagrams showing spectral trans¬ mission characteristics of colour filters according to the invention for applying in further cases of anomalous colour vision, Fig. 9 is a diagram depicting spectral sensitivity curves of colour sensitive receptors in a normal human eye and those in a human eye exhibiting another type of colour vision anomaly, Fig. 10 is a diagram showing spectral transmission characteristic of a colour filter according to the inven¬ tion for improving the colour vision of an eye exhibiting the anomaly as of Fig. 9, Figs. 11 to 14 are schematic cross sections of differ¬ ent embodiments of the optical means according to the inven¬ tion formed as eye-glasses, Fig. 15 is a schematic cross section of an embodiment of the optical means according to the invention formed as a contact lens, Fig. 16 is a schematic cross section of an embodiment of the optical means according to the invention formed as an intraocular lens, and Fig. 17 is a schematic side view of an embodiment of the optical means according to the invention formed as a filter plate for colour TV set. MODES FOR CARRYING OUT THE INVENTION In the figures identical elements or element of identi¬ cal functions are marked by same reference signs. Fig. 1 depicts a visibility curve V (\) showing spec¬ tral light efficiency of a normal human eye, and spectral P(λ) , D(λ), T(λ) sensitivity curves of light sensitive receptors in a normal human eye, where on the vertical axis the relative spectral sensitivity S(λ) in % and on the horizontal axis the wavelength " λ in nm are shown. The visibility curve V(λ) is a resultant of the sensitivity curves PCX) , D (X) , and T (X) . It can be seen that the protos sensitivity curve P(λ) has a maximum at approx. 565 nm, the deuteros sensitivity curve D(λ) has a maximum at approx. 530 nm and the tritos sensitivity curve T(λ) has a maximum at approx. 448 nm. In Fig. 2 normalized spectral sensitivity curves P(λ) , D(λ) , T(λ) of light sensitive receptors in a normal human eye are shown, where on the vertical axis the relative spectral sensitivity s Qc.) in % and on the horizontal axis the wavelength in nm is depicted. In the diagrams shown in Figs. 3 and 9, also the normalized spectral sensitivity curves are shown. The intersection point of the normalized sensitivity curves T(X) and D( ) is approx. at 480 nm and that of the normalized sensitivity curves D(λ) and P(λ) is approx. at 550 nm. The maximum and intersection points and to a certain extent the shapes of the sensitivity curves may be different for each group of people. In the course of our experiments we have recognized that the most frequent reason for anomalous colour vision is the deviation of the sensitivity curves of the receptors from the sensitivity curves of the corresponding receptors in a normal eye. This recognition led us to compare sensi¬ tivity curves P*Cλ), D*(λ) and T*(3 of an eye to be tested with respective sensitivity curves P(λ) , D(λ) and T (\ ) of a normal eye separately. In the course of examination of persons with anomalous colour vision, we have found that the sensitivity curves of the receptors may be displaced inde¬ pendently of each other and in both directions along the wavelength axis. We have also experienced that a deviation could be found in the shape of each curve, e.g. the curve is wider or narrower than the corresponding curve of a normal eye. The displacement along the wavelength and the devia¬ tion in shape could occur simultaneously. According to the invention the following method is used for correcting parachromatism or for modifying colour vision. First of all, spectral sensitivity curves P*(X), D*(^) and T*(X) of the tested eye will be determined, e.g. by a per se known microspectrographic measurement. Then, the colour vision of the tested eye is modified by the applica¬ tion of a colour filter, i.e. practically the corresponding sensitivity curves P*(λ), D*(λ) and T*(^) are corrected so that the colour sensing of protos, deuteros and tritos receptors in the tested eye correspond to the protos, deuteros and tritos spectral sensitivity curves P(λ), D(λ) , and T(λ) of a human eye with normal or desired colour vision. The spectral transmission characteristic T ( ) of the colour filter for the above correction may be determined on the basis of the following equations: P(λ) = P*(λ) . τ P (X) (1) where P(λ), D(λ) and T(λ) are sensitivity curves of protos, deuteros and tritos receptors of a human eye with normal or desired colour vision, P*(λ) / D*(λ) and T*(λ) are sensitivity curves of protos, deuteros and tritos receptors of the eye with a colour vision to be modified, and τp(λ) , ^D(λ) and τ τ(λ) are spectral transmission char¬ acteristics of colour filters for sensitivity corrections of protos, deuteros and tritos receptors. From the equations (1) to (3) , the transmission characteristics τ p ( ) , τp(X) and τ-p(X) are obtained as the following quotient functions: P (}) τp (λ) (4 ) P* (λ) D (λ) τ D (λ) (5) T Q) Tm . f. )π . ( 6) T* θL) The transmission characteristic τ( ) of a single colour filter correcting all receptor errors is determined on basis of the transmission characteristics TpQ), TD(A) and τrp( ) according to equations (4) to (6) , substantially as a resultant thereof. In determining the resultant, sensitivity curves P(λ) , D(^) and T(λ) of the receptors in a normal human eye, as shown in Fig. 2, are taken as a basis. The transmission characteristic Tp(λ) is chosen in a first wavelength range around maximum value of spectral sensitivity curve P(λ) of protos, the transmission charac¬ teristic TD( / 0 in a second wavelength range around maximum value of spectral sensitivity curve O ( " \) of deuteros, and the transmission characteristic τ<-, ( ' \) in a third wavelength range around maximum value of spectral sensitivity curve T( ) of tritos, of a human eye with normal colour vision. Boundary values of said three wavelength ranges can be fixed according to intersection points of normalized sensi¬ tivity curves P(λ), D(^) and T ( ~ \) of a normal human eye. So the first wavelength range extends from a first wavelength value, namely 550 nm, corresponding to the intersection point of sensitivity curves P(λ) and D(λ) to 780 nm, the second wavelength range extends from a second wavelength value, namely 480 nm, corresponding to the intersection point of sensitivity curves D( ) and 1 ( ~ ) to said first wavelength value, and the third wavelength range extends from 380 nm to said second wavelength value. The boundary values of said three wavelength ranges can also be fixed according to maxima of sensitivity curves P(λ), D(λ) and T(λ) of a normal human eye so that the boundary values are at midpoints between wavelength values at said maxima. In this way, said first and second wavelength values are 548 nm and 489 nm, respectively. In practice, the first and second wavelength values can be chosen within ranges 550 ± 30 nm and 480 ± 20, respectively. However, the curve consisting of three sections so obtained generally does not represent a continuous function, discontinuities may occur at the boundaries of wavelength ranges. According to the invention, the transmission characteristic T (λ) can be derived from said curve in different ways. In a first method, a continuous curve is matched to the three sections as far as technically possible. Hence, at discontinuities between sections the continuous curve passe from one section into the adjacent section on a path as short as possible. In another method, a continuous curve is derived by eliminating the disconti¬ nuities by multiplying the sections by constants. The con¬ stant can be determined e.g. by dividing the higher value by the lower value at each discontinuities, and multiplying each value of the section associated with the lower value by the constant so obtained. Breakpoints in the continuous curve, which might occur at the boundaries of the wavelength ranges, are rounded off in the course of practical realiza¬ tion. According to a further method, by multiplying the sections by constants, the constants are determined so that the decrease of light intensity in particular wavelength range caused by the colour filter, which decrease would exceed the adaptation ability of the eye, is reduced. In this case, a continuous curve is obtained by approximating a curve to the three sections multiplied by constants. The continuous curve so obtained is normalized in order that the colour filter has the lowest possible light absorption. For an optimal normalization each value of the continuous curve is divided by the maximum value and multi¬ plied by 100 within the wavelength range (380-780 nm) of visible light. Preferably, the normalization shall be made to at least 90 %. After the normalization the transmission characteristic τ(λ) to be realized is obtained. The light absorption caused by the colour filter of transmission characteristic τ (X) is compensated for each receptor within certain limits by the adaptation ability of the eye. Because of the eye's higher sensitivity caused by the adaptation, it is advisable to coat the optical means according to the invention with a protecting layer per se known, providing protection for the eye against UV radia¬ tion. Fig. 3 depicts sensitivity curves P(X), D(X) , T(X) of colour sensitive receptors in a normal human eye, and sensitivity curves P*(λ), D*(X), T*(Α) of corresponding receptors in an eye with anomalous colour vision. The sensitivity curve P*(λ) is displaced in the direction of greater wavelengths in comparison to sensitivity curve P(X) and its shape also deviates from that of sensitivity curve P( " X). The sensitivity curve D*(X) is displaced in the direction of smaller wavelengths in comparison to sensi¬ tivity curve D(λ) and its shape is practically the same as that of sensitivity curve D(X) . Further, sensitivity curve T*(X) is displaced in the direction of greater wavelengths in comparison to sensitivity curve T(X) and its shape is also different from that of sensitivity curve T(λ). The extents of the displacements are as follows: Δλp = 17.5 nm, Δλo = ~ 4 nm Δ T = 17.5 nm. Fig. 4 shows spectral transmission characteristic τ(λ) as a function of wavelength of a colour filter correcting the parachromatism as per Fig. 3. It can be seen that the transmission characteristic τ(λ) has a monotonously de¬ creasing transmission in the wavelength range around the maximum value of the sensitivity curve T(λ,), while the transmission monotonously increases in the wavelength range around the maximum value of the sensitivity curve D(λ), and again monotonously decreases in the wavelength range around the maximum value of the sensitivity curve P(X) . The colour vision of the eye with said parachromatism is influenced by this colour filter so as if the sensitivity curve T*(λ) shown in Fig. 3 would be shifted to the left by A ~ \ rp, the sensitivity curve D* (X) to the right by λ D and the sensitivity curve P*( ) also to the left by Δλ . In order to practicability, the transmission characteristic τ (X) is rounded off at the boundaries of the wavelength ranges. If the spectral sensitivity curves P*(X), D*(λ), T*φ) of the tested eye are practically of the same shape as the spectral sensitivity curves P(λ), D( ), T(X) of an eye with normal colour vision, and there is only a displacement in the direction of longer or shorter wavelengths at one sensitivity curve, or at two or even at all the three sensitivity curves individually, a colour filter can be applied, which has a transmission characteristic τ (X) that results in a shift of the light coming into the eye so that, in each of said three wavelength ranges around maximum values of sensitivity curves P(λ) , D(X) and T(Λ) of an eye with normal colour vision, the transmission characteristic τ(X) is monotonously increasing thereby causing a shift of the light in the direction of smaller wavelengths, or monotonously decreasing thereby causing a shift of the light in the direction of greater wavelength, or of a sub¬ stantially constant value causing practically no shift along the wavelength. In such cases, it is enough to deter¬ mine the displacements of maximum values of the sensitivity curves P*(X), D*(X) and T*(X) of the tested eye for estab¬ lishing the transmission characteristic τ(X) of the colour filter in each of said three wavelength ranges. The transmission characteristic τ (X) of the colour filter providing said wavelength shifts can be obtained by generating three quotient curves from spectral sensitivity curves P(X) , D(λ) and T(λ) of a human eye with normal or desired colour vision and curves obtained by shifting maxima of these spectral sensitivity curves to maxima, as deter- mined, of corresponding spectral sensitivity curves P*(λ), D*(X) and of the eye with colour vision to be modi¬ fied, and choosing the spectral transmission in each of said three wavelength ranges substantially according to the respective quotient curve. It has been found that a majority of the eyes with anomalous colour vision exhibit only a displacement along the wavelength as mentioned above, and in most cases of parachromatism there are displacements at sensitivity curves P*(X) and D*(λ), only. For a correction of such anomalous colour vision, according to the invention, pre-manufactured set of eye-glasses or contact lenses can be used, similarly to known sets of dioptric lenses. Members of such set repre¬ sent a two-dimension multitude, as shown in Fig. 5, and are fitted with colour filters that ensure a shift of transmit¬ ting light along the wavelength in said wavelength ranges around maximum values of spectral sensitivity curves P( .) and D(λ) of a human eye with normal colour vision according to coordinate values Δ^p and Δλβ, respectively, of Fig. 5. The Δλp and Δl D coordinate values are changing incremen¬ tally, preferably in steps of 5 nm. If displacements of tritos sensitivity curves T*(X) are also taken into account, these are of lesser importance in parachromatism, the set represents a three-dimensional multitude. As shown in Fig. 5, A\ D on the horizontal axis and λp on the vertical axis may have values of 0, ±7.5, ±12.5, ±17.5 and ± 22.5 nm. If the sensitivity curve D*( ) of an eye with colour vision to be corrected is displaced e.g. by 6 nm towards greater wavelength and the sensitivity curve P*(λ) of the same eye is displaced e.g. by 12 nm towards smaller wavelengths, then a member of the set, marked by an asterisk in Fig. 5, is selected for the correction. This member provides for the transmitting light a shift of 7.5 nm towards greater wavelengths in the wavelength range around the maximum sensitivity of deuteros and a shift of 12.5 nm towards smaller wavelengths in the wavelength range around the maximum sensitivity of protos, which, in prac¬ tice, ensures an appropriate correction of this parachro¬ matism. The optical means improving or modifying colour vision according to the invention can be implemented in many ways. A colour filters with a desired transmission characteristic T(λ) can be advantageously realized by per se known inter¬ ference filters consisting of optical thin-layers. By means of interference filters, a colour filter of almost any transmission characteristic τ(X) can be made. In this tech¬ nology numerous thin-layers of different materials and with thicknesses falling into the μm range are applied on glass or plastic carrier. The thicknesses and materials of the layers can be designed by computer programmes commercially available. As input data for the design, it is sufficient to specify the transmission characteristic τ(λ) of the colour filter to be implemented. In some cases, the colour filter may be made from coloured glass or plastic of appropriate transmission, or from the combination of such coloured glass or plastic layers. In the literature and in glass catalogues spectral transmissions of numerous coloured glasses are described (e.g. Van Fanderlik: Optical Properties of Glass, Elsevier, Amsterdam, 1983, pp. 154-155). The colour filter according to the invention may also be implemented by a glass or plastic carrier having on its surface one or more dye layers of appropriate transmission. By eye-glass painting procedures usually applied in the optical industry, water or alcohol based solutions of aniline dyes with various spectral transmission can be applied on a lens surface. An appropriate transmission τ(X) can be assured by subtractive mixing of various dyes, i.e. by an appropriate selection of material composition and thickness of dye layers applied. The painting can be con¬ served by a protecting thin Si0 2 layer. The colour filter according to the invention may also be realized by a combination of the technologies mentioned above. E.g. it is possible to ensure a required transmis¬ sion through joint use of coloured glass and dye on its surface. The interference filter may be combined with col¬ oured glass, so that the optical thin-layers are applied on a coloured carrier. In the following some examples will be given for colour filters used in optical means according to the invention. Example 1 By testing a given person's eye, it has been deter¬ mined that each of the sensitivity curves of the protos and deuteros was displaced by 17.5 nm towards greater wave¬ lengths, while the tritos receptors were of a sensitivity corresponding to that of a normal eye. This means that Δλp = 17.5 nm, Δλ D = 17 - 5 nm and ΔtT = °* For protos correction a colour filter of transmission characteristic τp(X) as shown in Fig. 6 would be necessary, while for deuteros correction a colour filter of transmission charac¬ teristic TD( ) also shown would be required. For tritos no correction is necessary, and this corresponds to a horizon¬ tal transmission characteristics Tιj-(λ) • T ^e transmission characteristics τp(X) and T-Q (X) are obtained according to equations (4) and (5) , respectively. The transmission char¬ acteristic T(Λ) to be implemented, as shown by dotted line in Fig. 6, is generated so that the transmission character¬ istics τp(λ), τ D (X) and τ τ ( ) are chosen in the wavelength ranges from 550 to 780 nm, from 480 to 550 nm, and from 380 to 480 nm, respectively, and these three sections are multiplied by constants in order to obtain a continuous curve. The colour filter can be implemented by applying optical layers of specified materials and thicknesses on a carrier by means of any thin-layer technology, e.g. by vaporizaton. To obtain the transmission characteristic τ (X) as shown, the following twelve thin-layers are applied in sequence on a glass carrier. Layer 1 0.12 μm MgF 2 Layer 2 0.75 μm Si0 2 Layer 3 0.25 μm Zr0 2 Layer 4 0.25 μm Si0 2 Layer 5 0.25 μm Zr0 2 Layer 6 0.25 μm Siθ 2 Layer 7 0.25 μm Zr0 2 Layer 8 0.25 μm Si0 2 Layer 9 0.25 μm Zr0 2 Layer 10 0.25 μm Si0 2 Layer 11 0.30 μm Zr0 2 Layer 12 0.15 μm Si0 2 As a thirteenth layer, a UV-protecting layer per se known can be applied. As a carrier, e.g. a +2D eye-glass is used, if the person uses this eye-glass on his tested eye. If he does not wear glasses, the layers are applied on a 0D eye-glass. Example 2 The sensitivity curves of protos and deuteros of the tested person's eye were displaced towards smaller wave¬ lengths by 27.5 nm and 17.5 nm, respectively, while the tritos receptors had a sensitivity corresponding to that of a normal eye. This means that p = -27.5 nm, λβ = -17.5 nm and ΔXT = °« For protos correction a colour filter of transmission characteristic Tp(λ) as shown in Fig. 7 would be required, while for deuteros correction a colour filter of transmission characteristic τjy ( ) also shown would be necessary. The transmission characteristics τ P (λ) and τ D (λ) are obtained according to equations (4) and (5) , respective¬ ly. For tritos no correction is necessary, and this corre¬ sponds to a horizontal transmission characteristic τ τ (X). The transmission characteristic T (X) of the colour filter to be implemented, as shown by dotted line in Fig. 7, is gener¬ ated so that the transmission characteristics τp(λ), τj)(λ) and Trp(λ) are chosen in the wavelength ranges from 548 to 780 nm, from 489 to 548 ' nm, and from 380 to 489 nm, respec¬ tively, and a continuous curve is approximated to these three sections. The colour filter can be realized by apply¬ ing optical layers of specified materials and thicknesses on a carrier by means of any thin-layer technology. To obtain the transmission characteristic τ(X) as shown, the following ten thin-layers are applied in sequence on a transparent plastic carrier. Layer 1 0.25 μm MgF 2 Layer 2 0.95 μm Zr0 2 + Ti0 2 compound Layer 3 0.25 μm MgF 2 Layer 4 0.25 μm Zr0 2 + Ti0 2 compound Layer 5 0.25 μm MgF 2 Layer 6 0.25 μm Zr0 2 + Ti0 2 compound Layer 7 0.25 μm Si0 2 Layer 8 0.25 μm Zr0 2 Layer 9 0.40 μm Si0 2 Layer 10 0.50 μm MgF 2 The compound Zr0 2 + Ti0 2 is a product manufactured under Code No. 16413 by the firm MERCK. It is advisable to apply a per se known UV-protecting layer as an eleventh layer. As a carrier e.g. a -2D eye-glass is used, if the person wears such eye-glass on his tested eye. If he does not wear glasses, the layers are applied on a OD eye-glass. Example 3 By testing a given person' s eye, it has been determined that the sensitivity curve of the protos was displaced by 12.5 nm towards smaller wavelengths, the sensitivity curve of the deuteros was displaced by 7.5 nm towards greater wavelength and the tritos receptors had a sensitivity cor¬ responding to that of a normal eye. The maxima of sensitivity curves P*(λ) and D* ) are 20 nm closer to each other than in the case of normal colour vision. This means that Δλp = - 12.5 nm, Δλ D = 7.5 nm and Δ^τ =0 - For protos correction a colour filter of the transmission characteristic τ P (X) as shown in Fig. 8 would be necessary, while for deuteros correction a colour filter of transmis¬ sion characteristic T"D(X) also shown would be required. For tritos no correction is necessary, and this corresponds to a horizontal transmission characteristic τ τ (λ) . By generat¬ ing the resultant of these three transmission characteris¬ tics, as described in Example 1, the transmission character¬ istic T (X) of the colour filter to be implemented is ob¬ tained, as shown by dotted line in Fig. 8. The colour filter can be realized by applying optical layers of specified materials and thicknesses on a carrier by means of any thin-layer technology. To obtain the transmission character¬ istic τ(λ) as shown, the following eight thin-layers are applied in sequence on a glass carrier. Layer 1 0.46 μm Zr0 Layer 2 0.05 μm Si0 2 Layer 3 0.05 μm Zr0 Layer 4 0.18 μm Si0 2 Layer 5 0.26 μm Zr0 2 Layer 6 0.28 μm Si0 2 Layer 7 1.74 μm Zr0 2 Layer 8 0.25 μm MgF As a ninth layer, a UV-protecting layer per se known can be applied. As a carrier, e.g. a hard +5D contact lens is used in a way that the thin-layers are hermetically sealed between two plastic half-lenses. The thin-layers are applied on one of the half-lenses and then the two half- lenses are put together and melted along their edges (Fig. 15) . Example 4 By testing a given person's eye, it has been determined that the sensitivity curves of the protos and deuteros were displaced towards greater wavelengths by 10 nm each, while the tritos receptors were of a sensitivity corresponding to that of a normal eye. This means that Δλp = 10 nm, ΔAD = 10 nm and = °* FΪ9* 9 shows the sensitivity curves P(X), D(X) , T(λ) of receptors in a normal human eye and also the sensitivity curves P*(λ), D*(λ) and T*(X) of the recep¬ tors of the eye exhibiting the anomaly as above. For the correction of the anomaly a colour filter of a transmission characteristic τ(X) as shown in Fig. 10 is suitable, which can be implemented by means of a 2 mm thick glass filter made of a coloured glass manufactured by the firm BALZERS under Code No. 8006T240. The optical means for improving or modifying colour vision comprising a colour filter of transmission T (X) can be made as conventional eye-glasses, in the form of contact lens or intraocular lens, or as any other optical means placed between the eye and the object to be viewed. The eye-glasses could be similar to simple sunglasses, but for people who wear glasses anyway to correct dioptric errors, a coating of optical thin-layers or a painting, forming a colour filter according to the invention, can be applied on dioptric glasses. Hereinafter, some embodiments of the optical means for improving or modifying colour vision according to the invention will be described on the basis of drawings. Fig. 11 shows optical means implemented as an eye-glass 1 comprising a negative dioptric lens 11 and a zero-dioptre coloured lens 10, which lens 10 forms a colour filter ac¬ cording to the invention. It is advisable to match the lens 10 to the standard curvature surface of the dioptric lens 11. The material of the lenses 10 and 11 could be glass or plastic. Fig. 12 shows optical means implemented as an eye-glass 2 comprising a positive dioptric lens 12 and a zero-dioptre coloured lens 13, the latter representing a colour filter according to the invention. Again, the lens 13 is matched to the standard curvature surface of the dioptric lens 12. The material of the lenses 12 and 13 could be glass or plastic. Fig. 13 shows optical means implemented as an eye-glass 3 comprising a zero-dioptre glass or plastic lens 14 and optical thin-layers 15 applied on its concave surface. The thin-layers 15 represent an interference colour filter according to the invention. The optical thin-layers 15 are shown in the drawing, for sake of visibility, much thinner than their real thickness. Fig. 14 shows optical means implemented as an eye¬ glass 4 comprising zero-dioptre coloured lenses 16 and 17, which together represent a colour filter according to the invention. The material of the lenses 16 and 17 could be glass or plastic. Fig. 15 shows optical means implemented as a contact lens 5 comprising two half-lenses 18 and 19 of hard mate¬ rial, which assure the necessary dioptres, and between them optical thin-layers 20 to make up an interference colour filter according to the invention. The thin-layers 20 are applied on one of the half-lenses, e.g. on the half-lens 18, and then the two half-lenses 18 and 19 are put together and melted along their edges 21. The biocompatible material of the half-lenses 18 and 19 hermetically seals the thin-layers 20, so they cannot cause any problem when wearing the con¬ tact lens 5. In some cases, the contact lens 5 may also be made of coloured plastic material of appropriate trans¬ mission characteristic, these contact lenses 5 may also be made of a soft material. Fig. 16 shows optical means implemented as an intraocular lens 6, which is to replace the natural lens of the eye mostly in the course of cataract operation. Between two half-lenses 22 and 23, which assure the necessary dioptres, there are optical thin-layers 24 to make up the colour filter according to the invention. The thin-layers 24 are applied on one of the half-lenses, e.g. on the half-lens 22, and then the two half-lenses 22 and 23 are put together and melted along their edges 25. The biocompatible material of the half-lenses 22 and 23 hermetically seals the thin- layers 24, so they cannot cause any problem when wearing the implanted intraocular lens 6. The intraocular lens 6 has two hapticas 26 and 27, per se known, for fixing the intra¬ ocular lens 6. Fig. 17 shows optical means implemented as a filter plate 7, which can be placed in front of a screen 29 of a colour TV set 28 having a support 33, or of a colour dis¬ play, by means of a per se known suspending structure 30. If a person with anomalous colour vision would like to watch a TV screen 29 in realistic colours, he puts on the filter plate 7. The filter plate 7 as shown comprises two glass or transparent plastic layers 31 and 32 with different colour¬ ing, but it can be made of a plate of glass or transparent plastic material on which an interference filter represent¬ ing the colour filter according to the invention is applied. However, the filter plate 7 may also be implemented in any other way already mentioned. It is also possible to apply, e.g. by vapourization, an optical thin-layer system repre¬ senting the colour filter according to the invention on the screen 29. According to the invention, not only anomalous colour vision can be corrected, but a normal colour vision can also be modified, e.g. the colour distinguishing ability of a person with normal colour vision may be improved in order to execute a special task easier. E.g. the red-green colour distinguishing ability can be improved by shifting the light coming into the eye in the wavelength range around the maximum value of sensitivity curve P towards greater wavelengths and in the wavelength range around the maximum value of sensitivity curve D(X) towards smaller wavelengths. This possibility can be applied e.g. in medical diagnosis in dermatology, in visual tasks of image processing, in quality testing of foodstuff, in sorting tasks, in special military tasks, in forgery tests of banknotes. The optical means according to the invention can be implemented so that for a person having normal colour vision, the modification of the colour vision for a special task is accomplished for one of his eye, only. In order to achieve a desired colour vision, transmission characteristic τ (λ) of the colour filter according to the invention can be determined on the basis of equations (4) to (6) in a way that instead of the sensitivity curves of receptors of a normal eye, sensitiv¬ ity curves corresponding to the desired colour vision are taken into consideration. According to the invention, the colour filter of the optical means to improve or modify colour vision is to be determined on the basis of colour vision characteristics of the given eye. In general, both eyes of a person of anoma¬ lous colour vision exhibit the same anomalous colour vi¬ sion. Rarely, there are individuals with different colour vision in both eyes, which means that, of course, each eye needs a colour filter of its own to correct its parachro¬ matism, different from the colour filter of the other eye. It will be evident to those skilled in the art that the above disclosures are exemplary only and that various other alternatives, adaptations and modifications may be made within the scope of the present invention as defined by the following claims.

Claims: CLAIMS 1. A method for improving or modifying colour vision, in the course of which the vision of an eye of a person is modified by applying a colour filter, characterized by determining spectral sensitivity of colour-sensitive protos, deuteros and tritos receptors of the eye with colour vision to be modified, and applying a colour filter with a spectral transmission so that it compensates, in three wavelength ranges around maximum values of spectral sensi¬ tivity curves of protos, deuteros and tritos receptors of a human eye with normal colour vision, differences between spectral sensitivity, as determined, of corresponding receptors of the eye with colour vision to be modified and spectral sensitivity of corresponding receptors of a human eye with normal or desired colour vision. 2. The method according to Claim 1, characterized in that the colour filter is realized by an eye-glass (1, 2, 3, 4) or a contact lens (5) or an intraocular lens (6) . 3. The method according to Claim 1, characterized in that the colour filter is placed between the eye and an object to be viewed. 4. Optical means for improving or modifying colour vision of a human eye, comprising a colour filter, charac¬ terized in that the colour filter has a spectral transmis¬ sion so that it compensates, in three wavelength ranges around maximum values of spectral sensitivity curves of protos, deuteros and tritos receptors of a human eye with normal colour vision, differences between spectral sensi¬ tivity, as determined, of corresponding receptors of the eye with colour vision to be modified and spectral sensitivity of corresponding receptors of a human eye with normal or desired colour vision. 5. The optical means according to Claim 4, character¬ ized in that the spectral transmission of the colour filter substantially corresponds in said three wavelength ranges to three curves obtained as quotients of spectral sensitivity curves of protos, deuteros and tritos receptors of a human eye with normal or desired colour vision and spectral sensi¬ tivity curves, as determined, of corresponding receptors of the eye with colour vision to be modified. 6. The optical means according to Claim 4, character¬ ized in that the spectral transmission of the colour filter is chosen so that the colour filter provides in said three wavelength ranges wavelength shifts substantially corre¬ sponding to differences between wavelength values associated with maxima of spectral sensitivity curves of protos, deuteros and tritos receptors of a human eye with normal or desired colour vision and wavelength values, as determined, associated with maxima of spectral sensitivity curves of corresponding receptors of the eye with colour vision to be modified. 7. The optical means according to Claim 6, character¬ ized in that the colour filter has a spectral transmission the values of which are, in each of said three wavelength ranges, monotonously increasing causing a shift into the direction of smaller wavelengths, or monotonously decreasing causing a shift into the direction of greater wavelengths, or substantially constant causing practically no shift along the wavelength. 8. The optical means according to any of Claims 4 to 7, characterized in that the spectral transmission character¬ istic of the colour filter has a normalized maximum value which is greater than 90 %. 9. The optical means according to Claim 4, character¬ ized in that said three wavelength ranges are a first wave¬ length range extending from 550 ± 30 nm to 780 nm, a second wavelength range extending from 480 ± 20 nm to 550 ± 30 nm, and a third wavelength range extending from 380 nm to 480 ± 20 nm. 10. The optical means according to Claim 4, character- ized in that the optical means are a dioptric or zero- dioptre eye-glass (1, 2, 3, 4) with an additive in its own material and/or painted on its surface and/or consisting of two or more differently coloured layers and/or having a set of optical thin-layers (15) on its surface forming an interference filter. 11. The optical means according to Claim 4, character¬ ized in that the optical means are a dioptric or zero- dioptre contact lens (5) with an additive in its own materi¬ al and/or painted on its surface and/or consisting of two or more differently coloured layers and/or comprising a set of optical thin-layers (20) forming an interference filter. 12. The optical means according to Claim 4, character¬ ized in that the optical means are a dioptric or zero- dioptre intraocular lens (6) with an additive in its own material and/or painted on its surface and/or consisting of two or more differently coloured layers and/or comprising a set of optical thin-layers (24) forming an interference filter. 13. The optical means according to Claim 11 or Claim 12, characterized in that the set of optical thin-layers (20, 24) are hermetically sealed into the material of the lens (5, 6) . 14. The optical means according to Claim 4, character¬ ized in that the optical means are a glass or transparent plastic filter plate (7) with an additive in its own mate¬ rial and/or painted on its surface and/or consisting of two or more differently coloured layers (31, 32) and/or having a set of optical thin-layers on its surface forming an inter¬ ference filter. 15. The optical means according to any of Claims 10 to 12 and 14, characterized by further comprising a layer protecting against UV radiation. 16. A method for making optical means for improving or modifying colour vision of a human eye, in the course of which an optical body is formed, said optical body comprising a colour filter, characterized in that the spec¬ tral transmission of the colour filter is chosen so that the colour filter compensates, in three wavelength ranges around maximum values of spectral sensitivity curves of protos, deuteros and tritos receptors of a human eye with normal colour vision, differences between spectral sensitivity, as determined, of corresponding receptors of the eye with colour vision to be modified and spectral sensitivity of corresponding receptors of a human eye with normal or de¬ sired colour vision. 17. The method according to Claim 16, characterized in that the spectral transmission of the colour filter is ob¬ tained by determining spectral sensitivity curves of protos, deuteros and tritos receptors of the eye with colour vision to be modified, generating three quotient curves from spec¬ tral sensitivity curves of protos, deuteros and tritos receptors of a human eye with normal or desired colour vision and spectral sensitivity curves, as determined, of corresponding receptors of the eye with colour vision to be modified, and choosing the spectral transmission in each of said three wavelength ranges substantially according to the respective quotient curve. 18. The method according to Claim 16, characterized in that the spectral transmission of the colour filter is obtained by determining wavelength values associated with maxima of spectral sensitivity curves of protos, deuteros and tritos receptors of the eye with colour vision to be modified, generating differences between wavelength values associated with maxima of spectral sensitivity curves of protos, deuteros and tritos receptors of a human eye with normal or desired colour vision and wavelength values, as determined, associated with maxima of spectral sensitivity curves of corresponding receptors of the eye with colour vision to be modified, and choosing the spectral transmis¬ sion so that the colour filter provides in each of said three wavelength ranges a wavelength shift substantially corresponding to the respective difference. 19. The method according to Claim 18, characterized in that the spectral transmission characteristic of the colour filter providing said wavelength shifts is obtained by generating three quotient curves from spectral sensitivity curves of protos, deuteros and tritos receptors of a human eye with normal or desired colour vision and curves obtained by shifting maxima of these spectral sensitivity curves to maxima, as determined, of spectral sensitivity curves of corresponding receptors of the eye with colour vision to be modified, and choosing the spectral transmission in each of said three wavelength ranges substantially according to the respective quotient curve. 20. The method according to Claim 17 or Claim 19, characterized in that, in determining the spectral transmis¬ sion of the colour filter, a continuous curve is matched to said three quotient curves, and said continuous curve is transformed by multiplying by a constant so that its normal¬ ized maximum value is greater than 90 %. 21. The method according to Claim 17 or Claim 19, characterized in that, in determining the spectral transmis¬ sion of the colour filter, said three quotient curves are matched to one another at boundaries of said three wave¬ length ranges by multiplying the quotient curves by con¬ stants in order to obtain a continuous curve, and said continuous curve is transformed by multiplying by a constant so that its normalized maximum value is greater than 90 %. 22. The method according to Claim 17 or Claim 19, characterized in that, in determining the spectral transmis¬ sion of the colour filter, said three quotient curves are multiplied by constants, a continuous curve is matched to curves obtained by said multiplication, and said continuous curve is transformed by multiplying by a constant so that its normalized maximum value is greater than 90 %. 23. The method according to Claim 1 or Claim 16, char¬ acterized in that said three wavelength ranges are a first wavelength range extending from 550 ± 30 nm to 780 nm, a second wavelength range extending from 480 ± 20 nm to 550 ± 30 nm, and a third wavelength range extending from 380 nm to 480 ± 20 nm.

Inventors: ABRAHAM GYOERGY, SZAPPANOS JANOS, WENZEL GOTTFRIEDNE, ABRAHAM, GYOERGY, SZAPPANOS, JANOS, WENZEL, GOTTFRIEDNE
Applicants: ABRAHAM GYOERGY, SZAPPANOS JANOS, WENZEL GOTTFRIEDNE, ABRAHAM, GYOERGY, SZAPPANOS, JANOS, WENZEL, GOTTFRIEDNE
Application year: 1993
Main classification: G02C7
IPC codes: A61F2, A61F9, G02C7