METHODS AND MEANS FOR UTILIZING APODIZED BEAMS

Abstract: Apodized beams of electromagnetic radiation are used in a transmissometer and earth motion detector. A laser beam (11) which is apodized by a conical scanning means is transmitted from a device (14) to a remote point (20) where it is retroreflected to the device to provide measurements relating to the transmissivity of the physical environment. In a different application the conically scanned apodized laser beam (11) is directed to a retroreflector (22) which is then returned to the transmitting point. Relative movement between the transmitting point and the remote point are detected by the change in beam position with respect to the retroreflector (22). With several transmitters and receivers orientated at different propagation angles different relative movement parameters are obtained. The conically scanned laser beam has a substantially Gaussian intensity profile, but alternative symmetrical profiles of other electromagnetic radiation can be used.

Description: DESCRIPTION Methods and Means for Utilizing Apodized Beams Background This invention relates to the utilization of apodized beams of electromagnetic radiation. In particular the invention is directed to a method and means of utilizing such beams which have a substantially Gaussian cross-sec¬ tional intensity profile or a profile with symmetry about the maximum intensity and being substantially symmetrical about the points of inflection of the intensity curve. With the invention, apodized laser beams are used to provide a transmissometer and an earth motion detector. A transmissometer is a device for determining the optical transmission characteristics of a particular medium. The optical transmission factor is defined as the ratio of the final intensity to the initial intensity of light after it has traversed a medium. Clearly this factor varies with the path length through the medium as well as the characteristic extinction of the medium. In the atmosphere, the transmission in the visible portion of the spectrum is effected principally by scat- tering. As a consequence, the transmission is a weak function of color and any convenient wave length can be used for such measurements. Preferably a laser beam is used, but this does not provide as accurate information as desired, because of beam steering difficulties and non- optimized beam profiles. In the prior art of lasers not related to trans¬ missometer devices, laser beams have been apodized by means of filters. Such filters present a major detrimen¬ tal affect on the intensity of the beam propagated from the device and hence long path length transmissometer applications are not practical. OM? Overall the effective results obtained from trans- missometers are relatively poor. By this invention the applicant has provided for utilization of a unique form of apodizing a beam which is a subject of a separate patent application filed simulta¬ neously with the present application under Serial No. (attorney's docket no. 160/31), and the contents of said application are incorporated by reference herein. In the prior art, U.S. Patent 3,698,820 (Hanff) there is disclosed means for measuring the transmissive power of the atmosphere where there are two transmitters and receivers, and wherein refinement of the transmitted beam is not an issue, whether by apodization or otherwise. Likewise in U.S. Patent 4,225,245 (Roiret) the means for measuring the optical transmissive power of the atmosphere for application of determining visibility at airports uses a broad spectrum light source without any refinement. Notably in both these U.S. patents signals are obtained from both transmitting and receiving ends which are regarded as active from, at least, electrical considera¬ tions. U.S. Patent 3,419,333 (Towner) is another exemplary transmissometer system using a broad spectrum light source for determining range of visibility along an airport runway. More specifically dealing with aligning beams such as laser beams there is U.S. Patent 4,146,329 (King) which has an automated system for aligning the optics and which uses a null position sensor to servo control a mirror. In U.S. Patent 3,942,894 (Maier) there is dis¬ closed a self-referencing retransmitting alignment sensor for a collimated light beam. Once again no reconsidera¬ tion is given to refine the laser beam. In U.S. Patent 3,894,804 (Detwiler) there is dis- closed simply an intensity level display apparatus for allowing measurement of beam shape and intensity during alignment of an optical system. OMPI In review of this art it is apparent that in the transmissometer utilization of a laser beam, only a broad beam is propagated so that the results of transmissivity which can be obtained are coarse and lack as much defini- tion as would otherwise be desirable. One other application of laser beams is in the detection of relative movement for measurement of distance between two points. One useful application is in the determination of any earth motion, horizontal and/or vertical which is of a progressive nature, and likewise another application is in the determination of more sudden seismic actions which could lead to more accurate predic¬ tion of earthquakes. Furthermore movement of structural objects is an important field of utilization of the laser beam technology. In the prior art relating to such fields it is always desirable to be more precise than has been previously possible. In U.S. Patent 4,284,350 (Coon) there is an example of a laser geotherm which incorporates a laser and seismic reflector wherein frequency differences are obtained as a measure of earth surface motion. Another general patent dealing with laser radar is that of U.S. Patent 3,409,369 (Bickel). It is also apparent from the Coon patent that earth motion detection using the beams of which the present invention is concerned is a relatively new art in which little work has been done. Summary of the Invention There is provided apparatus and method for utilizing a beam of electromagnetic radiation having a substantially Gaussian cross-sectional intensity profile, or a non- Gaussian profile which is substantially symmetrical about the points of inflection and a maximum intensity of the profile intensity curve. Such beam is at least partially apodized so that small changes in the beam characteristics can be measured so as to provide an indication of the i transmissivity between the transmitting point of the beam and a remote point. Another form of utilization is to provide details of the change of orientation of the propogated beam. Means for aligning the apodized beam in at least one transverse plane relative to its direction of propagation provides together with data obtained from a scanning means information which is usefully interpreted as characteris¬ tics of the physical environment. The point of inflection of the intensity curve is that point between the low and maximum point of the curve where the curve changes from concave upwards to concave downwards. Brief Description of Drawings Figure 1 is the optics layout of a transmissometer utilizing a laser beam. Figure 2 is a diagramatic view illustrating a conical scan of a laser beam of Gaussian cross-sectional intensity profile. Figure 3 is a illustrative two part figure showing scans of retroreflector array for beam steering feedback. The return beam received. hen the laser points to the right of the retroreflector (shown at the left part of this Figure) is electronically subtracted from the laser points to the left of the retroreflector. In the right part of the Figure, the electronic difference is obtained between the signal returned when the beam points to the bottom of the array and the top of the reflector for feedback. Figure 4 is a diagramatic view of aligning means for beam steering including matched wedge prisms and also the relative vector diagrams. Figure 5 is a block diagram of the major electronic components associated with the transmissometer shown in Figure 1. Figure 6 is a block digram of the electronic compon¬ ents shown in relation to the transmissometer of Figure 1. Figure 7 is a diagramatic component functional layout of an earth motion detector using an apodized laser beam. Figure 8 is a two part figure showing the sector scans of a retroreflector array similar to Figure 3, and in this case is applied to an earth motion detector device. Figure 9 is a graphical representation of a signal response as against time in an earth motion detector device. Detailed Description A transmissometer includes a laser source 10 which generates a red laser beam 11 to measure atmospheric extinction over long paths. The laser beam 11 is divided by a beam splitting means 12 which includes a polarizing beam splitter 13 such that the beam 11 is divided into a main component 15 and a reference beam 16. The source splitting means 12 also includes a mirror 17 to direct the reference beam 16 substantially parallel to the propagated main beam 15 to a beam chopping means 18. The device 14 is constituted substantially by mounting various elements on a single rigid plate 19 which is located at a generating point. At a remote point indicated by numeral 20 which may be at a distance between two kilometers and ten kilometers as indicated by arrow 21 there is located a retroreflector array 22 for returning the beam 15 propagated from the device back to the trans¬ mitting device as beam 23. The laser source 10 provides a helium-neon laser as the beam source, and is selected to have an output power of 10 milliwatts at a wave length of 633 nanometers. It operates in a single transverse mode wth a Gaussian intensity profile. The beam divergence is about one milliradian and the output light is plane polarized. : The beam splitting means 12 divides the beam 11 so that the reference beam 16 contains about ten percent of the intensity of the main beam 11. The intensity of the reference beam 16 can be coarsely adjusted by rotating the Laser beam 11 about its axis and the reference beam 16 is then turned to be parallel to the main beam 15 for entry into the laser chopper assembly 18. Such assembly 18 includes a rotatable disc with arsely adjusted by rotating the Laser beam 11 about its axis and the reference beam 16 is then turned to be parallel to the main beam 15 for entry into the laser chopper assembly 18. Such assembly 18 includes a rotatable disc with axially spaced slots, two sets of slots being at difference radii and being used to modulate the main beam 15 and the reference beam 16 at different frequencies. The reference beam 16 is then fed to a reference signal focusing mechanism 24 wherein the modulated refer¬ ence beam 16 is focused by a lens 25 onto the end of a fiber optical bundle 26. Also part of the reference signal focusing mechanism 24 is a polarizing element 27, and, in the housing 28 of the focusing mechanism 24, there is mounting space ahead of the lens 25 for filters to further attenuate the reference beam strength 16. Coarse steps in attenuation can be provided by fixed absorption filters, and finer attenuation control is provided by the rotatable polarizer 27. The main beam 15 is directed to conical scan means 29 which includes a pair of wedges 30 and 31 that rotate continuously at 5Hz. This rotation results in a conical scan of the main beam 15. The purpose of the conical scan is two fold:' firstly, it results in a time-averaged apodization of the output beam 15 and, secondly, provides a returned beam 23 which is suitably modulated for servo pointing the beam 15 towards the retroreflector means 22. The prisms 30 and 31 are rel at ively rotatable to each other in the housing 29 about an axis substantially parallel to an undeflected axis of the beam 15 and, after this is effected as desired, locking screws set the prisms 30 and 31 in a position at a selected radial angle rela- tive to each other. With the prisms 30 and 31 locked so there is a requisite deflection of the laser beam 11 as indicated by angle 32 between the nonreflected central axis 33 of the laser beam 11 and the central axis 34 of the deflected laser beam. Such deflected laser beam 11 would transcribe a conical shape as illustrated by the diverging cone 35 which over a scan cyclle transcribes a circle 36. The peak of the apodized Gaussian beam in its conical scan about the laser non-deflected axis 32 traces a circle depicted by dotted line 37. Two circles 36 and 37 are illustrated in the far field as being at the remote point which is at retroreflector 22. The direction of the scan is depicted by arrows 38 at the scanning housing 29 and 39 on the retroreflector array 22. The device also includes an alignment mirror 40 which is adjustable and is used for the initial alignment of the propagated main beam 15. The main beam 15 is then directed to vertical servo means 41 and thereafter to horizontal servo means 42. The servo means 41 and 42 are devices which are driven by the output of the servo electronics to direct the main beam.15 toward the retroreflector 20. A further elaboration of these principles are set out below. Each of the servo means 41 and 42 has a pair of prisms 43 and 44 which are aligned so that as the beam 15 passes through the wedge prisms 43 and 44 the beam 15 is deflected. The prisms 43 and 44 are relatively radially rotatable in opposite directions and the amount of rota¬ tion is controlled by a fine angle stepper motor. As the wedges 43 and 44 rotate the magnitude of the deflection of beam 15 can change from a minimum of zero to a maximum twice the deviation angle of the wedge prisms 43 and 44. In relation to Figure 4 the aligning means for steering the beam 15 shows the two prisms 43 and 44. The beam 15 incident to both prisms 43 and 44 shows no net deflection where the wedge 44 cancels the deflection effected by the wedge 43. This is further highlighted in the front view of the prisms 43 and 44 where the axes 45 and 46 in the respective prisms indicate the cancellation of deflection. As illustrated by turning the axes 45 and 46 through an angle theta oppositely through each other the net deflection is to the right hand side as represented by the sum of vectors A + B. The vertical component of deflection along the Y axes cancel out while the horizontal components of deflection along the X axes are additive. After passing through the servo means 41 and 42 the beam 15 is directed to an output mirror 47 which launches the main beam 15 for propagation from the device 14 towards the remote point 20 where the retroreflector array 22 is set up. The axis of launch of beam 15 is the same as the axis 48 about which the receiving telescope 49 is mounted on the device 14. The retroreflector array 22 effectively returns the beam 15 along path 23 so as to provide a folded measuring path. The array 22 employs fifteen corner cubic reflector elements 50, each side of which measures 2.5 centimeters. In Figure 3 the array is illustrated showing two concentric circles of the cubes 50, a larger outer circle 51 containing 12 of the cubes and a smaller inner circle in which the remaining three cubes are mounted on the circumference. As the beam 15 is projected, after conical scanning, from the device 14 to the retroreflector array 22 it sweeps over the face 52 of the array 22 so that different cubic members 50 of the array 22 are subjected to differ- ent intensities. Thus in the left hand figure of Figure 3 the phantom circle 53 indicates the beam 15 at the start of the scan to the right, the scan following the direction of arrow 54. Phantom circle 55 indicated the beam 15 in the middle of the scan to the right and phantom circle 56 indicates the beam 15 just completing the scan to the right. In the right hand part of Figure 3 the scan again follows arrow 57 and phantom circle 58 indicates beam 15 at the start of a scan to the bottom, phantom circle 59 indicated beam 15 in the middle of the scan to the bottom and phantom circle 60 indicates the beam 15 just comple¬ ting the scan to the bottom. The scans of the retrore- flective array 22 provides for beam steering feedback. The return beam 23 received during the scan of the right of the retroreflector 22 is electronically subtracted from the scan to the left of the retroreflector 22 and this difference represents the beam aiming error in the horizontal plane. Similarly the difference is computed for the right part of Figure 3 during scans to the bottom of the retroreflector 22 and the top of the retroreflector 22. This difference represents the beam aiming error in the vertical plane. The phantom circles 53, 56, 57, 58, 59 and 60 are only illustrative of the scans. In practice, the scans will usually completely cover the retroreflector array as illustrated in Figure 8. Retrieving means includes a receiving means for the retrieving of information from the beam 15 propagated to the remote point 22, and this includes the receiving telescope 49 which is used to collect and focus the reflected laser beam 23. The receiving telescope 49 includes a 12.5 centimeter diameter reflecting telescope with a primary mirror 61 and a secondary mirror 62. These mirrors 61 and 62 are mounted so that the beam 23 is centralized to pass through an aperture in the primary mirror 61 and through rear housing wall 63 of the tele¬ scope 49. In place of an eye piece for the telescope 49 there is a signal combining means 64 which receives both the reference beam 16 through the fibre optic 26 and the return beam 23 and in turn directs these beams to a CV-FI translational means 74 for translating the beam intensi¬ ties to electrical parameters. A small fraction of the combined beams 16 and 15 are directed towards an auxiliary eye piece 65 to help in aligning the device 14. The eye piece 65 includes a reticle 66 and an ocular 67. The fibre optic 26 is connected to resolver means through the signal combining means 64 through a lens 68 which assists in focusing the reference beam 16 to a polarizing beam splitter 69 within the signal combining means 64. The main portion of the beam intensity of the return beam 23 and the reference 16 is passed to the resolver means through a series of baffles 70 between which is placed an ocular 71 and thereafter to a polarizer 72 and narrow band pass filter 73 which effective¬ ly collimates and filters the beam 23 and 16 prior to entry into the translational means 74, which is a photo- multiplier tube. In designing the signal combining means 64, the light from both beams 16 and 23 is designed to fall exactly in the same area of a photocathode of the photomultiplier means 74. Also the combined beams 16 and 23 are colli- mated when passing through the polarizer 72 and the narrow band pass filter 73 and the baffles 70 effectively act as field and aperture stops for suppression of any stray light. The photomultiplier tube 74 is a commercially avail¬ able high gain tube which has an end-on-cathode with a high quantum efficiency at the wave length of the helium- neon laser. Turning now to the electronic components of the transmissometer in relation to the device illustrated in Figure 1 reference is made to Figures 5 and 6 which illustrate the major electronic components and functional lay out in relation to the transmissometer. The light or beam chopping means 18 for modulating the main beam 15 and reference beam 16 is controlled by a chopper frequency control 75 which includes a commercially available motor speed control that provides for a stable chopping frequency. The signal conditioning electronics includes a unit which adjusts the signal gain through a voltage controlled amplifier 76 which receives the elec¬ trical parameter signal representative of the reference beam intensity 16 and return beam intensity 23, such signals passing from the photomultiplier tube 74 to the voltage controlled amplifier 76 along line 77. The output from the amplifier 76 is fed along line 78 to demodulating and discriminating units 79 and 80 which are also fed along lines 81, 82 and 83 with the chopper frequency from the chopper frequency control circuit 75. The demodulator and discriminating circuitry feed the separated reference signal along line 84 and separated return signal along 85 to a ratiometric amplifer 86 which outputs along line 87 a ratio of the return signal over the reference signal. This ratio is fed by line 87 to the servo control electronics 88 which is interfaced circuitry to process signals from the conical scan means 29 indicating scanned positions. These signals are indicated as entering the servo control electronics along lines 89, 90, 91 and 92. Line 89 would represent a signal relative to the top scan position from the scan means 29, line 90 indicate a signal representative of the right scan position from the scan means 29, along line 91 passes a signal from the bottom scan position of the scan means 29 and along line 92 passes a signal from the left scan position of the scan means 29. The servo control electronics 88 calculates trans¬ mission measurements from these outputs and generates a vertical error signal along line 93 and a horizontal error signal along line 94 such signals providing information about the beam position. Signals along lines 93 and 94 are directed to a field data acquisition computer 95 which includes a CMOS computer used for data acquisition and the control of all functions of the transmissometer. The computer 95 develops the proper control strategy to drive stepper motors of the vertical servo means 41 and horizon¬ tal servo means 42 through interrogation of the error signal from the servo control electronics, and in this manner minimizes pointing error. The vertical control signai passes from the computer 95 along line 96 to the vertical servo means 41 and the horizontal control signal passes from teh computer 95 along line 97 to the horizon¬ tal servo means 42. The control computer controls the aiming of the beam 15, accumulates data, and measures the beam width to thereby obtain information representa¬ tive of the physical characteristics at either of, or between, the transmitting point of the device 14 and the remote point 20 of the retroreflector array 22. In this fashion information is obtained about the transmissivity between the generating point and the remote point 20. In addition to the apodization of the laser beam 15 achieved by the conical scanning means 29, the conical scan technique provides a means for pointing the laser beam 15 at the retroreflector array 22. The feedback signals are derived from the periodic varying intensity of the return beam 23 in its conical sweep as diagrammatical- ly indicated by the circle 36 in Figure 2 and the phantom circles 53, 55 and 56 of the left hand part of Figure 3 and 58, 59 and 60 on the right hand part of Figure 3. Conical scan position signals from the conical scan means 29 time the input of the return signal intensities into a pair of differential amplifiers. One amplifier subtracts the return signal intensity as the beam 15 passes to the left of the retroreflector array 22 from the intensity returned as the beam 15 passes to the right of the retroreflector array 22. The other amplifier is used to compute differences in the return signal intensity as the beam 15 passes over the top and bottom of the retrore- flector array 22. If both differences are zero the beam is centered about the retroarray. If the differences are other than zero, the signs of the differences indicate the direction in which the beam 15 is off target (right or left, up or down) and the magnitudes indicate the degree of positioning error. These error signals are used through the electronics described to control the servo means 41 and 42 which steer the beam 15 in the horizontal (left-right) and vertical (up-down) planes respectively. In other forms of the invention these planes may not be substantially perpendicular to each other. Aiming of the beam 15 is accomplished by the align- ment of the prisms 43 and 44 in the horizontal and ver¬ tical servo means 41 and 42. The physical principle involved in the adjustment has been described and in each means the wedges 43 and 44 are rotatable in opposite directions, preferably simultaneously, the amount of rotation is controlled by a fine angle stepper motor. As the wedges 43 and 44 rotate, the magnitude of the beam deflection can change from a minimum of zero to a maximum of twice the deviation of the angle of the wedge prisms 43 and 44. The intensity of the reflected beam 23 collected by receiving telescope 49 is dependent not only on absorption and scattering but also on beam spreading due to atmos¬ pheric turbulence. This beam dispersion is an inherent feature created by the atmospheric medium and its contri- bution to changing transmission must be established. The technique selected by the applicants is normalization of the transmission through periodic beam width measure¬ ments. Beam width, in this application, is defined as the horizontal width between half intensity points of the main beam which, prior to apodization has a substantially Gaussian cross-section and is illustrated in the associ¬ ated application Serial No. (attorney's docket 160/31). It can be measured by a controlled deflection of the beam from its centered position. In practice, the wedges 43 and 44 of the horizontal servo means 42 are rotated from the centered position in one direction and until the returned signal intensity ..Pϊ falls to one half its initial value. The prisms 43 and 44 are then rotated in the opposite direction past the center point to the opposite half intensity point. The wedges 43 and 44 are then returned to the central position. The beam width is calculated from the pulse count needed to drive the horizontal servo means 42 between the half intensity points and the initial alignment position of the horizontal steering prisms 43 and 44 in the servo means 42. In practice, a sub routine in the field data acquisi¬ tion computer is activated periodically, preferably hourly, to interrupt the transmission measurement and make the beam width measurement. The transmission data are normalized to an average beam width during data pro- cessing. The apodization through the conical scan means 29 creates a beam of uniform intensity when intergrated over time. This means that within the beam volume all partic¬ les with identical physical characteristics will absorb and scatter light the same. This is not true of light beams that have Gaussian or other shapes to their cross- sections. This uniform intensity feature eliminates a common deficiency of laser transmissometers and other long path or far field transmissometers that do not use an apodized beam. In the electronic retrieval means the servo control electronics 88 receives effectively signals of the com¬ bined return and reference intensities along line 87, four conical scan positions signals along lines- 89, 90, 91 and 92 and the chopped frequency signal along line 81. The combined signal I and lo is initially discriminated by the demodulating electronics 76, 79 and 80 which lock in on the signals I and lo chopped at discrete frequencies. These signals are then electronically ratioed to obtain the transmission parameter I/Io, or T. This information is passed to the servo control electonics 88 and in turn to the computer 95. The servo control electronics 88 serves as an electronic interface between the electro- optical and the electro-mechanical components located on the optical table of the device 14 and the control com¬ puter 95. The four scan position signals from the conical scanning means 29 indicate the position of the beam 15 in its s,can about the retroreflector 22. These signals are used to time the input of the transmission signal to two differential amplifiers. Differences in the trans¬ mission signals computed during top and bottom sector scans are integrated to develop a beam aiming error signal in the plane vertical to the scan access. Similarly, differences computed during the right and left sector scans are integrated to develop a beam aiming signal in the plane horizontal to the scan access. The vertical and horizontal error signals are passed along lines 93 and 94 to the computer 95 which generates servo control signals along lines 96 and 97 based upon the interrogation of the error signals. These control signals are then outputted to the appropriate servo means 41 and 42. By this invention there has been developed a laser transmissometer which provides for the continual pointing of the laser beam 15 at a retroreflector array 22 thereby eliminating the errors associated with changes in the beam direction due to reflactive index changes. This provides a means of normalizing the transmission data to minimize the effects of atmospheric turbulence on the dispersion of the beam 15 and provide a beam of uniform intensity. The transmissometer is designed to operate in a field installation with a folded path of ten kilometers. A decided advantage of the applicaion is facilitated by the electric passivity of the retroreflector array 22. The computer 95 effectively controls all functions of the transmissometer and it is anticipated that in operation automatic functioning for periods of a week or more without operator internention will be possible. Further¬ more the data from the transmissometer can be accessed by telephone using remote terminals that can be indefinitely far away. In other applications of the device the receiving means which is constituted by the receiving telescope 49 and associated elements on the optical table can be located at the remote point 20, and through suitable telephone wire or radio connection the information for retrieval can be related to the control circuitry located suitably at the device 14. An earth motion detector utilizing a laser beam of a substantially Gaussian cross-sectional profile which is conically scanned is next described. The description relates to a determination of changes in the relative positions between a generating point where a transmitting device is located and a remote point where a retroreflector is located. The devices can be mounted on suitable foundations on the ground, and, obviously, in alternative applications of the detector the relative movement between physical structures on the ground could easily be determined in the same manner. Furthermore various of the devices and. retroreflectors can be arranged at different points thereby to propagate laser beams in different directions, and in this fashion multidirectional indications of movement can be obtained. In Figure 7 the earth motion detector functional layout illustrates a device which includes a rigid optical table 200 on which is mounted a laser source 201 which transmits a helium-neon laser beam 202 at a wave length of 633 nanometers (red) and a power of about four milli- watts. The beam 202 enters light chopper means 203 which is a device used to modulate the laser beam 202 to enhance detection of the returned optical signal. In this connec¬ tion the chopper means 203 is associated with a reference signal detector 204 into which the beam 202 passes. The detector 204 includes a sensor to detect the modulation i parted by the light chopper means 203 and the informa¬ tion obtained thereby is used to further enhance the signal-to-noise ratio of the system. The signal detector 204 has two outputs: the main beam 205 for propagation from the earth motion, detector device at the transmitting point 1 and a modulation signal along line 206 to a signal conditioner 207 which is described further below. Beam 205 passes from the detector 204 to a horizontal servo means 206 and thereafter to a vertical servo means 207 which act to align the beam 205 relatively in the horizontal and vertical planes. Each of the servo means 206 and 207 includes wedge prisms 208 and 209, and the beam 205 firstly passes through prisms 208 and after reflection by mirrors 210 and 211 through prisms 209. This arrangement of the servo means 206 and 207 in the earth motion detector device is advantageous since the beam position can be steered by these devices very precisely. The steering wedge prisms 208 and 209 are rotated through a worm gear drive in the servo means 206 and 207, and, this greatly enhances the resolution of beam positioning and beam position deter¬ mination. The worm gear drive includes a stepper motor drive wherein each pulse sent to the stepper outputs the shaft in a rotation by some incremental angle. A control computer 212 sends signals along line 213 to control the vertical servo means 207 vertically and along line 214 to control the horizontal servo means 206 horizontally. The control computer 212 assigns a step count to one revolution of the steering wedges. The null position, where no deflection is effected by the steering wedges 208 and 209 is taken as step zero. This null position is indicated by a switch closure on each steering mechanism 206 and 207. Thereby the beam position can be noted by step position from the horizontal and vertical servo means 206 and 207. OMΠ The servo means 206 and 207 therefore are used to position the outgoing laser beam 205 on the axis of the reflector array 215. The horizontal servo means 206 corrects positioning errors in the horizontal plane to the laser beam 205 and the vertical servo means 207 corrects positioning errors in the plane vertical to the laser beam 205. The positioning information is recorded in the control computer 212 to produce a record of relative position of the transmitter at a transmitting point and the reflector array 215 at a remote point 216. After passage through the servo means 206 and 207 the beam 205 passes to conical scanning means 217 which rotates the outgoing laser beam 205 in a manner so that the beam spot that reaches the reflector array 215 at least partially apodized sweeps around and over the reflector in a circular fashion. As this is done the position of the beam 205 on its sweep is electronically tagged and this information is used to develop a feedback signal to operate the servo means 206 and 207. * Signals as to the position of the conical scan means 217 are transmitted from the conical scan means 217 along lines 218, 219, 220 and 221 to a multiplexer unit 222. As with the transmissometer these signals give an indication of the top, right, bottom, and left positions of the conical scan means 217. The output from the conical scan means 217 is re¬ flected by a fixed mirror 223 to an output mirror 224 which launches the beam 205 for propagation to the remote reflector array 215 at remote position 216. The retroreflector array 215 is made up of an array of corner cube reflectors 50 similar to that in the transmissometer and a characteristic of the corner cube reflectors is that they have a property of reflecting rays of the beam 205 that enter their field of view along a parallel path back to the transmitting device. The reflector array 215 cube reflector 50 outputs are rela¬ tively insensitive to changes in their angular position which makes them desirable for field applications at the remote point 216 which is electrically passive, in this preferred embodiment of the invention. The reflected beam 225 is returned to receiving means for retrieval of the information contained thereon. The receiving means includes a receiver telescope 226, again similar to the transmissometer telescope, which is a small reflector-type telescope used to collect the return optical signal. The output of the telescope 226 is directed to a further detector translational means 227 which acts to convert the beam information into electrical signal parameters which are then transmitted along line 228 to the signal conditioner 207. The signal along line 228 includes both the pure signal and a noise factor and through the signal condi¬ tioner 207 as modulated by the signal along line 206 from the reference signal detector 204 suitable discrimination is effected. The signal conditioner also receives a gain-control signal along line 229 from the control computer, and the function of the signal conditioner 207 is to discriminate the modulated returned signal along line 228 from the background noise and to scale the amplitude of this discriminated signal to an appropriate level. A conditioned return signal is outputted along line 230 to the multiplexer 222. The multiplexer 222 receives four conical scanning signals along lines 218, 219, 220 and 221 and the function of the multiplexer is to sort the return signal into four component signals. The four components represent the return signal intensity as the laser beam 205 points to the right, top, left, and bottom of the retroreflector array 215. The four components are outputted along lines 231, 232, 233 and 234 to an integrater 235. The integrator includes four separate integrating components 236, 237, 238 and 239 which act to integrate each of the four component return signals along lines 231, 232, 233 -and 234 respectively. The function of the integrator 235 is to average the input signals over a fixed time interval and the four average return signal components are outputted along lines 240, 241, 242 and 243 to the control computer 212. The control computer 212 functions in a threefold manner: firstly, to record the position of beam 205; secondly, to develop the control strategy to maintain aim of the transmitted beam 205; and thirdly, to develop a gain-control signal to scale the amplitude of the return signal to a reasonable level, such signal passing along line 229 to the signal conditioner 207. The output from the control computer 212 are the vertical and horizontal control signals along lines 213 and 214 respectively to the servo means 207 and 206. In the earth detection device it has been found desirable to over-apodize the intensity profile " of the laser beam 205, and in this manner an over-apodized beam profile increases the sensitivity of the device to changes in position of the beam 205. Apodization is the subject of the application which is being filed simultaneously with the present application under Serial No. (attorney's docket 160/31) and in that application profiles of Gaussian cross-section, apodized profiles and over-apodized pro- files are illustrated. By having the over-apodized time-averaged beam intensity, a slight trough is formed at the point of central intensity and two gentle lobes are formed to either side thereof. Viewed from a different standpoint this is calculated to increase the ratio of the error signal to the error in beam position horizontally across the beam. When there is a proportionately larger error signal produced for small changes in beam position horizontally across the beam, there is consequently increased sensitivity of the device to changes in relative position between the transmitting point and the remote point 216. The device is thereby of increased and more accurate sensitivity to relative positional changes. Reference is made to Figures 8 and 9 for an under¬ standing of the development of the feedback signal from the retroreflector array 215, such signal being contained as information in the beam 225. In Figure 8 the retroreflector array is illustrated with phantom circle depicting the scan of the laser beam 205 in different positions over the array. The scan direction is indicated by arrow 244, and at the start of a scan to the right side the beam is projected on the array as indicated by circle 245 being at time t=tl. The scan thereafter moves to position as indicated by circle 246 at time t=t2. The beam position at completion of scan to the right is depicted by circle 247 at time t=t3 In the right hand portion of Figure 8 the beam is depicted at commencement of the scan leftwardly at time t=t3 by circle 247. At time t=t4 the scan is depicted by circle 248 and just after completion of the scan to the left, the beam is depicted by circle 249 at time t=t5. Referring to the informational exchange at the various time intervals, at time tl the received return signal from beam 225 is shunted to the integrator 236 of integration means 235. At time t2 the return signal from beam 225 is shunted to integrator 237, while at that time the signal is retained on integrator 26. At time t3 the return signal is shunted to integrator 238 and the signal input to integrator 236 is terminated. At time t4 the return signal is shunted to integrator 239 and the signal to integrator 237 is terminated. The time t5 the return signal is shunted to integrator 238 is terminated. Thereafter the cycle repeats itself. The average signals are passed along lines 240, 241, 242 and 243 respectively to the control computer 212 where they are sorted and stored in individual "sample and hold" means. After completion of a cycle the information averaged during the scan from tl to t3 at laser beam 205 OMPI points to the right hand side of the retroreflector array 215 is substracted from the information averaged during the scan from t3 to t5. This difference constitutes the horizontal error in beam aiming. Similarly, the differ- ence is computed between the signals averaged from t2 to t4, and from t4 to a time t6 at which time the beam scan will be in the same position as depicted by circle 246 at time t2. This difference constitutes the vertical error in beam aiming. Should the differences by zero then the scanning beam 205 is centered about the retroreflector array 215. Should the differences be other than zero their sign, positive or negative, indicates the direction which the beam 205 is off target, namely too far right, left, up, or down, and their magnitude is proportional to the distance the beam 205 is off target. The control computer 212 utilizes these data to develop the servo control signals for transmission along lines 213 and 214 to center the scanning beam 205 about the retroreflector array 215. For instance, if the error signals indicate that the beam is low, the control com¬ puter 212 will output a train of electrical pulses to the vertical servo means 207 that will re-position the steering wedge prisms 208 and 209 of servo means 207 to raise the output beam 205. When a vertical error signal returns to zero the computer 212 will stop outputting pulses to the vertical servo means 207. Figure 9 represents the output signal as a voltage for the relative signals at the different time intervals indicated. As indicated, in various systems employing the earth motion detector there will be a different field deployment for detecting relative motion. With two earth motion detectors positioned the transmitting-receiving network for each could occupy the same structure or optical bench and the output beams 205 will be orientated at some known angle relative to each other. This angle ay be such that the relative angle motions in the planes, vertical and horizontal, to the propagation axis of each system can be measured. Such a bi-directional system permits the differentiation of rotational motion from translational motion of the transmitting system. For instance, with a single detector set up to output the beam 205 in a northerly direction, should an earth motion occur that translates the transmitting/re¬ ceiving network to the east, a shift in the horizontal plane would be recorded. This shift could be explained in several manners: for instance a transmitting-receiving network translation to the east; a retroreflector trans¬ lation to the west; a transmitting/receiving rotation counter clockwise, or a combination of any one of these. With the bi-directional system set up, for instance with one beam orientated north and another east the information obtained will eliminate incorrect conclusions as to the movement which did in fact.occur. * Thus a shift in the horizontal would be recorded by the first detector oriented north, and no horizontal shift would be recorded by the east orientated detector. Since a rotational motion of the transmitting/receiving network requires that horizontal shifts be recorded by both instruments simultaneously this horizontal shift would be eliminated. Thus the motion could be explained as the translation of the transmitting/ receiving or as a translation of the retroreflector array associated with the northerly ori¬ entated detector. In other examples should the angle between the output beams 205 be other than ninety degrees, say 120 degrees, then sufficient information would be recorded to determine that the transmitting/receiving network experi¬ enced an easterly translation. Although the invention has been described with reference to a laser beam of substantially Gaussian profile, there are other embodiments where the form of light may or may not be monochromatic, or other form of electromagnetic radiation. Alternatively, instead of symmetry about the maximum intensity point of the Gaussian profile, the symmetry can be about the points of inflec¬ tion in other Gaussian or non-Gaussian intensity curves having symmetry about the maximum. Such inflection points would be when the curvature of the profile changes from concave upwards to concave downwards. Furthermore, in some applications only partial apodization may be used in the device. Many changes and variations may be made in the method, apparatus and devices providing widely different embodiments in applications for this invention without departing from the scope thereof. All matter contained in the above description as shown in the accompanying drawings shall be interpreted as illustrating but not limiting, the invention being interpreted solely by the scope of the appended claims.

Claims: Claims: 1. Apparatus for utilizing a beam of electromagnetic radiation, said beam having a cross-sectional intensity profile and being substantially symmetrical about the maximum intensity point and points of inflection of said profile comprising a device adapted for location at a transmitting point said device including means for genera¬ ting said electromagnetic radiation beam for propagation from the transmitting point to a relatively remote point, apodizing means for at least partially apodizing at least a portion of the generated beam, means for aligning said apodized beam portion in at least one transverse plane relative to the direction of propagation of said apodized beam from the transmitting point towards said remote point, and means for retrieving from said apodized and aligned beam, after propagation to the remote point, information representative of the physical characteristics at either of, or between, the transmitting point and the remote point. 2. Apparatus as claimed in claim 1 wherein the generated beam is a laser, and the means for generating the beam is a laser source. 3. Apparatus as claimed in claim 2 including means for aligning said apodized beam portion in at least two transverse planes relative to the direction of propaga- tion. 4. Apparatus as claimed in claim 3 wherein the means for obtaining information from the apodized and aligned beam is contained within the device at the gen¬ erating point. 5. Apparatus as claimed in claim 4 including retro¬ reflector means at the remote point, said retroreflector means returning the propagated beam to the device. ? 6. Apparatus as claimed in any one of the above claims wherein apodization is effected by beam scanning means. 7» Apparatus as claimed in claim 6 wherein the scanning means effects a conical scan to the beam. 8. Apparatus as claimed in claim 7 wherein the scanning means includes prism means adapted to deflect the beam, such prism means being adapted to rotate about an axis substantially parallel to the undeflected axis of. the beam and whereby the output from the scanning means traces substantially a conical path at the remote point, such conical path being adapted to provide an at least partly apodized beam at the remote point. 9. Apparatus as claimed in claim 8 wherein the propagated beam maintains a substantially uniform inten- sity over a predetermined beam width. 10.- Apparatus as claimed in claim 7 including servo means, said servo means being adapted to effect beam alignment in the said transverse plane. 11. Apparatus as claimed in claim 10 wherein when the beam is adapted to be propagated from the transmitting point in a substantially horizontal direction, and the servo means acts to align the beam in a substantially horizontal plane and a substantially Vertical plane. 12. Apparatus as claimed in claim 11 wherein the servo means includes wedge prisms, such prisms being spaced apart and being radially aligned relative to each other thereby to effect requisite beam alignment. 13. Apparatus as claimed in claim 5 wherein the retroreflector means includes an array of substantially cubic reflector elements. 14. Apparatus as claimed in claim 13 wherein the cubic reflector elements are arranged in two concentric circles, a lesser number of elements in an inner circle and a larger number in an outer circle. 15. , Apparatus as claimed in claim 5 wherein the reflector means is electrically passive and the device at the transmitting point is electrically active. 16. Apparatus as claimed in claim 7 including beam chopper means and wherein at least a portion of the beam is modulated by said beam chopper means thereby to enhance the detection and retrieval of information from the returned beam. 17. Apparatus as claimed in claim 16 wherein the entire generated beam is modulated by said beam chopper means. 18. Apparatus as claimed in claim 7 including beam splitting means and wherein a portion of the generated beam is split by said splitting means and is retained within the device as a reference beam for comparison with the beam from the remote point. 19.' Apparatus as claimed in claim 18 wherein the reference beam is adapted to be directed by fiber optical means to resolver means, said resolver means being adapted also to receive the beam from the remote point. 20. Apparatus as claimed in claim 19 wherein the reference beam and the beam from the remote point are adapted to be fed to translational means, said transla- tional means acting to translate beam intensity to an electrical parameter and being adapted to be connected with demodulating means, said demodulating means being connected with control means, said control means being adapted to activate said aligning means. 21. Apparatus as claimed in claim 20 wherein the control means is adapted to generate vertical and hori¬ zontal error signals, such signals being adapted to be directed to computation means for controlling the beam generation characteristics and obtaining information from the beam from the remote point. 22. Apparatus as claimed in claim 21 wherein the control means is adapted to receive signals from the apodizing means whereby the control means is adapted to activate the aligning means to respond to said signals from said apodizing means. 23. Apparatus as claimed in claim 22 wherein the retrieved information is interpretted by evaluation means, said evaluation means providing a measure of the trans- missivity parameters between the generating point and remote point. 24. Apparatus as claimed in claim 7 wherein the beam is substantially over-apodized prior to propagation from the transmitting point. 25. Apparatus as claimed in claim 24 including at least two aligning means for aligning the beam in the transverse plane and wherein the generated beam is direc¬ ted through the aligning means for alignment in the transverse plane prior to propagation from the trans- mitting point. 26. Apparatus as claimed in claim 25 wherein on passage through each aligning means, the beam passes through wedge prism means thereby to substantially accurately orientate the direction of the beam on propagation from the trans- mitting point. ' 27. Apparatus as claimed in claim 6 wherein the scanning means includes tagging means adapted to elec- ' tronically tag the beam on passage through the scanning means and whereby said tagging means is adapted to gen- erate a signal, such signal being adapted to be fed back to the aligning means to facilitate alignment of the propagated beam. 28. Apparatus as claimed in claim 5 wherein the propagated beam is reflected from said retroreflector means to receiver means within the device. 29. Apparatus as claimed in claim 28 wherein the receiver means includes photodetector means adapted to translate selected beam characteristics to electrical parameters. 30. Apparatus as claimed in claim 24 wherein the propagated beam is adapted through its conical scanning to sweep over an area at the remote point thereby providing at any one time different intensities to different por¬ tions of the area, and the retrieval means includes discriminating means to distinguish between at least two different intensity signals at different portions of the remote point. 31. Apparatus as claimed in claim 30 wherein the retrieval means includes means to discriminate firstly between intensity signals in a vertical plane, and second¬ ly, intensity signals in a horizontal plane from the remote point. 32. Apparatus as claimed in claim 31 wherein a change in relative position of the device at the transmitting point and the portion of the remote point generates a difference in the signal discrimination to the retrieval means, such difference being an indication of relative ovement between the transmitting point and the remote point. 33. Apparatus as claimed in claim 32 wherein changes in the signals in any one direction are adapted to provide a signal indicative of changes in relative position between different positions of the earth, and thereby furnish a detection of earth movement. 34. Apparatus as claimed in claim 33 wherein the signal from the overapodized beam provides a trough portion of increased intensity sensitivity, and changes in such intensity are employed to obtain a measure of varia¬ tion of beam orientation. 35. A system for detecting relative movement in more than one plane includes locating multiple devices ac- cording to claim 24 at one or more transmitting points, each device being adapted to propagate a beam in a differ¬ ent direction to different selected remote points, the retrieved information from the multiple devices being collected by collection means and being compared by computing means to obtain a detection of multidirectional change in relative positions between the transmitting and remote points. 36. Apparatus for utilizing a laser beam having a substantially Gaussian cross-sectional intensity profile comprising a device adapted for location at a transmitting point said device including laser source means for gener¬ ating said laser beam for propagation from the transmit¬ ting point to a relatively remote point, beam scanning means for conically scanning said beam thereby at least partially apodizing at least a portion of the generated laser beam, means for aligning said apodized beam portion in at least two transverse planes relative to the direc- ?I tion of propagation of said apodized beam from the trans¬ mitting point towards said remote point, and means for retrieving from said apodized and aligned beam, after propagation to the remote point, information representa- tion of the physical characteristics at either of, or between, the transmitting point and the remote point. 37. - Apparatus as claimed in claim 36 wherein the scanning means includes prism means adapted to deflect the beam, such prism means being adapted to rotate about an axis substantially parallel to the undeflected axis of the beam and whereby the output from the scanning means traces substantially a conical path at the remote point, such conical path being adapted to provide an at least partly apodized beam at the remote point. 38. Apparatus as claimed in claim 37 including retro- -reflector means at the remote point, said retroflector means returning the propagated beam to the device, and wherein the means for obtaining information from the apodized and aligned beam is contained within the device at the generating point. 39. Apparatus as claimed in claim 38 wherein when the beam is adapted to be propagated from the transmitting point in a substantially horizontal direction, and including servo means, said servo means being adapted to align the beam in a substantially horizontal plane and a substantially vertical plane. 40. Apparatus as claimed in claim 39 wherein the propagated beam maintains a substantially time-averaged uniform intensity over a predetermined beam width at least at the remote point, and the retrieved information is interpreted by evaluation means, said evaluation means providing a measure of the transmissivity parameters between the generating point and the remote point. 41. Apparatus as claimed in claim 40 including beam splitting means and wherein a portion of the generated beam is split by said splitting means and is retained within the device as a reference beam for comparison with the beam from the remote point. 42. Apparatus as claimed in claim 41 wherein the reference beam and the beam from the remote point are adapted to be fed to translational means, said transla- tional means acting to translate the beam intensity to one or more electrical parameters and being adapted to be connected with demodulating means, said demodulating means being connected with control means, and said control means being adapted to activate said aligning means. 43. Apparatus as claimed in claim 42 wherein the control means is adapted to generate vertical and horizon¬ tal error signals, such signals being adapted to be directed to computation means for controlling the beam generation characteristics and for obtaining information from the beam from the remote point. 44. Apparatus as claimed in claim 43 wherein the control means is adapted to receive a signal from the apodizing means whereby the control means is adapted to activate the aligning means to respond to said signal from said apodizing means. 45. Apparatus as claimed in claim 37 wherein the beam is substantially over-apodized prior to propagation from the transmitting point at least at the remote point, said over-apodized beam providing a trough portion of increased intensity sensitivity, and wherein changes in such intensity being adapted to provide a signal indica¬ tive of changes in relative position between different positions of the earth, thereby to furnish a detection of earth movement. 46. Apparatus as claimed in claim 45 wherein the propagated beam is adapted to sweep over an area at the remote point thereby providing at any one time dffferent intensities to different portions of the area, and the retrieval means includes discriminating means to distin¬ guish between at least two different intensity signals at different portions of the remote point. 47. Apparatus as claimed in claim 46 wherein the retrieval means includes means to discriminate firstly between intensity signals in a vertical plane, and se¬ condly, between intensity signals in a horizontal plane from the remot point. 48. Apparatus as claimed in claim 47 wherein a change in relative position of the device at the transmitting point and the position of the remote point generates a difference in the signal discrimination to the retrieval means, such difference being an indication of relative movement between the transmitting point and the remote point. 49. Transmissometer apparatus for providing a measure of the transmissivity parameters between two points and utilizing a laser beam of a substantially Gaussian cross-sectional intensity profile comprising a device adapted for location at a transmitting point said device including means for generating said laser beam for pro¬ pagation from the transmitting point to a relatively remote point, beam scanning means for conically scanning said beam thereby at least partially apodizing at least a portion of the generated laser beam thereby to maintain a substantially uniform time-averaged intensity over a predetermined beam width at least at the remote point, means for aligning said apodized beam portion in at least two transverse planes relative to the direction of propagation of said apodized beam from the transmitting C PI point towards said remote point, and means for retrieving from said apodized and aligned beam, after propagation to the remote point, information representative of the transmissivity parameters between, the transmitting point and the remote point, including retroreflector means at the remote point, said retroreflector means returning the propagated beam to the device, and wherein the means for obtaining information from the apodized and aligned beam is contained within the device at the generating point. 50. Apparatus for determining changes in the re¬ lative positions between two points, and utilizing a laser beam having a substantially Gaussian cross-sectional intensity profile comprising a device adapted for location at a transmitting point said device including means for generating said laser beam for propagation from the transmitting point to a relatively remote point, beam scanning means for conically scanning, said beam thereby to provide an at least over-apodized beam at said remote point, means for aligning said over-aopdized beam portion in at least two transverse planes relative to the direc¬ tion of propagation of said over-apodized beam from the transmitting point towards said remote point, and means for retrieving from said apodized and aligned beam, after propagation to the remote po ' int, information representa- tive of the relative positions between the transmitting point and the remote point, including retroreflector means at the remote point, said retroreflector means returning the propogated beam to the device, and wherein means for obtaining information from the over-apodized and aligned beam is contained within the device at the gener¬ ating point. 51. A method of utilizing a beam of electromagnetic radiation, said beam having a cross-sectional intensity profile and being substantially symmetrical about the maximum intensity point and points of inflection of said profile comprising generating said electromagnetic radia¬ tion beam in a device adapted for location at a trans¬ mitting point said beam being for propagation from the transmitting point to a relatively remote point, at least partially apodizing at least a portion of the generated beam, aligning said apodized beam portion in at least one transverse plane relative to the direction of propagation of said apodized beam from the transmitting point towards said remote point, and retrieving from said apodized and aligned beam, after propagation to the remote point, information representative of the physical char¬ acteristics at either of, or between, the transmitting point and the remote point. 52. The method as claimed in claim 51 wherein the generated beam is a laser. 53. The method as claimed in claim 52 including aligning said apodized beam portion in at least two transverse planes relative to the direction of propaga¬ tion. 54. The method as claimed in claim 53 wherein obtaining information from the apodized and aligned beam is obtained from within the device at the generating point. 55. The method as claimed in claim 54 including retroreflecting the propagated beam from the remote point to the device. 56. The method as claimed in any one of claims 51 to 55 wherein apodizing is effected by beam scanning. 57. The method as claimed in claim 56 wherein the scanning effects a conical scan to the beam. ^' ' Ϊ : - ' Λ 'rl 58. A method for util iz ing a laser beam having a substantially Guassian cross-sectional intensity profile comprising generating said laser beam in a device adapted for location at a transmitting point for propagation from the transmitting point to a relatively remote point , conically scanning said beam thereby to at least partially apodize at least a portion of the generated laser beam, aligning said apodized beam portion in at least two transverse planes relative to the direction of propagation of said apodized beam from the transmitting point towards said remote point, and retrieving from said apodized and aligned beam, after propagat ion to the remote point , information representative of the physical characteristics at either of, or between, the transmitting point and the remote point. 59. Th e method as cl a imed in c laim 58 includ ing splitting a portion of the generated, beam, and retaining said portion within the device as a reference beam for comparison with the beam from the remote point. 60. Th e method as claimed in cl aim 59 includ ing feeding the reference beam and the beam from the remote point to translational means to provide an output signal, demodulating the signal from said translational means , feeding - the demodulated s ignal to control means , and activating said aligning means with a s ignal from the control means. 61. The method as cl a imed i n c l aim 60 i nclud ing generating vertical and horizontal error signals by the control means , directing such signals to computation means for controlling the beam generation characteristics and obtaining information from the beam from the remote point. OMII 62. The method of providing a measure of the trans¬ missivity parameter between two points and a utilizing laser beam of a substantially Gaussian cross-sectional intensity profile comprising generating said laser beam in a device adapted for location at a transmitting point for propagation from the transmitting point to a relatively remote point, conically scanning said beam to at least partially apodize at least a portion of the generated laser beam thereby to maintain a substantially time-aver- aged uniform intensity over a predetermined beam width at least at the remote point, aligning said apodized beam portion in at least two transverse planes relative to the direction of propagation of said apodized beam from the transmitting point towards said remote point, and retrieving from said apodized and aligned beam, after propagation to the remote point, information representa¬ tive of the transmitting* parameters * between, the trans¬ mitting point and the remote point, r_etroreflecting at the remote point, the propagated beam to the device, and obtaining information from the apodized and aligned beam from within the device at the generating point. 63. A method for determining changes in the relative positions between two points and utilizing a laser beam having a substantially Gaussian cross-sectional intensity profile comprising for generating- said laser beam in a device adapted for location at a transmitting point for propagation from the transmitting point, to a relatively remote point, conically scanning said -beam thereby to provide at least an over-apodized beam at said remote point aligning said over-apodized beam portion in at least two transverse planes relative to the direction of pro¬ pagation of said over-apodized beam from the trans¬ mitting point towards said remote point, and retrieving from said over-apodized and aligned beam, after propaga- tion to the remote point, information representative of the relative positions between the transmitting point and the remote point, including retroflecting at the remote point, the propagated beam to the device, and obtaining information from the over-apodized and aligned beam from within the device at the generating point.

Inventors: HOFFER THOMAS E, LEE PAUL H, SCHORRAN DAVID E, HOFFER, THOMAS, E., LEE, PAUL, H., SCHORRAN, DAVID, E.
Applicants: SOUTHERN CALIFORNIA EDISON CO, SOUTHERN CALIFORNIA EDISON COMPANY
Application year: 1983
Main classification: G01N21
IPC codes: G01B11, G01H9, G01N21, G01S17