Apparatus and method for detecting an information of the displacement of an object.

Abstract: An apparatus for detecting the velocity information of an object (7) comprises a light source (1); optical system for irradiating beam from the light source, which is provided with a first lens or lens group (11) and a second lens or lens group (12) having an identical focal distance which are arranged apart from each other substantially two times such focal distance along the direction of the optical axis, to irradiate the beam onto the measuring object through the first and second lenses or lens group, and the optical system being arranged so as to make the value of sin ϑ/λ substantially constant where ϑ is the incident angle of the beam irradiated onto the measuring object and λ is the wavelength of the beam; and detector (9) for detecting the scattering rays of light from the measuring object irradiated by the above-mentioned optical system to detect the velocity information of the measuring object. With the constituents thus arranged, the apparatus is capable of effectively preventing the deviation of the intersecting position of the beams irradiated on the measuring object to perform a high-precision detection of the velocity information at all times.

Description: BACKGROUND OF THE INVENTION The present invention relates to an apparatus and a method for detecting information of the displacement of an object. The present invention relates in particular to a velocimeter for measuring the velocity of a moving object which may be a fluid without contacting it, and moreover to a Doppler velocimeter for detecting velocity by detecting the frequency shift of light. Traditionally, the laser Doppler velocimeter has been in use as an apparatus for performing a noncontact high-precision measurement of the traveling velocity of a moving object, for example a fluid. The laser Doppler velocimeter is an apparatus for measuring the traveling velocity of the moving object or fluid by the utilization of the effect (Doppler effect) that the frequency of scattering rays of light by the moving object or fluid is shifted in proportion to its traveling velocity when a laser beam is irradiated onto the moving object or fluid. Fig. 1 is a view illustrating an example of a conventional laser Doppler velocimeter. In Fig. 1, the laser light emitted from the laser light source 1 is produced into a parallel beam 3 by the function of the collimator lens 2, and splitted into two beams 5a and 5b by the beam splitter 4. The splitted beams 5a, 5b are reflected by the reflection mirrors 6a and 6b respectively and are irradiated at an incident angle  by the two-beam irradiation onto one and a same position on a moving object or fluid 7 at a traveling velocity V. The scattering lights from the moving object at that time is detected by the photodetector 9 through the condenser lens 8. The frequency of the scattering rays of light by the two beams is proportional to the traveling velocity V and affected by the Doppler shift of + Δf and - Δf, respectively. Now, given the wavelength of the laser light as λ, the Δf can be expressed in an equation (1) given below. Δf = V sin ()/λ The scattering rays of light affected by the Doppler shifts +Δf and -Δf, interfere with each other to result in the variation of light intensity on the light receiving plane of the photodetector 9. Its frequency F is obtainable by an equation (2) given below. F = 2 Δ f = 2V sin ()/λ With the measurement by the equation (2) of the frequency F (hereinafter referred to as Doppler frequency) of the photodetector 9, the traveling velocity V of the moving object 7 can be obtained. In such a laser Doppler velocimeter as in the above example of the conventional art, the Doppler frequency F is inversely proportional to the laser wavelength λ as understandable from the equation (2). Therefore, it is necessary for the laser Doppler velocimeter to use a laser light source capable of emitting a light having stable wavelength. As a laser light source capable of continuous transmission with a stable wavelength, a gas laser such as He - Ne is often employed, but the size of its laser oscillator is large and a high voltage power source is needed. Accordingly, the apparatus becomes large and expensive. On the other hand, the laser diode (or semiconductor laser) employed for a compact disc, video disc, optical fiber communications or the like is very small and easy to drive. However, there is a problem of its temperature dependence. Fig. 2 (quoted from Optical Semiconductor Devices compiled in Mitsubishi Semiconductor Data Book 1987) illustrates an example of the typical temperature dependence of a laser diode. The portion where the wavelength changes continuously is mainly caused by the temperature changes by the refractive index of the active layer of the laser diode, which is 0.05 to 0.06 nm/°C. The portion where the wavelength changes discontinuously is called longitudinal mode hopping, which is 0,2 to 0.3 nm/°C. In order to stabilize the wavelength, a controlling method is usually adopted to maintain the laser diode at a constant temperature. Such method requires the installation of the temperature control members such as heater, radiator, and temperature sensor with small thermal resistance to control the temperature precisely. This makes the laser Doppler velocimeter comparatively large in its size and high in its cost in addition, it is still impossible to eliminate completely the unstableness resulting from the longitudinal mode hopping. With a view to solving the above-mentioned problems, a method for detecting the scattering lights from a moving object or fluid by the use of a photodetector has been proposed in EP-A-391278 (Art. 54(3) EPC prior art document), as a laser Doppler velocimeter, in which the laser light as the light source is incident on a diffraction grating, and the two of the obtainable diffracted lights, which are +n order and -n order (n is 1, 2, and, ... except zero order, are irradiated onto the moving object at an intersecting angle which is the same angle formed by the two beams. Fig. 3 illustrates an example of diffraction wherein a laser light I is incident on a transmission type diffraction grating 10 having a grating pitch d, perpendicularly to the direction in which the grating is arrayed, and the diffraction angle  n is expressed by an equation given below. sin  n = m λ/d where m is the diffraction order (0, 1, 2, and ... ) and λ is the wavelength of light. Here, the light of ±n order other than zero order is expressed by an equation given below. sin  n = ±n λ/d where n is 1, 2, and ... Fig. 4 is a view illustrating the two-beam irradiation of said ±n order light onto the moving object 7 by the use of the mirrors 6a and 6b in such a manner that its incident angle becomes  n . The Doppler frequency F of the photodetector 9 is expressed by an equation given below, obtained from the equations (2) and (3): F - 2Vsin  n /λ = 2nV/d The Doppler frequency F does not depend on the wavelength of the laser light I and is inversely proportional to the grating pitch d of the diffraction grating 10 and is proportional to the traveling velocity V of the object 7. Because the grating pitch d is sufficiently stable, the frequency proportional to only the traveling velocity V of the object 7 is obtainable as the Doppler frequency F. In this respect, when a reflection type diffraction grating is used as the grating 10, same result will be obtained. The pre-characterizing clauses of claims 1 and 5 are based on the apparatus and method known from document EP-A-127244. The optical means of this known apparatus comprises a first lens and a second lens which form an afocal system, i.e. the first and second lenses are positioned such that the image focal plane (back focal plane) of the first lens coincides with object focal plane (front focal plane) of the second lens. The diffraction grating of the optical means is positioned at the front focal plane of the first lens, and the object is positioned at the back focal plane of the second lens. It is an advantage of the known apparatus and method that due to the optical means for irradiating the beam onto the object the luminous energy losses are comparatively low and that the position of the spot which is formed by the beam on the object does not change when the wavelength of the irradiated light changes or fluctuates. This results in a comparatively high S/N ratio of the signal detected by the detecting means and, therefore, contributes to the measurement precision. The installation and the operation of the known apparatus are easier when the working distance, i.e. the distance between the second lens and the object, is large. In order to make the working distance of the known apparatus large, it is necessary that the focal distance of the second lens is made large, whereby the distance between the two lenses is increased and the apparatus as a whole becomes comparatively long. Furthermore, fluctuations or variations of the wavelength λ of the light emitted by the light source means result in variations or fluctuations of the Doppler shift Δf = V sin ()/λ, so that the Doppler shift varies even if the velocity V does not vary. Therefore, the measurement precision is degraded, because fluctuations of the wavelength λ cannot be avoided unless the above mentioned complicated devices are provided to stabilize the wavelength. It is an object of the invention to provide an apparatus the operativity of which is improved by making the working distance longer while at the same time allowing a high-precision detection. Furthermore, it is an object of the invention to provide a correspondingly improved method. These objects are achieved by the apparatus according to claim 1 and by the method according to claim 5. By the specific arrangement according to the invention, a large working distance is achieved without enlarging the focal distance of the second lens and without enlarging the total length of the apparatus. Furthermore, despite the fact that the object is not positioned at the image focal plane of the second lens, the position of the spot generated by the light beam on the object is invariant to wavelength fluctuations. Finally, the above mentioned Doppler shift Δf is not changed by a fluctuation of the wavelength λ because the value of the term (sin /λ) is held constant by the specific optical means according to the invention. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a view showing an example of the conventional laser Doppler velocimeter. Fig. 2 is a graph showing an example of the temperature dependence of the oscillating frequency of a laser diode. Fig. 3 is a view illustrating a diffraction grating. Fig. 4 is a view illustrating a laser Doppler velocimeter using the diffraction grating. Fig. 5 is a view illustrating the principle of the present invention. Fig. 6 is a view illustrating an embodiment according to the present invention, and Figs. 7A, 7B, and 7C are views showing the respective states of beam deviations. DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS The principle of the present invention will be described in conjunction with Fig. 5, in which a reference numeral 10 designates the same diffraction grating as has been described earlier; 11 and 12, lenses having focal distance f; and I 0 , I 1 , I 2 , and I 3 designate optical paths for the measuring beam. The lenses 11 and 12 are arranged apart by a distance 2f, and given the distance between the diffraction grating 10 and the lens 11 as "a", and the distance between the lens 12 and the measuring point M on a measuring object as "b", thereby obtain a + b = 2f. A reference mark D designates the virtual divergence origin and a reference mark "a'" designates the distance from D to the lens 11. The laser light having a wavelength λ is made by a collimator lens and others (not shown) to be parallel beam I 0 and incident on the transmission type diffraction grating 10 perpendicularly to the direction in which the grating 10 is arrayed. Then, the diffraction light I 1 is emitted at a diffraction angle  1 . When the beam I 1 is incident on the convex lens 11 having the focal distance f, a beam I 2 such as shown in Fig. 5 is obtained. When the beam I 2 is incident on another convex lens 12 arranged apart by 2f, the parallel beam I 3 is again obtained, which is irradiated onto the object at an incident angle which is the same as the diffraction angle  1 from the diffraction grating (here, the incident angle is designated by a reference mark  2 ). In this respect, another diffraction light of different reference mark from the diffraction grating 10 intersects said beam at the measuring point M through an axisymmetric optical path, thereby forming the fringe thereon. In Fig. 5, however, the diffraction light of the different reference mark is omitted. The scattering rays of light from the object moving at a velocity V are detected by a detector (not shown), and the optical signals, which contain the Doppler signals expressed by an equation given below in accordance with the equation (2), are detected. F = 2Vsin  2 /λ In this system, if the variation of the focal distance of the lenses caused by the wavelength fluctuation is neglected, the angle of emission (diffraction angle)  1 of the diffracted beam I 1 and the angle of incidence  2 onto the object maintain the relationship of  1 =  2 even when the diffraction angle is varied due to the wavelength fluctuation. Also, provided that the diffracted light is a light of n order, an equation given below can be established. sin  1 = n λ/d Therefore, from the equations (6) and (7), an equation given below is obtained. F = 2Vsin  2 /λ = 2Vsin  1 /λ = 2nV/d From the equation (8), it is apparent that the Doppler frequency which is not affected by the fluctuation of the wavelength is obtainable in this system. Since the term (sin  2 /λ) is a constant value in this system, it is possible to obtain the Doppler frequency which is not affected by the wavelength fluctuation. The influence of the varying angles of the diffraction due to the wavelength fluctuations of the lens group 6a and 6b, which has been neglected earlier, is taken into account. As the wavelength λ changes by the temperatures as shown in Fig. 2, a wavelength fluctuation of approximately 10 nm should be considered at the time of applying the working temperature. Now, for the two wavelengths λ 1 = 780 nm and λ 2 = 790 nm, if the lens material is given to be BK7, the refraction indices are n 1 = 1.51118 and n 2 = 1.51098, respectively, and in terms of the ratio of the focal distances, f 1 /f 2 = (n 1 - 1)/(n 2 - 1) ≃ 1.00039 where f 1 and f 2 are the focal distances for the respective wavelengths. Now, the distance between the lenses is established two times of the focal distance f 2 at λ 2 = 790 nm in Fig. 5. Then, with this arrangement if the wavelength λ 2 = 790 nm is taken into account, the result is sin  1 = sin  2 on condition that a + b = 2f 2 as described earlier. Next, the wavelength λ 1 = 780 nm is taken into account in this arrangement. The  1 and  2 given below are the angles of this wavelength. The focal distance f 1 of the lens changes in accordance with the ratio expressed by the equation (9). Then, if the ray tracing of the beam I 1 is executed, the expression given below is established for the lens 11. Also, the following equation is established: d sin  1 = λ 1 where d is the grating pitch of the diffraction grating. By this equation, the angle  1 is induced. Also, for the lens 12, the position of the beam I 2 on the axis, i.e., D, is (2f 2 + a'). Therefore, 1 2f 2 +a' + 1 b = 1 f 1 (b > 0) On the other hand, the respective distances h a and h b of the incident position of beam on the lenses it and 12 from the optical axis become as follows: h a = a tan  1 h b = h a ( 2f 2 +a' a' ) Therefore, the angle  2 is induced by an equation given below.  2 = tan -1 (h b /b) In terms of the ratio of the Doppler signals: Now, the angles  1 and  2 are obtained by assigning f 2 = 30 mm, a = 10 mm, and d = 1.6 µm, and are assigned to the above-mentioned equation. Then, the result is F 1 = 0.99960 · F 2 and the error is just 0.04 %. Now, if angles the  1 and  2 are obtained by assigning f 2 = 30 mm, a = 30 mm, and d = 1.6 µm, the result is: F 1 = 0.99999977 F 2 This is also negligible as in the above case. In other words, it is safe to consider that the variation of the refraction index caused by the wavelength fluctuation of the lens of approximately 10 nm is substantially negligible. Said discussion is made for the influence of a single-piece lens, but the precision is further improved if a double-piece lens, the chromatic aberration of which has been corrected, is used, for example. In this way, it can be deduced that the Doppler frequency is not affected substantially by the wavelength fluctuation. Also, in this system, the "a + b" does not change substantially even if the  1 varies. As a result, the beam I 3 should always pass through the point M, and there is no substantial deviation generated by the wavelength fluctuation between the two beams intersecting each other at the point of measurement. Furthermore, the beam transmitted through the diffraction grating 10 is deflected by the lens system rather than an element such as diffraction grating which results in a considerable loss of luminous energy, therefore, it is possible to intensify the signal light with ease. Also, it is easy to form a wide area of parallel fringes on the intersecting point, because if parallel light is incident on the diffraction grating 10, the light emitted from the second lens 12 is necessarily parallel light since the distance between the lenses is 2f. Subsequently, using a specific embodiment, the present invention will be described. Fig. 6 is a view schematically showing the principal part of the optical system of an embodiment according to the present invention. In Fig. 6, a reference numeral 101 designates a Doppler velocimeter; 1, a light source means comprising a laser diode, semiconductor, or the like, for example (hereinafter referred to as laser); 2, a collimator lens for producing a beam of parallel light 3 from the beam emitted from the laser 1; and 10, a transmission type diffraction grating which is arranged to diffract light of ± primary order having the grating pitch d. The optical means which comprises the diffraction grating 10 further comprises an optical system comprising two single-piece convex lenses or lens groups 11L and 12L (hereinafter referred to as lens group), having a substantially same focal distance f, which are arranged with a space two times of the focal distance f. Reference numeral 7, designates a moving object or moving fluid (hereinafter referred to as moving object) in motion in the direction indicated by arrow 7a at a traveling velocity V. The distances "a" and "b" satisfy the relationship of "a + b = 2f". A reference numeral 8 designates a condenser lens which converges the scattering rays of light affected by the Doppler shift from the moving object 7 on the detecting surface 9a of an photodetector 9 functioning as detecting means. The surface of the moving object 7 and the detecting surface 9a make a substantially conjugate relationship. A computing means such as an electronic computer (not shown) obtains the traveling velocity V of the moving object 7 using the Doppler signals obtained by the photodetector 9. In the present embodiment, the laser light emitted from the laser 1 (laser diode, wavelength λ = 0.68 µm) is produced by the collimator lens 2 into the parallel beam 3 of approximately 2 mm diameter, and is incident on the transmission type diffraction grating 10 perpendicularly to the direction t in which the grating 10 is arrayed. Then, the diffraction lights 5a and 5b of ± primary order are emitted at a diffraction angle  1 = 12°. When the beams 5a and 5b are incident on the convex lens 11L having the focal distance f, such beams 13a and 13b as shown in Fig. 6 are obtained. When the beams 13a and 13b are incident on another convex lens 12L which is arranged at a position 2f away, the parallel beams 14a and 14b are again obtained, which are irradiated onto the object 7 as the spot diameters of 2 mm  at the same angle  2 as the diffraction angle  1 from aforesaid diffraction grating (i.e.  1 = 2 ). Then, the scattering rays of light from the measuring object 7 are effectively converted by the convex lens 12L and a condenser lens 8 on the light receiving surface 9a of the photodetector 9 to detect the optical signal containing the Doppler signal expressed by the equation (10). Here, if the wavelength λ of the laser light fluctuates the diffraction angle  1 of the diffraction light of a specific order also changes. At this juncture, however, the value of sin  2 /λ is made to be constant by the system formation set forth earlier. The two diffraction beams 14a and 14b are irradiated to intersect each other so that the spots thereof are overlapped on the surface of the moving object 7. In the present embodiment, the focal distances f of the lens group 11L and the lens group 12L in the optical system are substantially equal, and the diffracting grating 10 and the moving object 7 are arranged so as to make the conjugate relationship of equal magnification. At this juncture, the two diffraction lights 14a and 14b on the surface of the moving object 7 form spots of approximately 2 mm diameter. Even when the diffraction angle  1 formed by the diffraction lights ±n order from the diffraction grating 10 is changed into a diffraction angle  1 ' due to the fluctuation of the wavelength λ of the laser light, the diffraction lights of the ±n order incident on the lens group 11L form an image on the surface at the position 11a (a position at which the image height is slightly different from the position corresponding to the diffraction angle  1 and are subsequently diverged and made by the lens group 12L to be the parallel beams to be irradiated onto the surface of the moving object 7 at the angle  1 ', Then, at this time, the two beams are formed to maintain the state in which their spots are overlapped with each other thereon. The condenser lens 8 converges on the detecting surface 9a of the photodetector 9 the scattering rays of light having the frequency affected by the Doppler shift, Δf and - Δf, which are proportional to the traveling velocity V of the moving object 7 and are expressed by the equation (1). At this time, the two scattering rays of light affected by the Doppler shift Δf and - Δf interfere with each other on the detection surface 9a. The photodetector 9 detects the luminous energy based on the luminous intensity of the interference fringe thus produced. In other words, the photodetector 9 detects the Doppler signals which do not depend on the wavelength λ of the laser 1 having the Doppler frequency F, F = 2V/d which is proportional to the traveling velocity V in the equation (8) where n = 1. Then, by the operation of the computing means (not shown), the traveling velocity V is obtained by the equation (10) using the output signals from the photodetector 9. For example, in the system shown in Fig. 4, if the oscillating wavelength of the laser 1 fluctuates, the spots of the two diffracted lights 5a and 5b are becoming deviated, not overlapped with each other on the surface of the moving object 7, for example as shown in Fig. 7B and Fig. 7C. The scattering rays of light detected by the photodetector 9 are those from the area where the two spot diameters 5a and 5b are overlapped. Therefore, if the two spot diameters 5a and 5b are not overlapped but are being deviated, the detecting amount of the scattering rays of light for the detection of the photodetector 9 is decreased. As a result, the S/N ratio of the Doppler signal is lowered, and there is a possibility that the measurement precision for the traveling velocity V is degraded. To counteract this in the present embodiment, each element is arranged as has been described to enable that the two spots of the two light beams 14a and 14b intersect such that they substantially overlap with each other on the surface of the moving object 7 without fail as shown in Fig. 7A. Thus, the S/N ratio of the Doppler signals obtained by the photodetector 9 is maintained in an excellent condition to make a high-precision detection of the traveling velocity V of the moving object 7 possible. Also, since a < b, the distance b becomes comparatively long, whereby the working distance becomes greater. Hence, there is more freedom obtainable in installing the velocimeter. In the present embodiment, although the transmission type diffraction grating is shown, a reflection type diffractions grating may also be employed as well. In the embodiment set forth above, the diffraction light of ± primary order is used, but a diffraction light of the second order or more may also be applied in addition thereto. Further, it may be possible to input the laser light 3 into the diffraction grating 10 at a specific angle, not necessarily the incident angle perpendicular thereto. In this case, two diffraction lights of ±n order diffraction light should be irradiated onto the moving object while the same intersecting angle as the intersecting angle formed by the two diffraction lights of the ±n order diffraction light from the diffraction grating 10 is being maintained. As far as a beam emitted from a same light source is used and provided that at least one of the two diffraction lights irradiated onto the moving object is an n order diffraction light, the other diffraction light can be any order other than the n order, such as 0, n+1, n+2, or the like. It may be possible to obtain the Doppler signals in such as manner that one of the beams, emitted from a same light source to be inputted into light receiving elements, is irradiated onto a moving object as an n order diffraction light, while the other one of them is directly incident on the light receiving elements, not through the moving object, to interfere with the scattering rays of light from the moving object. There is a method of moving the diffraction grating toward the grating arrangement direction in order to apply a bias to the Doppler signal for detecting the velocity in the vicinity of zero and the traveling direction. In this case, it is possible to obtain the same effect if the optical construction is formed in the same way as shown in Fig. 6. Also, it may be possible to employ an acoustic-optical element instead of the method of moving the refraction grating toward the grating arrangement direction. In the descriptions of the embodiment according to the present invention, a single-piece thin lens is represented as the lens to be applied, however, it is possible to use a single-piece thick lens as a matter of course. In such a case, the distance between the principal plane of an image of the front lens 11L and the principal plane of an object of the rear lens 12L should be established to be substantially 2f (two times the focal distance). Similarly, when the lenses 11L and 12L are constructed by lens groups, i.e., equivalent lens system comprising a plurality of lenses, the distance between the principal plane of image of the lens group 11L and the principal plane of object of the lens group 12L should be substantially 2f. The description in the present application hereof, which refers to as being set apart from each other substantially two times of the focal distance, includes those mentioned above as a matter of course. Also, in this case, a reference mark "a" should designate the distance between the principal plane of object of the lens (group) 11L and the diffraction grating 10 and a reference mark "b" should designate the distance between the principal plane of image of the lens (group) 12L and the measuring point.

Claims: An apparatus for detecting an information of the displacement of an object (7), including: light source means (1); optical means (10, 11L, 12L) for irradiating a beam from said light source onto the object (7), which comprises a diffraction grating (10) for diffracting a beam (3) from said light source (1), and a first lens or lens group (11L) and a second lens or lens group (12L), the distance between the first lens or lens group (11L) and the second lens or lens group (12L) being substantially equal to the sum of the focal distance of said first lens or lens group (11L) and of the focal distance of said second lens or lens group (12L) along a direction of the optical axis, wherein at least one beam (5a, 13a, 14a; 5b, 13b, 14b) diffracted by said diffraction grating (10) is irradiated onto said object (7) through said first lens or lens group (11L) and said second lens or lens group (12L); and detecting means (9) for detecting a light from the object (7) to which said beam (5a, 13a, 14a; 5b, 13b, 14b) has been irradiated by means of said optical means (10, 11L, 12L) whereby the information of the displacement of the object (7) is detected by said detecting means; characterized in that said first lens or lens group (11L) and said second lens or lens group (12L) each have the same focal distance (f); in that the sum of the distance (a) from said diffraction grating (10) to said first lens or lens group (11L) and the distance (b) from said object (7) to said second lens or lens group (12L) is made equal to two times said focal distance; and in that the distance (a) from said diffraction grating (10) to said first lens or lens group (11L) is smaller than the distance (b) from the object (7) to said second lens or lens group (12L). An apparatus according to Claim 1, wherein said optical means (10, 11L, 12L) is arranged so as to intersect ±n order diffraction lights (5a, 13a, 14a; 5b, 13b, 14b) from said diffraction grating (10) through said two lenses or lens groups (11L, 12L) on the object (7), where n is an arbitrary natural number. An apparatus according to Claim 1, wherein said detecting means (9) detects scattered rays of light from the object (7) and outputs Doppler frequency signals in response to a velocity of the object (7), the velocity of the object being detected from said Doppler frequency signals. An apparatus according to one of claims 1 to 3, characterized in that the beam (3) from said light source means (1) is incident on said diffraction grating (10) as collimated light. A method for detecting an information of the displacement of an object (7), including the steps of: irradiation of a beam onto the object (7) using a diffraction grating (10) for diffracting a beam (3) and a first lens or lens group (11L) and a second lens or lens group (12L), the distance between the first lens or lens group (11L) and the second lens or lens group (12L) being substantially equal to the sum of the focal distance of said first lens or lens group (11L) and of the focal distance of said second lens or lens group (12L) along a direction of the optical axis; wherein at least one beam (5a, 13a, 14a; 5b, 13b, 14b) diffracted by said diffraction grating (10) is irradiated onto said object (7) through said first lens or lens group (11L) and said second lens or lens group (12L); and detection of a light from the object (7) to which said beam (5a, 13a, 14a; 5b, 13b, 14b) has been irradiated by means of said optical means (10, 16), whereby the information of the displacement of the object (7) is detected by said detection; characterized in that said first lens or lens group (11L) and said second lens or lens group (12L) each have the same focal distance (f); in that the sum of the distance (a) from said diffraction grating (10) to said first lens or lens group (11L) and the distance (b) from said object to said second lens or lens group (12L) is made equal to two times said focal distance and in that the distance (a) from said diffraction grating (10) to said first lens or lens group (11L) is made smaller than the distance (b) from the object (7) to said second lens or lens group (12L). A method according to Claim 5, wherein said irradiation is performed by intersecting ±n order diffraction lights (5a, 13a, 14a; 5b, 13b, 14b) from said diffraction grating (10) through said two lenses or lens groups (11L, 12L) on the object (7), where n is an arbitrary natural number. A method according to Claim 5, wherein said detection is performed by receiving scattered rays of light from the object (7) and outputting Doppler frequency signals in response to the velocity of the object (7), the velocity of the object (7) being detected from said Doppler frequency signals. A method according to one of claims 5 to 7, wherein said beam (3) which is diffracted by said diffraction grating (10) is irradiated onto said diffraction grating (10) in a collimated state.

Inventors: ISHIDA YASUHIKO, KADOWAKI HIDEJIRO, SUGIYAMA HIROSHI, TAKAMIYA MAKOTO, ISHIDA, YASUHIKO, KADOWAKI, HIDEJIRO, SUGIYAMA, HIROSHI, TAKAMIYA, MAKOTO, Ishida, Yasuhiko, c/o Canon Kabushiki Kaisha, Kadowaki, Hidejiro, c/o Canon Kabushiki Kaisha, SUGIYAMA, HIROSHI, C/O CANON KABUSHIKI KAISHA, Takamiya, Makoto, c/o Canon Kabushiki Kaisha
Applicants: CANON KK, CANON KABUSHIKI KAISHA
Application year: 1991
Main classification: G01S17
IPC codes: G01S17