Patent Document

BACKGROUND OF THE INVENTION 
   1. Field of the Invention 
   The present invention relates to a displacement measuring device with an interference grating, which allows a light beam from a coherent light source to be incident on a scale in a plurality of directions and respective diffracted light beams to interfere with each other, thereby providing a detection signal. The device is suitable for use, among other things, in a linear encoder for measuring the relative displacement between a sensor portion and a scale, a measuring apparatus such as a linear gauge incorporating the linear encoder or a shape measuring apparatus, a measuring device such as for measuring inner and outer diameters, and apparatus for positioning or controlling the speed of a moving stage of a machining tool or an inspection machine. 
   2. Description of the Related Art 
   Optical encoders have become widely available which employ a scale having optical calibration markings formed at a constant pitch to generate cyclic detection signals. Furthermore, as one of the optical encoders of this type having an improved high resolution, a device with an interference grating for detecting displacement has been suggested, in which the scale is provided with calibration markings at a fine pitch using the holography technique so as to use the calibration markings as a diffraction grating to positively cause diffraction, thereby providing a detection signal. 
     FIG. 1  illustrates a device with an interference grating for detecting displacement, which the present applicant has suggested in Japanese Patent Laid-Open Publication No. Hei 1-185415. The displacement measuring device includes a scale  10  formed of a diffraction grating having a pitch p of the same order as a light source wavelength λ, for example, 1 μm or less. The device also includes a sensor portion  20  that has a coherent light source (also hereinafter simply referred to as a light source)  32 , such as a laser diode (LD), for illuminating the diffraction grating with a laser beam  14  of a wavelength λ, a collimator lens  34 , light-receiving elements  22 A,  22 B, and  22 C for optoelectronic conversion of a combined wave of a plurality of light beams yielded by the diffraction grating, polarizers  28 B,  28 C, and a quarter-wave plate  30 . The device is configured to generate a detection signal that varies periodically depending on the relative displacement between the scale  10  and the sensor portion  20 . In this measuring device, the sensor portion  20  includes a half mirror  40  for halving the laser beam  14  from the light source  32 , and a pair of mirrors  42 A and  42 B for allowing the halved laser beams to be incident symmetrically upon the same diffraction point  10 A on the diffraction grating at the same angle of incidence θ. The measuring device is further set to have an angle of incidence θ and an angle of diffraction φ(φ&lt;θ) that differ from each other to such an extent that a zeroth-order light beam of one of the halved incident light beams a and b and a first-order (diffracted) light beam of the other light beam can be separated from each other on the diffraction grating. The separated first-order light beams are reflected on a pair of mirrors  44 A and  44 B to be polarized orthogonally to each other by polarizers  46 A and  46 B, and their respective combined wave is then allowed to be incident on the light-receiving elements  22 A,  22 B, and  22 C through half mirrors  48  and  50 . 
   In this displacement measuring device, a light beam is incident and diffracted on the scale  10  at the angle of incidence θ and the angle of diffraction φ which are different from each other. Additionally, since the device is adapted to measure the relative displacement between the scale  10  and the other portion (the sensor portion  20 ), the device is attached to other apparatus, so that the scale  10  and the sensor portion  20  are mounted on separate members to allow either one of them to be displaced. 
   However, with the arrangement of this optical system, suppose that a pitch angle (the positional relationship of rotational directions on the drawing of  FIG. 2  showing the main portion of the optical system) between the sensor portion  20  and the scale  10  is deviated from the proper position. In this case, the angle of transmission φ from the scale  10  takes on different values for the right and left optical paths. Thus, as shown in  FIG. 3 , the measured values of the output signal level against the pitch angle with the pitch angle being varied teach that the contrast is reduced due to interference, causing the output signal level to be degraded. This raised a problem that a sufficient performance could not be made available. 
   Accordingly, to make full use of the function of a device with an interference grating for measuring displacement which has the optical system shown in  FIG. 1 , it is necessary to adjust the pitch angle, when attached to an apparatus, so as to provide an output signal of the maximum level. Furthermore, an additional adjustment also needs to be made for another direction, thereby requiring adjustments for two directions. This raised another problem that it took time to attach the device to an apparatus. 
   In Japanese Patent Laid-Open Publication No. Hei. 1-185415, a modified example is also described in which the angle of incidence θ is generally equal to the angle of diffraction φ as shown in  FIG. 4 . However, since the zeroth-order light beam and the first-order light beam were inseparably mixed up with each other, good signals could not be obtained. 
   SUMMARY OF THE INVENTION 
   The present invention was developed in view of the aforementioned prior art problems. It is therefore an object of the present invention to make the strength of a detection signal impervious to variations in pitch angle and provide good signals, thus allowing the measuring device to be easily attached to an apparatus and provide improved ease of use for the measuring device. 
   The present invention provides a device with an interference grating for measuring displacement, which allows a light beam from a coherent light source to be incident on a scale in a plurality of directions and respective diffracted light beams to interfere with each other to provide a detection signal. The measuring device solves the aforementioned problems by being configured such that the plurality of light beams are incident on a scale grating at positions spaced farther away from each other than a diameter of the light beams on the scale grating, and an angle of incidence of each light beam on the scale and an angle of transmission of a diffracted light beam of each light beam are generally equal to each other. 
   The measuring device can also be configured such that the plurality of light beams are incident at separated positions on a surface of the scale, thereby being incident on the scale grating at positions spaced farther away from each other than a diameter of the light beams on the scale grating. 
   Alternatively, the measuring device can be configured such that the plurality of light beams are incident at one position on the surface of the scale and then travel a thickness of glass to the scale grating to be thereby incident on a scale grating at positions spaced farther away from each other than a diameter of the light beams on the scale grating. 
   The measuring device may be also provided with an aperture for limiting the diameter of light beams incident on the scale to ensure that the zeroth-order light beam and the first-order diffracted light beams are separated from each other. 
   The measuring device may also include means for intercepting a light beam transmitted from the scale among the plurality of light beams to further ensure that the zeroth-order light beam and the first-order diffracted light beam are separated from each other. 
   According to the present invention, a variation in the attachment angle between the scale and the detector causes only a small degradation in efficiency of detection signals, thereby eliminating alignment work for the device to be attached to an apparatus. The positional relationship between the measuring device and the apparatus can be satisfied only by the machining accuracy specification of a mounting reference surface. This allows for not only facilitating the handling of the optical device but also eliminating the need for a special adjustment mechanism, thereby making it possible to simplify the configuration and thus reduce the number of parts employed. 

   
     BRIEF DESCRIPTION OF THE DRAWINGS 
     The above object, features and advantages of the present invention, as well as other objects and advantages thereof, will become more apparent from the description of the invention which follows, taken in conjunction with the accompanying drawings, wherein like reference characters designate the same or similar parts and wherein: 
       FIG. 1  is an optical path diagram illustrating the configuration of a prior art device with an interference grating for detecting displacement, which the present applicant has suggested in Japanese Patent Laid-Open Publication No. Hei. 1-185415; 
       FIG. 2  is an optical path diagram illustrating the main portion of the optical path of  FIG. 1 ; 
       FIG. 3  is a graph showing the variation characteristic of the output signal strength against the pitch angle in the optical system of  FIG. 1 ; 
       FIG. 4  is an optical path diagram illustrating the configuration of a modified example described by the present applicant in Japanese Patent Laid-Open Publication No. Hei. 1-185415; 
       FIG. 5  is an optical path diagram illustrating a first embodiment of the present invention; 
       FIG. 6  is a graph showing an exemplary variation characteristic of the output signal strength against the pitch angle according to the first embodiment; and 
       FIG. 7  is an optical path diagram illustrating a second embodiment of the present invention. 
   

   DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS 
   Preferred embodiments of the present invention will be explained hereunder. 
     FIG. 5  shows a device with an interference grating for measuring displacement according to a first embodiment of the present invention, similar to the prior art measuring device device shown in  FIG. 4 . The measuring device according to this embodiment includes, for example, a circular aperture  60  provided near the transmitting side of a collimator lens  34  to limit the diameter of a light beam incident on a scale  10 . In this measuring device, incident positions  10 A and  10 B of two light beams on the scale  10  are determined so as to be spaced sufficiently farther away from each other than the diameter of the light beam that is defined by the size of the aperture  60 . 
   Furthermore, a polarizing beam splitter  62  is used instead of the half mirror  40  to change the polarization of the two light beams incident on the scale  10 . Near the transmitting side of the scale  10 , there are also provided polarizing plates  64 A and  64 B which are oriented so as to cut the zeroth-order polarized light beam and transmit the first-order polarized light beam. 
   As illustrated, there are provided lenses  66 A and  66 B and light-receiving elements  68 A and  68 B which are intended to acquire reference signals from the light beams passing through the half mirrors  44 A and  44 B, for example, to provide feedback control to the quantity of light of the LD  32 , respectively. There is also provided a non-polarizing beam splitter (half mirror)  70 . There are also provided a polarizing plate  74 A, a lens  76 A, and a light-receiving element  78 A to acquire an A-phase signal from the light passing through the half mirror  70 . There are also provided a quarter-wave plate  72 B, a polarizing plate  74 B, a lens  76 B, and a light-receiving element  78 B to acquire from the light passing through the half mirror  70  a B-phase signal shifted in phase by 90 degrees with respect to the A-phase signal. 
   In this embodiment, the light beam emitted from the LD  32  is collimated through the collimator lens  34 , limited in light beam diameter by the aperture  60 , and then halved by the polarizing beam splitter  62  into two orthogonal linearly polarized light beams. 
   The light beams are reflected on the mirrors  42 A and  42 B disposed laterally at diametrically opposed positions, respectively, and then incident at an angle θ upon two points  10 A and  10 B spaced farther from each other than the diameter of the light beams on the scale  10 . 
   The ± first-order (diffracted) light beams through the scale  10  are transmitted at an angle of diffraction φ that is equal or generally equal to the angle of incidence θ. 
   The following equation is given here to the relationship among the wavelength λ of the light source, the grating pitch p of the scale being of the same order as the wavelength λ of the light source, for example, 1 μm or less, the angle of incidence θ, and the angle of diffraction φ. That is,
 
Sin θ−sin φ=λ/ p   (1)
 
   When the scale  10  is displaced laterally in the drawing by a displacement d, the phases of the diffracted light beams are each shifted by d/p in the opposite directions. The displacement of the scale converted into the phase difference between the light beams is observed as an interference light intensity shifted by a d/2p cycle through the interference between the two light fluxes. 
   The diffracted light beams pass through the polarizing plates  64 A and  64 B that are oriented to allow their respective linearly polarized light components to transmit therethrough. On the other hand, although a transmitting light beam (the zeroth-order light beam) or a noise component is also transmitted from the scale at the same angle as the angle of incidence θ, the light fluxes of the ± first-order light beams and the zeroth-order light beam do not overlap each other because the light beams are diffracted at the two points spaced farther from each other than the light beam diameter as described above. Additionally, since the polarizing plates  64 A and  64 B are positioned so as to intercept the zeroth-order light beam, most of the light beam does not transmit therethrough. The light beam cannot be completely intercepted here because the light beam incident upon the polarizing plates  64 A and  64 B has not been subjected to a perfect linear polarization due to the degree of polarization of the light source  32  and the polarization function of the polarizing beam splitter  62 . 
   The diffracted light beams having passed through the polarizing plates  64 A and  64 B are each reflected on the half mirrors  44 A and  44 B that are laterally disposed at diametrically opposed positions, and then incident upon the non-polarizing beam splitter  70  disposed at the center. 
   At this stage, the light beams having passed through the half mirrors  44 A and  44 B are incident upon the light-receiving elements  68 A and  68 B via the lenses  66 A and  66 B to be a reference signal. Like the prior art example shown in  FIG. 1  or  FIG. 4 , it is also possible to eliminate any one of the light-receiving elements  68 A and  68 B to employ only the other one. 
   The two linearly polarized light beams incident upon the non-polarizing beam splitter  70  are each halved to be transmitted therethrough and reflected thereon and then directed toward the light-receiving elements  78 A and  78 B through the same optical paths, respectively. 
   In one optical path (the right optical path in the drawing), the polarizing plate  74 A is disposed at an orientation of 45 degrees to interfere the two light beams with each other, thereby allowing the light-receiving element  78 A to convert the position of the scale into an electrical signal strength for output. 
   In the other optical path (the left optical path in the drawing), the quarter-wave plate  72 B is further placed to cause only one of the linearly polarized light beams to lag in phase by 90 degrees and also pass through the polarizing plate  74 B for interference, thereby being converted into an electrical signal having a phase difference of 90 degrees. 
   The two signals having a phase difference of 90 degrees that have been obtained at the light-receiving elements  78 A and  78 B are processed, thereby making it possible to determine the direction of displacement of the scale. 
   At this time, the transmitted light beams (the zeroth-order light beam) from the scale that have not been cut by the polarizing plates  64 A and  64 B are also directed toward the light-receiving elements. However, since these light beams deviate from the optical paths by the diameter of the light beams or more, the light beams would not interfere with the valid light beams, causing no degradation of output signals. This allows for yielding perfect interference between two light fluxes and thereby delivering a substantially ideal sinusoidal signal. 
   The light beams transmitted from the right and left half mirrors  44 A and  44 B are each used to monitor the intensity of the diffracted light beams and thereby control the quantity of light of the LD  32  to provide a constant intensity. 
     FIG. 6  shows the measured values of the signal strength against the pitch angle of the scale according to this embodiment. It can be seen that the drop in strength of the output signal against the pitch angle is reduced when compared with that of  FIG. 3 . 
   The angle of incidence θ is made equal or substantially equal to the angle of diffraction φ as described above. This hardly causes a difference in angle of incidence of the light beams, having passed through the right and left optical paths, on the light-receiving elements even in the presence of a variation in pitch angle. This is because of the following reason. That is, the angles θ and φ are inversely proportional to each other from Equation (1) expressing the relationship between the angle of incidences θ and the angle of diffraction φ. When the angles θ and φ are generally equal to each other, the sum of the angles θ and φ is generally constant. This hardly causes a difference in angle between the light beams having passed through the right and left optical paths, thereby making the signal almost free from a degradation in its strength. 
   Since this embodiment is provided with the circular aperture  60 , the diameter of an incident light beam can be reduced, thereby reducing the amount of separation between the incident positions of the light beams on the scale  10 . The aperture  60  is not limited in shape to a circular one, and can even be eliminated when the diameter of an incident light beam is originally small or the device has an allowable size. 
   Furthermore, in this embodiment, the light beams incident on the scale are differently polarized and the polarizing plates  64 A and  64 B are provided near the transmitting side of the scale to intercept the zeroth-order light beams, thereby making it possible to positively reduce the effects of noise. Depending on the condition, it is also possible to employ a half mirror instead of the polarizing beam splitter  62 , and eliminate the polarizing plates  64 A and  64 B. 
   Now, Referring to  FIG. 7 , a second embodiment of the present invention will be explained below in detail. 
   This embodiment provides a device with an interference grating for measuring displacement, in which a scale grating  12 B is formed on a glass substrate  12 A, and a scale  12  coated with glass  12 C is further provided on the scale grating  12 B. The measuring device employs prisms  80  and  82  instead of the polarizing beam splitter  62  and the non-polarizing beam splitter  70  of the first embodiment. With this arrangement, light beams are incident at a point on a surface  12 S of the scale  12  (i.e., the surface of the glass  12 C) but are separated farther than the diameter of the light beams after having traveled a thickness t of the glass  12 C to be incident on the scale grating  12 B. 
   The other features of this embodiment are the same as those of the first embodiment, and the same components are designated with the same reference symbols and will not be further detailed. 
   According to this embodiment, a plurality of light beams are incident at one point on the surface of the glass  12 C, thereby hardly causing errors due to undulations of the surface of the glass (on the side of incidence). 
   Although certain preferred embodiments have been shown and described, it should be understood that many changes and modifications may be made therein without departing from the scope of the appended claims.

Technology Category: 3