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JP4876659B2 - Optical scanning module and encoder - Google Patents
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JP4876659B2 - Optical scanning module and encoder - Google Patents

Optical scanning module and encoder Download PDF

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JP4876659B2
JP4876659B2 JP2006081915A JP2006081915A JP4876659B2 JP 4876659 B2 JP4876659 B2 JP 4876659B2 JP 2006081915 A JP2006081915 A JP 2006081915A JP 2006081915 A JP2006081915 A JP 2006081915A JP 4876659 B2 JP4876659 B2 JP 4876659B2
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illumination light
scanning module
optical
optical scanning
incident
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JP2007256692A (en
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昭宏 渡邉
亨 今井
進 牧野内
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Nikon Corp
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01DMEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
    • G01D5/00Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable
    • G01D5/26Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light
    • G01D5/32Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light
    • G01D5/34Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells
    • G01D5/36Forming the light into pulses
    • G01D5/38Forming the light into pulses by diffraction gratings
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01DMEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
    • G01D5/00Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable
    • G01D5/26Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light
    • G01D5/32Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light
    • G01D5/34Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells
    • G01D5/347Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells using displacement encoding scales
    • G01D5/34707Scales; Discs, e.g. fixation, fabrication, compensation
    • G01D5/34715Scale reading or illumination devices

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Optical Transform (AREA)
  • Mechanical Optical Scanning Systems (AREA)
  • Mechanical Light Control Or Optical Switches (AREA)

Description

本発明は光走査モジュール及びエンコーダに係り、更に詳しくは、光源からの照明光を走査する光走査モジュール、及び該光走査モジュールを用いたエンコーダに関する。   The present invention relates to an optical scanning module and an encoder, and more particularly to an optical scanning module that scans illumination light from a light source, and an encoder that uses the optical scanning module.

従来より、移動体の位置制御などを行なう際には、光学式エンコーダが比較的多く用いられている。この光学式エンコーダには、種々のタイプが存在するが、近年、移動体の移動方向に沿って周期的なパターンが形成されたスケールと、このスケールを照明する照明光を移動体の移動方向に沿って振動させるプローブと、スケールで反射し、照明光の振動情報と、スケールの位置情報とを含んだ反射光を検出する検出器とを備え、この検出器から検出される検出信号と、照明光を振動させるための駆動信号とに基づいてスケールの位置情報を求めるエンコーダ(スキャン型エンコーダとも呼ばれる)が提案されている(例えば特許文献1参照)。この特許文献1に開示されるようなスキャン型エンコーダは出力信号のS/N比が大きく、スケールの位置検出を高精度で行なうことができる。   Conventionally, a relatively large number of optical encoders have been used to control the position of a moving body. There are various types of optical encoders. In recent years, a scale in which a periodic pattern is formed along the moving direction of the moving body, and illumination light for illuminating the scale in the moving direction of the moving body. A probe that vibrates along, a detector that reflects off the scale and detects reflected light including vibration information of the illumination light and position information of the scale, and a detection signal detected from the detector, and illumination There has been proposed an encoder (also referred to as a scan-type encoder) that obtains scale position information based on a drive signal for vibrating light (see, for example, Patent Document 1). The scan type encoder as disclosed in Patent Document 1 has a large S / N ratio of the output signal, and can detect the position of the scale with high accuracy.

しかしながら、このスキャン型エンコーダでは、スケールを照明する照明光を移動体の移動方向に沿って振動させ、周期的なパターンを必要な範囲で走査する必要がある。そのため、例えばプローブを振動方向に所定ストロークで往復駆動する場合には、そのストロークを十分に確保するために、そのプローブの駆動のための大きなスペースが必要となるとともに、プローブの駆動機構が大型化する傾向があった。   However, in this scan type encoder, it is necessary to oscillate illumination light for illuminating the scale along the moving direction of the moving body and scan a periodic pattern within a necessary range. For this reason, for example, when the probe is reciprocated with a predetermined stroke in the vibration direction, a large space is required for driving the probe in order to sufficiently secure the stroke, and the probe drive mechanism is enlarged. There was a tendency to.

一方、スケールを照明する照明光を移動体の移動方向に沿って走査する手法として、例えば音叉型水晶振動子を用い、この音叉型水晶振動子の振動を利用してスケールに入射させる照明光の出射角を変調させることが考えられる。しかし、この場合、音叉型水晶振動子による照明光の出射角の変調は、外乱の影響を受け易いという欠点を有している。   On the other hand, as a method of scanning the illumination light for illuminating the scale along the moving direction of the moving body, for example, a tuning fork crystal resonator is used, and the illumination light incident on the scale using the vibration of the tuning fork crystal resonator is used. It is conceivable to modulate the emission angle. However, in this case, the modulation of the emission angle of the illumination light by the tuning fork type crystal resonator has a drawback that it is easily affected by disturbance.

米国特許第6,639,686明細書US Pat. No. 6,639,686

本発明は、上述の事情の下になされたもので、第1の観点からすると、照明光を走査する光走査モジュールであって、前記照明光が入射する反射面を有し、所定の周期でその反射面に交差する方向に往復移動しながら前記反射面で前記照明光を反射する反射光学部材と;前記反射光学部材によって反射された前記照明光を入射し、前記反射光学部材の往復移動に応じて、前記交差する方向に対応する計測方向における前記照明光の出射角度を変更する変更部材と;を備える第1の光走査モジュールである。 The present invention has been made under the above circumstances. From a first viewpoint, the present invention is an optical scanning module that scans illumination light, and includes a reflection surface on which the illumination light is incident, and has a predetermined period. reflecting optical member and configured to reflect the illumination light by the reflection surface while reciprocating in a direction intersecting with the reflecting surface; enters the illumination light reflected by the reflecting optical member, the reciprocating movement of the reflecting optical member And a changing member that changes an emission angle of the illumination light in a measurement direction corresponding to the intersecting direction .

これによれば、照明光は、反射光学部材の反射面によって反射され、変更部材に入射する。このとき、反射光学部材は、所定の周期でその反射面に交差する方向に往復移動しているので、その反射光学部材の反射面で反射された照明光は、往復移動しながら変更部材に入射する。この変更部材に入射した照明光は、変更部材によって、反射光学部材(反射面)の往復移動に応じて、前記交差する方向に対応する計測方向におけるその出射角度が変更される。この結果、変更部材から出射される照明光は、所定角度範囲で走査される。すなわち、反射光学部材の反射面で反射された照明光の往復移動が、変更部材によって角度方向の走査に変換され、結果的に大きな走査角、ひいては走査幅を得ることが可能になる。従って、計測方向における反射光学部材のストロークを小さくすることができ、反射光学部材として例えば小型の振動子などを採用することが可能になるとともに、往復移動による誤差を低減し高精度な位置検出が可能となる。 According to this, illumination light is reflected by the reflective surface of a reflective optical member, and injects into a change member. At this time, since the reflecting optical member reciprocates in a direction intersecting the reflecting surface at a predetermined cycle, the illumination light reflected by the reflecting surface of the reflecting optical member enters the changing member while reciprocating. To do. Illumination light incident on the changing member is changed in its emission angle in the measurement direction corresponding to the intersecting direction by the changing member in accordance with the reciprocating movement of the reflecting optical member (reflecting surface). As a result, the illumination light emitted from the changing member is scanned within a predetermined angle range. That is, the reciprocating movement of the illumination light reflected by the reflecting surface of the reflecting optical member is converted into scanning in the angular direction by the changing member, and as a result, a large scanning angle and consequently a scanning width can be obtained. Accordingly, the stroke of the reflecting optical member in the measurement direction can be reduced, and for example, a small vibrator or the like can be adopted as the reflecting optical member, and errors due to reciprocation can be reduced and highly accurate position detection can be performed. It becomes possible.

本発明は第2の観点からすると、照明光源から射出される照明光を走査する光走査モジュールであって、前記照明光源が接続される容器と、前記容器に収容され、前記照明光を計測方向に振動させつつ前記照明光を反射する手段と、前記手段によって反射された前記照明光が入射し、前記照明光の振動に応じて前記計測方向において前記照明光を角度変調する光学素子と、を備える第2の光走査モジュールである。 According to a second aspect of the present invention, there is provided an optical scanning module that scans illumination light emitted from an illumination light source, the container to which the illumination light source is connected, the container being accommodated in the container, and the illumination light being measured in a measuring direction. Means for reflecting the illumination light while vibrating, and an optical element on which the illumination light reflected by the means is incident and angle-modulates the illumination light in the measurement direction according to the vibration of the illumination light. It is the 2nd optical scanning module provided .

これによれば、照明光を振動させつつ照明光を反射する手段と光学素子とを備える構成であるので、計測方向における照明光の振動を小さくすることが可能となり、該振動による誤差を低減できるので高精度な位置検出が可能となる。また、照明光を計測方向に振動させつつ照明光を反射する手段が容器に収容されている。これにより、例えば微小なパーティクルなどの異物の手段への付着が抑えられ、その異物によって照明光が散乱されるなど、外乱の影響を受けるおそれが効果的に抑制される。また、照明光の振動数変化も同時に抑制されるため、振動周期に基づいて照明光を高精度に走査(又は角度変調)することが可能となる According to this, since the configuration includes the optical element and the means for reflecting the illumination light while vibrating the illumination light, it is possible to reduce the vibration of the illumination light in the measurement direction, and to reduce errors due to the vibration. Therefore, highly accurate position detection becomes possible. Further, means for reflecting the illumination light while vibrating the illumination light in the measurement direction is accommodated in the container. Thereby, for example, adhesion of foreign matter such as fine particles to the means is suppressed, and the possibility of being affected by disturbance such as scattering of illumination light by the foreign matter is effectively suppressed. Further, since the frequency of change of the illumination light is suppressed at the same time, it is possible to, based on the vibration periods scanning illumination light with high precision (or angle modulation).

発明の第1、第2の光走査モジュールのいずれかと第1、第2の光走査モジュールのいずれかによって走査された前記照明光が照射されるとともに、前記計測方向を周期方向とする回折格子が形成されたスケールと、前記照明光を受光して出力信号を出力する受光素子と、を備えるエンコーダである。 The first of the present invention, with any of the second optical scanning module, along with the first, the illumination light scanned by one of the second optical scanning module is irradiated, the diffraction of the measurement direction a periodic direction An encoder comprising: a scale on which a grating is formed; and a light receiving element that receives the illumination light and outputs an output signal .

以下、本発明の一実施形態を図1に基づいて説明する。図1には、一実施形態に係るエンコーダ100の構成が概略的に示されている。このエンコーダ100は、回折干渉方式のエンコーダであり、図1における矢印B,B’方向(X軸方向)に移動する不図示の移動体の変位を検出するリニアエンコーダである。   Hereinafter, an embodiment of the present invention will be described with reference to FIG. FIG. 1 schematically shows a configuration of an encoder 100 according to an embodiment. The encoder 100 is a diffraction interference type encoder, and is a linear encoder that detects the displacement of a moving body (not shown) that moves in the directions of arrows B and B ′ (X-axis direction) in FIG. 1.

図1に示されるように、エンコーダ100は、光源ユニット10、光ファイバ12、光走査モジュール20、インデックス回折光学素子(インデックススケール)13、ミラー14A,14B、移動回折光学素子(移動スケール)15、及び受光素子16を備えている。   As shown in FIG. 1, the encoder 100 includes a light source unit 10, an optical fiber 12, an optical scanning module 20, an index diffractive optical element (index scale) 13, mirrors 14A and 14B, a moving diffractive optical element (moving scale) 15, And a light receiving element 16.

前記光源ユニット10は、例えばコヒーレントな光、例えば波長λ(=850nm)のレーザ光を発振する光源を含む。そして、この光源ユニット10から射出される照明光ILは一端が光源ユニット10に接続された光ファイバ12により光走査モジュール20内へ導かれている。   The light source unit 10 includes a light source that oscillates, for example, coherent light, for example, laser light having a wavelength λ (= 850 nm). The illumination light IL emitted from the light source unit 10 is guided into the optical scanning module 20 by an optical fiber 12 having one end connected to the light source unit 10.

前記光走査モジュール20は、ケーシング22、走査振動子(以下、「振動子」と略述する)21及びレンズ24等を備えている。   The optical scanning module 20 includes a casing 22, a scanning vibrator (hereinafter abbreviated as "vibrator") 21, a lens 24, and the like.

前記ケーシング22は、例えばアルミニウム又はステンレス鋼などの金属から成る中空の略直方体状で、例えば窒素ガス又はヘリウムなどの希ガス、あるいはこれらの混合ガスである不活性ガスが充填された気密容器である。このケーシング22の−X側の側壁には、丸孔22cが形成され、該丸孔22cに上記光ファイバ12の他端に設けられたコネクタ12aが、不図示のシール材を介して挿入されている。コネクタ12aの内部に光ファイバ12の他端(射出端)が挿入されており、この射出端から照明光ILが+X方向に向けて射出されるようになっている。   The casing 22 is a hollow, substantially rectangular parallelepiped shape made of a metal such as aluminum or stainless steel, and is an airtight container filled with an inert gas which is a rare gas such as nitrogen gas or helium or a mixed gas thereof. . A round hole 22c is formed in the side wall of the casing 22 on the -X side, and a connector 12a provided at the other end of the optical fiber 12 is inserted into the round hole 22c via a sealing material (not shown). Yes. The other end (exit end) of the optical fiber 12 is inserted into the connector 12a, and the illumination light IL is emitted from the exit end in the + X direction.

前記振動子21は、ケーシング22内部でかつコネクタ12aの+X側に所定距離隔てた位置に、XZ面に直交してかつYZ面及びXY面に対して45°傾斜した状態で配置されている。この振動子21は、例えば長方形板状の水晶から成り、不図示の発振回路及び電源が接続されている。そして、この振動子21は、電源から発振回路に電圧が印加されることにより、矢印A、A’で示されるように、その厚さ方向に所定の振動数かつ所定の振幅で周期的に振動(往復駆動)される。これにより、振動子21へ入射した照明光ILは、振動子21の表面(反射面)21aで−Z方向に反射されるとともに、所定振幅でX軸方向に関して振動(走査)させられる。   The vibrator 21 is disposed at a position within the casing 22 and at a predetermined distance on the + X side of the connector 12a, perpendicular to the XZ plane and inclined by 45 ° with respect to the YZ plane and the XY plane. The vibrator 21 is made of, for example, a rectangular plate crystal, and is connected to an oscillation circuit (not shown) and a power source. The vibrator 21 is periodically vibrated at a predetermined frequency and a predetermined amplitude in the thickness direction as indicated by arrows A and A ′ by applying a voltage from the power source to the oscillation circuit. (Reciprocating drive). Thereby, the illumination light IL incident on the vibrator 21 is reflected in the −Z direction by the surface (reflection surface) 21a of the vibrator 21 and is vibrated (scanned) in the X-axis direction with a predetermined amplitude.

レンズ24は、振動子21の直下のケーシング22の底壁に形成された開口22bに不図示のシール材を介して嵌めこまれている。このレンズ24は、振動子21で反射された照明光ILを入射する凸状の入射面(非球面)と、入射した照明光ILを射出する平面状の出射面とを有する凸平状の屈折光学素子(非球面レンズ)である。このレンズ24は、所定の振幅で周期的に振動(往復駆動)される照明光ILを、レンズ24への入射位置に応じて、換言すれば振動子21の往復移動に応じてX軸方向に、屈折させ、出射角度を変更する。これにより、図中の矢印Cで示されるように、照明光ILが、所定の角速範囲で角度変調され、インデックススケール13の表面に沿ってX軸方向に走査される。   The lens 24 is fitted into an opening 22b formed in the bottom wall of the casing 22 directly below the vibrator 21 via a sealing material (not shown). The lens 24 has a convex refraction having a convex incident surface (aspherical surface) on which the illumination light IL reflected by the vibrator 21 is incident and a planar exit surface on which the incident illumination light IL is emitted. An optical element (aspheric lens). The lens 24 illuminates the illumination light IL periodically oscillated (reciprocatingly driven) with a predetermined amplitude in the X-axis direction according to the incident position on the lens 24, in other words, according to the reciprocating movement of the vibrator 21. Refract and change the exit angle. As a result, as indicated by an arrow C in the figure, the illumination light IL is angle-modulated within a predetermined angular velocity range and scanned along the surface of the index scale 13 in the X-axis direction.

前記インデックススケール13は、光走査モジュール20の下方にXY面に平行に配置された長手方向をX軸方向とする長方形板状のガラス部材から成る。このインデックススケール13の上面には、周期方向をX軸方向とする所定ピッチpの回折格子(透過型の位相格子)が形成されている。このインデックススケール13は、入射した照明光ILに基づいて複数の回折光を発生させる。図1では、それらの回折光のうち、インデックススケール13のX軸方向中央部で発生した±1次回折光が示されている。実線で示される+X側に射出される回折光が+1次回折光であり、点線で示される−X側に射出される回折光が−1次回折光である。なお、これらの回折光の出射角は、インデックススケール13の回折格子のピッチpとレーザ光の波長λとによって決定される。   The index scale 13 is formed of a rectangular plate-like glass member that is disposed below the optical scanning module 20 in parallel with the XY plane and whose longitudinal direction is the X-axis direction. On the upper surface of the index scale 13, a diffraction grating (transmission type phase grating) having a predetermined pitch p with the periodic direction as the X-axis direction is formed. The index scale 13 generates a plurality of diffracted lights based on the incident illumination light IL. FIG. 1 shows ± first-order diffracted light generated from the diffracted light at the central portion of the index scale 13 in the X-axis direction. The diffracted light emitted to the + X side indicated by the solid line is the + 1st order diffracted light, and the diffracted light emitted to the −X side indicated by the dotted line is the −1st order diffracted light. The exit angles of these diffracted lights are determined by the diffraction grating pitch p of the index scale 13 and the laser light wavelength λ.

ミラー14A,14Bは、インデックススケール13の下方で、互いにその反射面が対向するように、かつそれぞれYZ面にほぼ平行に配置されている。インデックススケール13で発生した+1次回折光は、ミラー14Aで反射した後移動スケール15上に入射する。一方、インデックススケール13で発生した−1次回折光は、ミラー14Bで反射した後移動スケール15上に入射する。本実施形態では、インデックススケール13の同一位置から発せられた±1次回折光は、ミラー14A,14Bで反射した後に移動スケール15上の同じ位置で交わる(すなわち、インデックススケール13で分離された±1次回折光は、移動スケール15の同一位置に入射する)ようにインデックススケール13と、ミラー14A,14Bと、移動スケール15の配置面との位置関係が設定されている。   The mirrors 14A and 14B are disposed below the index scale 13 so that the reflecting surfaces thereof face each other and are substantially parallel to the YZ plane. The + 1st order diffracted light generated at the index scale 13 is reflected by the mirror 14A and then enters the moving scale 15. On the other hand, the −1st order diffracted light generated by the index scale 13 is incident on the moving scale 15 after being reflected by the mirror 14B. In the present embodiment, ± 1st-order diffracted light emitted from the same position of the index scale 13 intersects at the same position on the moving scale 15 after being reflected by the mirrors 14A and 14B (that is, ± 1 separated by the index scale 13). The positional relationship among the index scale 13, the mirrors 14A and 14B, and the arrangement surface of the moving scale 15 is set so that the next diffracted light enters the same position of the moving scale 15.

移動スケール15は、不図示の移動体に取り付けられており、その移動体と共に図中の矢印B、B’で示されるように、X軸方向に沿って移動する。この移動スケール15は、ミラー14A,14Bの下方にXY面に平行に配置された長手方向をX軸方向とする長方形板状のガラス部材から成る。この移動スケール15の表面には、周期方向をX軸方向とする回折格子(透過型の位相格子)が形成されている。この回折格子のピッチは、インデックススケール13のインデックス格子のピッチと同じpであり、そのピッチpは、50μm以下、例えば8μm程度である。   The moving scale 15 is attached to a moving body (not shown), and moves with the moving body along the X-axis direction as indicated by arrows B and B 'in the drawing. The moving scale 15 is made of a rectangular plate-shaped glass member having a longitudinal direction arranged in parallel to the XY plane below the mirrors 14A and 14B and having an X-axis direction as a longitudinal direction. On the surface of the moving scale 15, a diffraction grating (transmission type phase grating) whose periodic direction is the X-axis direction is formed. The pitch of this diffraction grating is the same as the pitch of the index grating of the index scale 13, and the pitch p is not more than 50 μm, for example, about 8 μm.

インデックススケール13から発せられた±1次回折光の回折光は、移動スケール15に入射すると、移動スケール15に形成された回折格子の回折作用により再び回折する。移動スケール15で発生する回折光の出射角は、移動スケール15に入射する±1次回折光の入射角、移動スケール15の回折格子のピッチp、レーザ光の波長λによって定まる。   When the diffracted light of ± 1st order diffracted light emitted from the index scale 13 enters the moving scale 15, it is diffracted again by the diffraction action of the diffraction grating formed on the moving scale 15. The outgoing angle of the diffracted light generated by the moving scale 15 is determined by the incident angle of the ± first-order diffracted light incident on the moving scale 15, the pitch p of the diffraction grating of the moving scale 15, and the wavelength λ of the laser light.

移動スケール15からは、インデックススケール13からの+1次回折光の−1次回折光と、インデックススケール13からの−1次回折光の+1次回折光とが、ともに鉛直下方(−Z方向)に射出され、これらの回折光は、互いに干渉した状態で、受光素子16に入射する。受光素子16は、上記の干渉光の干渉強度を示す電気信号を出力するようになっている。   From the moving scale 15, the −1st order diffracted light of the + 1st order diffracted light from the index scale 13 and the + 1st order diffracted light of the −1st order diffracted light from the index scale 13 are both emitted vertically downward (−Z direction). The diffracted lights enter the light receiving element 16 in a state where they interfere with each other. The light receiving element 16 outputs an electric signal indicating the interference intensity of the interference light.

この場合の受光素子16からの出力信号は、振動子21により振動され、さらにレンズ24により角度変調された照明光ILに基づく信号である。従って、受光素子16からの信号を、時間に関するベッセル級数展開を用いて演算処理することで、移動スケール15の位置情報を算出することができる。   The output signal from the light receiving element 16 in this case is a signal based on the illumination light IL that is vibrated by the vibrator 21 and further angle-modulated by the lens 24. Therefore, the position information of the moving scale 15 can be calculated by processing the signal from the light receiving element 16 using the Bessel series expansion with respect to time.

以上説明したように、本実施形態に係る光走査モジュール20によると、光源ユニット10で発せられた照明光ILは、光ファイバ12を介して振動子21の表面(反射面)21aによって反射され、レンズ24に入射する。このとき、振動子21は、その厚さ方向(矢印A、A’で示される方向)に、所定の周期で振動(往復移動)しているので、その表面(反射面)21aで反射された照明光ILは、往復移動しながらレンズ24に入射する。このレンズ24に入射した照明光ILは、レンズ24によって入射位置に応じて(振動子21の往復移動に応じて)屈折されることで、その出射角度が変更される。この結果、レンズ24から出射される照明光ILは、所定角度範囲で走査される。すなわち、振動子21の反射面21aで反射された照明光ILの往復移動が、レンズ24によって角度方向の走査に変換され、結果的に大きな走査角、ひいては走査幅(インデックススケール13上でのX軸方向の走査幅)を得ることが可能になる。従って、本実施形態では、振動子21の振動幅(ストローク)を小さくすることができ、振動子21として小型の振動子を採用することが可能になっている。この小型化により振動子21自体の共振周波数が高くなり、往復駆動時(振動時)の周波数を向上させることができる。   As described above, according to the optical scanning module 20 according to the present embodiment, the illumination light IL emitted from the light source unit 10 is reflected by the surface (reflection surface) 21a of the vibrator 21 through the optical fiber 12, The light enters the lens 24. At this time, the vibrator 21 vibrates (reciprocates) at a predetermined cycle in the thickness direction (directions indicated by arrows A and A ′), and thus is reflected by the surface (reflection surface) 21a. The illumination light IL enters the lens 24 while reciprocating. The illumination light IL incident on the lens 24 is refracted by the lens 24 according to the incident position (according to the reciprocating movement of the vibrator 21), so that the emission angle is changed. As a result, the illumination light IL emitted from the lens 24 is scanned within a predetermined angle range. That is, the reciprocating movement of the illumination light IL reflected by the reflecting surface 21a of the vibrator 21 is converted into scanning in the angular direction by the lens 24. As a result, a large scanning angle and eventually a scanning width (X on the index scale 13) are converted. (Scanning width in the axial direction) can be obtained. Therefore, in the present embodiment, the vibration width (stroke) of the vibrator 21 can be reduced, and a small vibrator can be employed as the vibrator 21. This downsizing increases the resonance frequency of the vibrator 21 itself, and can improve the frequency during reciprocating drive (during vibration).

また、振動子21の振動幅を小さくすることで、振動子21により照明光ILを振動させる際の誤差を小さくすることができるとともに、光走査モジュール20の小型化を図ることが可能となる。   In addition, by reducing the vibration width of the vibrator 21, it is possible to reduce an error when the illumination light IL is vibrated by the vibrator 21 and to reduce the size of the optical scanning module 20.

また、本実施形態に係る光走査モジュール20によると、光源ユニット10から射出された照明光ILは、光源ユニット10に接続された光ファイバ12を介してケーシング22に収容された振動子21に入射し、その振動子21で反射されて走査される。この場合、ケーシング22は、その一部が振動子21によって走査された照明光ILが透過するレンズ24によって構成され、かつ内部が不活性ガスで満たされている。従って、ケーシング22内部の不活性ガス中に存在する振動子21に入射する照明光IL、又は振動子21で反射された照明光ILが、例えば微小なパーティクルなどの異物によって散乱される、あるいは雰囲気の温度変動の影響を受けるなど、外乱の影響を受けるおそれが効果的に抑制されている。また、振動子21が受ける外乱に対する影響、例えば雰囲気の相対湿度変化や異物付着などによる振動子21の振動数変化も同時に抑制されている。従って、振動子21の振動周期に基づいて照明光ILを高精度に走査、ひいてはレンズ24を介して角度変調することが可能となる。また、振動子21を収容するケーシング22の一部は照明光ILが透過するレンズ24によって構成されていることから、部品点数を削減することが可能となる。   Further, according to the optical scanning module 20 according to the present embodiment, the illumination light IL emitted from the light source unit 10 enters the vibrator 21 accommodated in the casing 22 through the optical fiber 12 connected to the light source unit 10. Then, it is reflected by the vibrator 21 and scanned. In this case, the casing 22 is constituted by a lens 24 through which a part of the illumination light IL scanned by the vibrator 21 is transmitted, and the inside is filled with an inert gas. Therefore, the illumination light IL incident on the vibrator 21 existing in the inert gas inside the casing 22 or the illumination light IL reflected by the vibrator 21 is scattered by foreign matters such as minute particles, or the atmosphere. The possibility of being affected by disturbances, such as the effects of temperature fluctuations, is effectively suppressed. Further, the influence on the disturbance received by the vibrator 21, for example, the change in the vibration frequency of the vibrator 21 due to the change in the relative humidity of the atmosphere or the adhesion of foreign matter is also suppressed. Therefore, it is possible to scan the illumination light IL with high accuracy based on the vibration period of the vibrator 21 and to perform angle modulation via the lens 24. In addition, since a part of the casing 22 that houses the vibrator 21 is configured by the lens 24 through which the illumination light IL is transmitted, the number of components can be reduced.

また、本実施形態に係るエンコーダ100は、振動幅を小さくすることで、照明光ILを振動させる際の誤差を小さくし、かつ往復駆動時(振動時)の周波数を向上させることができる小型の振動子21が用いられるとともに、照明光ILの振動中心のドリフトが効果的に抑制され、振動子21の振動周期に基づいて照明光ILを高精度に走査、ひいてはレンズ24を介して角度変調することが可能な光走査モジュール20を備えている。従って、エンコーダ100によると、光走査モジュール20によってインデックススケール13上で照明光ILを走査することで、高精度な照明光ILの走査が可能になり、結果的に移動スケール15の位置を精度良く求めることが可能になる。   In addition, the encoder 100 according to the present embodiment is a small-sized encoder that can reduce the error when vibrating the illumination light IL and reduce the frequency during reciprocating drive (during vibration) by reducing the vibration width. While the vibrator 21 is used, the drift of the vibration center of the illumination light IL is effectively suppressed, and the illumination light IL is scanned with high accuracy based on the vibration cycle of the vibrator 21, and the angle is modulated via the lens 24. An optical scanning module 20 is provided. Therefore, according to the encoder 100, by scanning the illumination light IL on the index scale 13 by the optical scanning module 20, it becomes possible to scan the illumination light IL with high accuracy, and as a result, the position of the moving scale 15 is accurately set. It becomes possible to ask.

なお、上記実施形態では、照明光ILを走査するのに長方形板状の水晶から成る振動子21を用いたが、これに限らず、例えばミラー又はプリズムなどの反射光学素子を用い、該反射光学素子を圧電素子のなどの駆動素子その他の駆動機構を用いて、反射面と交差する方向、例えば厚さ方向に往復移動させても良い。要は、変更部材(上記実施形態ではレンズ24)に入射する照明光を、X軸方向に関して所定ストロークで振動させることが出来れば良い。この意味からすると、振動子21の往復移動(振動)や、反射光学素子の往復移動は、上述の矢印A,A’方向に限らず、反射面に交差する方向であれば良い。   In the above embodiment, the vibrator 21 made of a quartz crystal having a rectangular plate shape is used to scan the illumination light IL. However, the present invention is not limited to this, and a reflective optical element such as a mirror or a prism is used. The element may be reciprocated in a direction intersecting the reflecting surface, for example, in the thickness direction, using a driving element such as a piezoelectric element or other driving mechanism. In short, it is only necessary that the illumination light incident on the changing member (the lens 24 in the above embodiment) can be vibrated with a predetermined stroke in the X-axis direction. In this sense, the reciprocating movement (vibration) of the vibrator 21 and the reciprocating movement of the reflective optical element are not limited to the directions of the arrows A and A ′ described above, and may be any direction that intersects the reflecting surface.

また、上記実施形態では、レンズ24が光走査モジュール20のケーシング22の一部を兼ねている場合について説明したが、これに限らず、例えば図2(A)に示される第1の変形例の光走査モジュール20’のように、インデックススケール13をケーシング22’の底面に形成された開口内に装着しても良い。また、この図2(A)の光走査モジュールの場合、振動子21に代えて、図中の点Oを中心に矢印D,D’で示されるように回動する振動子21’が用いられている。この振動子21’は、例えば音叉型の水晶振動子などで構成することができる。また、この図2(A)のケーシング22’の内部は、前述のように不活性ガスで満たされている。   Moreover, although the said embodiment demonstrated the case where the lens 24 served as a part of casing 22 of the optical scanning module 20, it is not restricted to this, For example, the 1st modification shown by FIG. 2 (A) is shown. Like the optical scanning module 20 ′, the index scale 13 may be mounted in an opening formed on the bottom surface of the casing 22 ′. Further, in the case of the optical scanning module of FIG. 2A, instead of the vibrator 21, a vibrator 21 ′ that rotates around a point O in the figure as indicated by arrows D and D ′ is used. ing. The vibrator 21 ′ can be composed of, for example, a tuning fork type crystal vibrator. Further, the inside of the casing 22 ′ in FIG. 2A is filled with the inert gas as described above.

この図2(A)の光走査モジュール20’を、前述の第1の実施形態の光走査モジュール20に代えて用いる場合には、図2(A)の光走査モジュール20’と、ミラー14A,14B、移動スケール15及び受光素子16とを組み合わせて、エンコーダを構成するようにすれば良い。このようにすることで、上記実施形態と同様に、ケーシング22’内部の不活性ガス中に存在する振動子21’に入射する照明光IL、又は振動子21’で反射された照明光ILが、例えば微小なパーティクルなどの異物によって散乱される、あるいは雰囲気の温度変動の影響を受けるなど、外乱の影響を受けるおそれが効果的に抑制されている。また、走査振動子が受ける外乱に対する影響、例えば雰囲気の相対湿度変化や異物付着などによる振動子の振動数変化も同時に抑制されている。従って、振動子21’の振動周期に基づいて照明光ILを高精度に角度変調することが可能となる。また、ケーシング22’の一部は照明光ILが透過するインデックススケールによって構成されていることから、上記実施形態に比べても部品点数の更なる削減が可能となる。   When the optical scanning module 20 ′ of FIG. 2A is used in place of the optical scanning module 20 of the first embodiment, the optical scanning module 20 ′ of FIG. 14B, the moving scale 15 and the light receiving element 16 may be combined to form an encoder. By doing in this way, similarly to the above embodiment, the illumination light IL incident on the vibrator 21 ′ existing in the inert gas inside the casing 22 ′ or the illumination light IL reflected by the vibrator 21 ′ is obtained. For example, the possibility of being affected by disturbances such as being scattered by foreign matters such as fine particles or being affected by temperature fluctuations of the atmosphere is effectively suppressed. In addition, the influence on the disturbance that the scanning vibrator receives, for example, the change in the vibration frequency of the vibrator due to the change in the relative humidity of the atmosphere or the adhesion of foreign matter is suppressed at the same time. Accordingly, the illumination light IL can be angularly modulated with high accuracy based on the vibration period of the vibrator 21 '. In addition, since a part of the casing 22 ′ is configured by an index scale through which the illumination light IL is transmitted, the number of parts can be further reduced as compared with the above embodiment.

あるいは、例えば図2(B)に示される第2の変形例の光走査モジュール20”のように、平凸レンズの平面上にインデックス格子を形成した光学部材13’をケーシング22”の底面に形成された開口内に隙間無く装着しても良い。また、この図2(B)の光走査モジュール20”の場合、振動子21に代えて上記振動子21’が用いられている。また、この図2(B)のケーシング22”の内部は、前述のように不活性ガスで満たされている。   Alternatively, an optical member 13 ′ having an index grating formed on the plane of a plano-convex lens is formed on the bottom surface of the casing 22 ″, for example, as in the optical scanning module 20 ″ of the second modification shown in FIG. 2B. It may be installed without any gap in the opening. In the case of the optical scanning module 20 ″ of FIG. 2B, the vibrator 21 ′ is used instead of the vibrator 21. Further, the inside of the casing 22 ″ of FIG. As described above, it is filled with an inert gas.

この図2(B)の光走査モジュールを、前述の第1の実施形態の光走査モジュール20に代えて用いる場合には、図2(B)の光走査モジュール20”と、ミラー14A,14B、移動スケール15及び受光素子16とを組み合わせて、エンコーダを構成するようにすれば良い。このようにすることで、上述の第1の変形例と同等の効果を得ることができる。   When the optical scanning module of FIG. 2B is used instead of the optical scanning module 20 of the first embodiment, the optical scanning module 20 ″ of FIG. 2B and the mirrors 14A, 14B, What is necessary is just to comprise an encoder combining the moving scale 15 and the light receiving element 16. By doing in this way, the effect equivalent to the above-mentioned 1st modification can be acquired.

なお、上記実施形態及び各変形例では、光源ユニット10から射出される照明光ILを、光ファイバ12を用いてケーシング(気密容器)の内部に導く場合について説明したが、これに限らず半導体レーザなどの小型の光源をケーシングの内部に設けても良い。この場合、光源が光走査モジュールの一部となる。   In the above-described embodiment and each modified example, the illumination light IL emitted from the light source unit 10 is guided to the inside of the casing (airtight container) using the optical fiber 12, but the present invention is not limited to this. A small light source such as may be provided inside the casing. In this case, the light source becomes a part of the optical scanning module.

また、上記実施形態では、振動子21又は21’が気密容器内に収容された場合について説明したが、振動子が受ける外乱の影響を無視できる、あるいはその影響を別の手段によって取り除くことができるなどの場合には、気密容器を必ずしも設けなくても良い。かかる場合にも、前述の振動子21のように反射面に交差する方向に往復移動する反射光学部材と、レンズ24のような変更部材との組み合わせを用いることで、反射光学部材の反射面で反射された照明光の往復移動が、変更部材によって角度方向の走査に変換され、結果的に大きな走査角、ひいては走査幅を得ることが可能になる。   In the above-described embodiment, the case where the vibrator 21 or 21 ′ is housed in an airtight container has been described. However, the influence of disturbance on the vibrator can be ignored, or the influence can be removed by another means. In such a case, an airtight container is not necessarily provided. Even in such a case, by using a combination of a reflecting optical member that reciprocates in the direction intersecting the reflecting surface like the above-described vibrator 21 and a changing member such as the lens 24, the reflecting surface of the reflecting optical member can be used. The reciprocating movement of the reflected illumination light is converted into angular scanning by the changing member, and as a result, a large scanning angle and thus a scanning width can be obtained.

また、上記実施形態では、インデックススケール13と移動スケール15とが有する回折格子の格子ピッチを同一としたが、これに限らず両者の格子のピッチを相互に異ならせても良い。   In the above embodiment, the grating pitches of the diffraction gratings included in the index scale 13 and the moving scale 15 are the same. However, the present invention is not limited to this, and the pitches of both gratings may be different from each other.

また、上記実施形態では、移動スケール15が移動する場合について説明したが、これに限らず、移動スケールが固定され光学系などの移動スケール15以外の部分が移動する場合につても本発明は好適に適用できる。また、回折干渉方式の透過型の光学式エンコーダの構成は、上記実施形態の構成に限定されないことは勿論である。例えば、上述のミラー14A,14Bに代えて、インデックススケール13からの+1次回折光の−1次回折光と、インデックススケール13からの−1次回折光の+1次回折光とを、移動スケール15上の同一点に入射させる回折光学素子を用いても良い。   In the above-described embodiment, the case where the moving scale 15 moves has been described. However, the present invention is not limited to this, and the present invention is also suitable when the moving scale is fixed and a part other than the moving scale 15 such as an optical system moves. Applicable to. Of course, the configuration of the diffractive interference transmission optical encoder is not limited to the configuration of the above embodiment. For example, instead of the above-described mirrors 14A and 14B, the −1st order diffracted light of the + 1st order diffracted light from the index scale 13 and the + 1st order diffracted light of the −1st order diffracted light from the index scale 13 are the same on the moving scale 15. A diffractive optical element that enters the light source may be used.

なお、上記実施形態では回折干渉方式の透過型の光学式エンコーダに本発明が適用された場合について説明したが、これに限らず、本発明は、いわゆる光ピックアップ方式や、いわゆる影絵方式など、その他の方式のエンコーダであっても照明光をスケール上で走査する場合には好適に適用できる。また、透過型の光学式エンコーダに限らず、反射型の光学式エンコーダにも本発明は適用できる。   In the above embodiment, the case where the present invention is applied to a diffractive interference transmission type optical encoder has been described. However, the present invention is not limited to this, and the present invention is not limited to a so-called optical pickup system, a so-called shadow picture system, and the like. Even an encoder of this type can be suitably applied when scanning illumination light on a scale. Further, the present invention can be applied not only to a transmissive optical encoder but also to a reflective optical encoder.

また、上記実施形態ではレンズ24として凸平状の非球面レンズを用いたが、これに限らず本発明は、平凸レンズ、両凸レンズ、平凹レンズ、両凹レンズ、メニスカスレンズ等を用いる場合にも好適である。   In the above embodiment, a convex aspherical lens is used as the lens 24. However, the present invention is not limited to this, and the present invention is also suitable when a planoconvex lens, a biconvex lens, a planoconcave lens, a biconcave lens, a meniscus lens, or the like is used. It is.

また、上記実施形態ではケーシング22の内部には不活性ガスが充填されている場合について説明したが、これに限らず、ケーシング22の内部は真空状態であってもよい。   Moreover, although the said embodiment demonstrated the case where the inside of the casing 22 was filled with the inert gas, not only this but the inside of the casing 22 may be a vacuum state.

以上説明したように、本発明の光走査モジュールは照明光を走査するのに適しており、本発明のエンコーダは移動体の変位又は位置情報を検出するのに適している。   As described above, the optical scanning module of the present invention is suitable for scanning illumination light, and the encoder of the present invention is suitable for detecting displacement or position information of a moving body.

本発明の一実施形態に係るエンコーダの概略的な構成を示す図である。It is a figure which shows schematic structure of the encoder which concerns on one Embodiment of this invention. 図2(A)は、第1の変形例に係る光走査装置を説明するための図、図2(B)は、第2の変形例に係る光走査装置を説明するための図である。FIG. 2A is a diagram for explaining the optical scanning device according to the first modification, and FIG. 2B is a diagram for explaining the optical scanning device according to the second modification.

符号の説明Explanation of symbols

10…光源ユニット、12…光ファイバ、13…インデックススケール、15…移動スケール、20…光走査モジュール、21…振動子、21a…反射面、22…ケーシング、24…レンズ、100…エンコーダ、IL…照明光。   DESCRIPTION OF SYMBOLS 10 ... Light source unit, 12 ... Optical fiber, 13 ... Index scale, 15 ... Moving scale, 20 ... Optical scanning module, 21 ... Vibrator, 21a ... Reflecting surface, 22 ... Casing, 24 ... Lens, 100 ... Encoder, IL ... Illumination light.

Claims (14)

照明光を走査する光走査モジュールであって、
前記照明光が入射する反射面を有し、所定の周期でその反射面に交差する方向に往復移動しながら前記反射面で前記照明光を反射する反射光学部材と
前記反射光学部材によって反射された前記照明光を入射し、前記反射光学部材の往復移動に応じて、前記交差する方向に対応する計測方向における前記照明光の出射角度を変更する変更部材とを備える光走査モジュール。
An optical scanning module that scans illumination light,
A reflective optical member having a reflective surface on which the illumination light is incident, and reflecting the illumination light on the reflective surface while reciprocating in a direction intersecting the reflective surface at a predetermined period ;
A change member that enters the illumination light reflected by the reflection optical member and changes an emission angle of the illumination light in a measurement direction corresponding to the intersecting direction according to the reciprocation of the reflection optical member ; Optical scanning module provided.
前記反射光学部材は、走査振動子であることを特徴とする請求項1に記載の光走査モジュール。   The optical scanning module according to claim 1, wherein the reflective optical member is a scanning vibrator. 前記反射光学部材は、駆動源によって往復駆動される反射光学素子であることを特徴とする請求項1に記載の光走査モジュール。   The optical scanning module according to claim 1, wherein the reflective optical member is a reflective optical element that is reciprocally driven by a drive source. 前記変更部材は、前記照明光を入射する入射面と、入射した前記照明光を射出する出射面とを有し、前記入射面と前記出射面とのいずれか一方を凸状又は凹状に形成した光学素子を含むことを特徴とする請求項1〜3のいずれか一項に記載の光走査モジュール。   The changing member has an incident surface on which the illumination light is incident and an exit surface on which the incident illumination light is emitted, and either the incident surface or the exit surface is formed in a convex shape or a concave shape. The optical scanning module according to claim 1, further comprising an optical element. 前記光学素子は、屈折光学素子であることを特徴とする請求項4に記載の光走査モジュール。   The optical scanning module according to claim 4, wherein the optical element is a refractive optical element. 前記反射光学部材及び前記変更部材のうち、少なくとも反射光学部材は、その内部が真空状態又は不活性ガスが充填された状態に維持された気密容器内に配置されていることを特徴とする請求項1〜5のいずれか一項に記載の光走査モジュール。   The at least reflective optical member of the reflective optical member and the changing member is disposed in an airtight container whose inside is maintained in a vacuum state or a state filled with an inert gas. The optical scanning module as described in any one of 1-5. 前記変更部材は、前記気密容器の一部を構成することを特徴とする請求項6に記載の光走査モジュール。   The optical scanning module according to claim 6, wherein the changing member constitutes a part of the hermetic container. 前記照明光を射出する照明光源が、前記気密容器に一体的に接続されていることを特徴とする請求項6又は7に記載の光走査モジュール。   8. The optical scanning module according to claim 6, wherein an illumination light source that emits the illumination light is integrally connected to the airtight container. 照明光源から射出される照明光を走査する光走査モジュールであって、
前記照明光源が接続される容器と、
前記容器に収容され、前記照明光を計測方向に振動させつつ前記照明光を反射する手段と、
前記手段によって反射された前記照明光が入射し、前記照明光の振動に応じて前記計測方向において前記照明光を角度変調する光学素子と、を備える光走査モジュール。
An optical scanning module that scans illumination light emitted from an illumination light source,
A container to which the illumination light source is connected;
Means for reflecting the illumination light contained in the container and vibrating the illumination light in a measurement direction;
An optical scanning module comprising: an optical element on which the illumination light reflected by the means is incident and angle-modulates the illumination light in the measurement direction according to vibration of the illumination light.
前記光学素子は、前記照明光の振動によって変更される前記照明光の入射位置に応じて前記照明光の走査角を大きくするように前記照明光を屈折させることを特徴とする請求項9に記載の光走査モジュール。The said optical element refracts the said illumination light so that the scanning angle of the said illumination light may be enlarged according to the incident position of the said illumination light changed by the vibration of the said illumination light. Optical scanning module. 前記容器は、前記照明光が透過する前記光学素子によって該容器の一部が構成され、かつ内部が真空状態又は不活性ガスで満たされている状態であることを特徴とする請求項9又は10に記載の光走査モジュール。11. The container according to claim 9, wherein a part of the container is constituted by the optical element through which the illumination light is transmitted, and the inside is filled with a vacuum state or an inert gas. 2. An optical scanning module according to 1. 記光学素子は、屈折光学素子であることを特徴とする請求項9〜11のいずれか一項に記載の光走査モジュール。 Before Symbol Light optical element includes an optical scanning module according to any one of claims 9 to 11, characterized in that a refractive optical element. 記光学素子は、その一方の面に回折格子が形成された光学素子であることを特徴とする請求項9〜11のいずれか一項に記載の光走査モジュール。 Before Symbol Light optical element includes an optical scanning module according to any one of claims 9 to 11, characterized in that an optical element in which the diffraction grating on one surface thereof are formed. 請求項1〜13のいずれか一項に記載の光走査モジュールと
前記光走査モジュールによって走査された前記照明光が照射されるとともに、前記計測方向を周期方向とする回折格子が形成されたスケールと
前記照明光を受光して出力信号を出力する受光素子と、を備えるエンコーダ。
The optical scanning module according to any one of claims 1 to 13 ,
Together with the illumination light scanned is irradiated by the optical scanning module, and the scale in which the diffraction grating is formed to the measurement direction a periodic direction,
A light receiving element that receives the illumination light and outputs an output signal .
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