JP2023133433A5 - - Google Patents
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- 239000000835 fiber Substances 0.000 claims description 51
- 238000006073 displacement reaction Methods 0.000 claims description 28
- 238000001514 detection method Methods 0.000 claims description 20
- 230000010287 polarization Effects 0.000 claims description 14
- 230000002452 interceptive effect Effects 0.000 claims description 6
- 230000003287 optical effect Effects 0.000 claims description 2
- 238000005259 measurement Methods 0.000 claims 1
Description
第1の発明の変位検出装置は、光路長差により生じる複数の干渉強度ピークを持つ、可干渉性の低いマルチモードのレーザ光源と、レーザ光源からの光を集光させるレンズと、レンズで集光され偏波保持ファイバで伝送された光を分岐するビームスプリッタと、分岐された光が照射される回折格子と、回折格子からの回折光を重ね合わせ干渉させた干渉光を受光する受光素子を備え、干渉光の強度変化から、回折格子の変位量を検出する変位検出装置であって、偏波保持ファイバのファイバ長Lを、直交する二つの伝搬モード経由の光による干渉光の強度がピークとなる長さ、(2mn eff L CAV L beat )/λと(2(m+1)n eff L CAV L beat )/λとの間の干渉強度がほぼ0となる長さに設定した(ただし、mは0以上の正の整数、n eff はレーザ光源の共振器の実効屈折率、L CAV はレーザ光源の共振器長、L beat は偏波保持ファイバのビート長、λは光源の波長である)。 The displacement detection device of the first invention includes a multi -mode laser light source with low coherence that has a plurality of interference intensity peaks caused by optical path length differences , a lens that focuses light from the laser light source, and a lens that focuses light from the laser light source. A beam splitter that splits the light that has been transmitted through a polarization-maintaining fiber, a diffraction grating that is irradiated with the split light, and a light receiving element that receives the interference light that is obtained by superimposing and interfering the diffracted light from the diffraction grating. This is a displacement detection device that detects the amount of displacement of a diffraction grating from changes in the intensity of interference light, and the intensity of the interference light due to light via two orthogonal propagation modes is the peak of the fiber length L of the polarization-maintaining fiber. The length was set so that the interference strength between (2mn eff L CAV L beat )/λ and (2(m+1)n eff L CAV L beat )/λ was almost 0 (however, , m is a positive integer greater than or equal to 0, n eff is the effective refractive index of the resonator of the laser light source, L CAV is the resonator length of the laser light source, L beat is the beat length of the polarization maintaining fiber, and λ is the wavelength of the light source. be).
第2の発明の変位検出装置は、レーザ光源からの光を集光させるレンズと、偏波保持ファイバで伝送された光を分岐するビームスプリッタと、分岐された光を反射する被測定面の移動に連動して移動するターゲットミラーと、ターゲットミラーから反射された光を重ね合わせ干渉させた干渉光を受光する受光素子を備え、干渉光の強度変化から、ターゲットミラーの変位量を検出する変位検出装置において、偏波保持ファイバのファイバ長Lを、直交する二つの伝搬モード経由の光による干渉光の強度がピークとなる長さ、(2mn
eff
L
CAV
L
beat
)/λと(2(m+1)n
eff
L
CAV
L
beat
)/λとの間の干渉強度がほぼ0となる長さに設定した(ただし、mは0以上の正の整数、n
eff
はレーザ光源の共振器の実効屈折率、L
CAV
はレーザ光源の共振器長、L
beat
は偏波保持ファイバのビート長、λは光源の波長である)。
第3の発明の変位検出装置は、光を出射する可干渉距離をもつ可干渉性の低い光源と、レーザ光源からの光を集光させるレンズと、レンズで集光され偏波保持ファイバで伝送された光を分岐するビームスプリッタと、分岐された光が照射される回折格子と、回折格子からの回折光を重ね合わせ干渉させた干渉光を受光する受光素子を備え、干渉光の強度変化から、回折格子の変位量を検出する変位検出装置において、偏波保持ファイバは、レーザ光源から出射した光を偏波保持ファイバに入射した場合、偏波保持ファイバの長さLは可干渉距離L
low
と2つの偏波モードの伝搬定数の差から求められるビート長L
beat
の積から光源の波長λを割った長さよりも長く、偏波保持ファイバの直交する二つの伝搬モード経由の光による干渉光の強度がほぼ0となる、レンズで集光された光を伝送する。
第4の発明の変位検出装置は、レーザ光源からの光を集光させるレンズと、レンズで集光され偏波保持ファイバで伝送された光を分岐するビームスプリッタと、分岐された光を反射する被測定面の移動に連動して移動するターゲットミラーと、ターゲットミラーから反射された光を重ね合わせ干渉させた干渉光を受光する受光素子を備え、干渉光の強度変化から、ターゲットミラーの変位量を検出する変位検出装置において、偏波保持ファイバは、レーザ光源から出射した光を偏波保持ファイバに入射した場合、偏波保持ファイバの長さLは前記可干渉距離L
low
と2つの偏波モードの伝搬定数の差から求められるビート長L
beat
の積からレーザ光源の波長λを割った長さよりも長く、偏波保持ファイバの直交する二つの伝搬モード経由の光による干渉光の強度がほぼ0となる、前記レンズで集光された光を伝送する。
The displacement detection device of the second invention includes a lens that focuses light from a laser light source, a beam splitter that splits the light transmitted through a polarization-maintaining fiber, and a movement of a surface to be measured that reflects the split light. Displacement detection is equipped with a target mirror that moves in conjunction with the target mirror, and a light receiving element that receives interference light that overlaps and interferes with the light reflected from the target mirror, and detects the amount of displacement of the target mirror from changes in the intensity of the interference light. In the device, the fiber length L of the polarization-maintaining fiber is defined as the length at which the intensity of interference light due to light via two orthogonal propagation modes reaches its peak, (2mn eff L CAV L beat )/λ and (2(m+ 1) The length was set so that the interference intensity between n eff L CAV L beat )/λ is almost 0 (where m is a positive integer greater than or equal to 0, and n eff is the effective refraction of the resonator of the laser light source. (L CAV is the cavity length of the laser light source, L beat is the beat length of the polarization maintaining fiber, and λ is the wavelength of the light source).
The displacement detection device of the third invention includes a light source with low coherence that has a coherence distance that emits light, a lens that focuses light from the laser light source, and the light that is focused by the lens and transmitted through a polarization-maintaining fiber. It is equipped with a beam splitter that splits the split light, a diffraction grating that is irradiated with the split light, and a light receiving element that receives the interference light obtained by superimposing and interfering the diffracted light from the diffraction grating. In a displacement detection device that detects the amount of displacement of a diffraction grating, when light emitted from a laser light source is input to the polarization-maintaining fiber, the length L of the polarization-maintaining fiber is the coherence length L low The interference light is longer than the length obtained by dividing the light source wavelength λ by the product of the beat length L beat obtained from the difference in the propagation constant of the two polarization modes, and is caused by light that has passed through two orthogonal propagation modes of the polarization-maintaining fiber. It transmits light that is focused by a lens and has an intensity of almost 0.
The displacement detection device of the fourth invention includes a lens that focuses light from a laser light source, a beam splitter that splits the light that was focused by the lens and was transmitted through a polarization-maintaining fiber, and a beam splitter that reflects the split light. Equipped with a target mirror that moves in conjunction with the movement of the surface to be measured, and a light-receiving element that receives interference light that overlaps and interferes with the light reflected from the target mirror, and detects the amount of displacement of the target mirror from changes in the intensity of the interference light. In a displacement detection device that detects a polarization-maintaining fiber, when light emitted from a laser light source is input to the polarization-maintaining fiber, the length L of the polarization-maintaining fiber is equal to the coherence length L low and the two polarizations. It is longer than the length obtained by dividing the wavelength λ of the laser light source from the product of the beat length L beat obtained from the difference in the propagation constants of the modes, and the intensity of the interference light due to the light via the two orthogonal propagation modes of the polarization maintaining fiber is approximately 0, the light focused by the lens is transmitted.
Claims (8)
前記レーザ光源からの光を集光させるレンズと、
前記レンズで集光され偏波保持ファイバで伝送された光を分岐するビームスプリッタと、
前記分岐された光が照射される回折格子と、
前記回折格子からの回折光を重ね合わせ干渉させた干渉光を受光する受光素子を備え、
前記干渉光の強度変化から、前記回折格子の変位量を検出する変位検出装置であって、
前記偏波保持ファイバのファイバ長Lを、直交する二つの伝搬モード経由の光による干渉光の強度がピークとなる長さ、(2mn eff L CAV L beat )/λと(2(m+1)n eff L CAV L beat )/λとの間の干渉強度がほぼ0となる長さに設定した(ただし、mは0以上の正の整数、n eff は前記レーザ光源の共振器の実効屈折率、L CAV は前記レーザ光源の共振器長、L beat は前記偏波保持ファイバのビート長、λは前記光源の波長である)
変位検出装置。 A multi -mode laser light source with low coherence and having multiple interference intensity peaks caused by optical path length differences ;
a lens that focuses light from the laser light source;
a beam splitter that splits the light focused by the lens and transmitted by the polarization maintaining fiber;
a diffraction grating on which the branched light is irradiated;
comprising a light receiving element that receives interference light obtained by superimposing and interfering the diffracted light from the diffraction grating,
A displacement detection device that detects a displacement amount of the diffraction grating from a change in the intensity of the interference light,
The fiber length L of the polarization maintaining fiber is defined as the length at which the intensity of interference light due to light via two orthogonal propagation modes reaches its peak, (2mn eff L CAV L beat )/λ and (2(m+1) The length was set such that the interference intensity between n eff L CAV L beat )/λ is almost 0 (where m is a positive integer greater than or equal to 0, and n eff is the effective refractive index of the resonator of the laser light source. , L CAV is the resonator length of the laser light source, L beat is the beat length of the polarization maintaining fiber, and λ is the wavelength of the light source)
Displacement detection device.
偏波保持ファイバで伝送された光を分岐するビームスプリッタと、
前記分岐された光を反射する被測定面の移動に連動して移動するターゲットミラーと、
前記ターゲットミラーから反射された光を重ね合わせ干渉させた干渉光を受光する受光素子を備え、
前記干渉光の強度変化から、前記ターゲットミラーの変位量を検出する変位検出装置において、
前記偏波保持ファイバのファイバ長Lを、直交する二つの伝搬モード経由の光による干渉光の強度がピークとなる長さ、(2mn eff L CAV L beat )/λと(2(m+1)n eff L CAV L beat )/λとの間の干渉強度がほぼ0となる長さに設定した(ただし、mは0以上の正の整数、n eff は前記レーザ光源の共振器の実効屈折率、L CAV は前記レーザ光源の共振器長、L beat は前記偏波保持ファイバのビート長、λは前記光源の波長である)
変位検出装置。 A lens that focuses the light from the laser light source ,
a beam splitter that splits the light transmitted through the polarization-maintaining fiber;
a target mirror that moves in conjunction with the movement of a surface to be measured that reflects the branched light;
comprising a light receiving element that receives interference light obtained by superimposing and interfering the light reflected from the target mirror,
A displacement detection device that detects a displacement amount of the target mirror from a change in the intensity of the interference light,
The fiber length L of the polarization maintaining fiber is defined as the length at which the intensity of interference light due to light via two orthogonal propagation modes reaches its peak, (2mn eff L CAV L beat )/λ and (2(m+1) The length was set such that the interference intensity between n eff L CAV L beat )/λ is almost 0 (where m is a positive integer greater than or equal to 0, and n eff is the effective refractive index of the resonator of the laser light source. , L CAV is the resonator length of the laser light source, L beat is the beat length of the polarization maintaining fiber, and λ is the wavelength of the light source)
Displacement detection device.
前記光源からの光を集光させるレンズと、a lens for collecting light from the light source;
前記レンズで集光され偏波保持ファイバで伝送された光を分岐するビームスプリッタと、a beam splitter that splits the light collected by the lens and transmitted through the polarization-maintaining fiber;
前記分岐された光が照射される回折格子と、a diffraction grating on which the branched light is irradiated;
前記回折格子からの回折光を重ね合わせ干渉させた干渉光を受光する受光素子を備え、comprising a light receiving element that receives interference light obtained by superimposing and interfering the diffracted light from the diffraction grating,
前記干渉光の強度変化から、前記回折格子の変位量を検出する変位検出装置において、In a displacement detection device that detects a displacement amount of the diffraction grating from a change in the intensity of the interference light,
前記偏波保持ファイバは、前記光源から出射した光を前記偏波保持ファイバに入射した場合、前記偏波保持ファイバの長さLは可干渉距離LIn the polarization-maintaining fiber, when the light emitted from the light source is input to the polarization-maintaining fiber, the length L of the polarization-maintaining fiber is a coherence length L. lowlow と2つの偏波モードの伝搬定数の差から求められるビート長LThe beat length L obtained from the difference between the propagation constants of the two polarization modes and beatbeat の積から前記光源の波長λを割った長さよりも長く、前記偏波保持ファイバの直交する二つの伝搬モード経由の光による干渉光の強度がほぼ0となる、前記レンズで集光された光を伝送するThe light focused by the lens is longer than the product of λ divided by the wavelength λ of the light source, and the intensity of interference light due to light passing through two orthogonal propagation modes of the polarization maintaining fiber is approximately 0. to transmit
変位検出装置。Displacement detection device.
たTa
請求項5に記載の変位検出装置。The displacement detection device according to claim 5.
前記レンズで集光され偏波保持ファイバで伝送された光を分岐するビームスプリッタと、a beam splitter that splits the light collected by the lens and transmitted through the polarization-maintaining fiber;
前記分岐された光を反射する被測定面の移動に連動して移動するターゲットミラーと、a target mirror that moves in conjunction with the movement of a measurement surface that reflects the branched light;
前記ターゲットミラーから反射された光を重ね合わせ干渉させた干渉光を受光する受光素子を備え、comprising a light receiving element that receives interference light obtained by superimposing and interfering the light reflected from the target mirror,
前記干渉光の強度変化から、前記ターゲットミラーの変位量を検出する変位検出装置において、A displacement detection device that detects a displacement amount of the target mirror from a change in the intensity of the interference light,
前記偏波保持ファイバは、前記レーザ光源から出射した光を偏波保持ファイバに入射した場合、前記偏波保持ファイバの長さLは可干渉距離LWhen the light emitted from the laser light source is incident on the polarization-maintaining fiber, the length L of the polarization-maintaining fiber is equal to the coherence length L lowlow と2つの偏波モードの伝搬定数の差から求められるビート長Land the beat length L obtained from the difference in the propagation constants of the two polarization modes. beatbeat の積から前記レーザ光源の波長λを割った長さよりも長く、前記偏波保持ファイバの直交する二つの伝搬モード経由の光による干渉光の強度がほぼ0となる、前記レンズで集光された光を伝送するis longer than the product of the wavelength λ of the laser light source divided by the wavelength λ of the laser light source, and the intensity of the interference light due to the light passing through the two orthogonal propagation modes of the polarization maintaining fiber is approximately 0. transmit light
変位検出装置。Displacement detection device.
請求項7に記載の変位検出装置。The displacement detection device according to claim 7.
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