JPH0474934A - Measuring apparatus of characteristics of beam - Google Patents

Measuring apparatus of characteristics of beam

Info

Publication number
JPH0474934A
JPH0474934A JP18729690A JP18729690A JPH0474934A JP H0474934 A JPH0474934 A JP H0474934A JP 18729690 A JP18729690 A JP 18729690A JP 18729690 A JP18729690 A JP 18729690A JP H0474934 A JPH0474934 A JP H0474934A
Authority
JP
Japan
Prior art keywords
beam splitter
reflecting member
detector
flat plate
splitter
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP18729690A
Other languages
Japanese (ja)
Inventor
Masayuki Miyahara
正行 宮原
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Canon Inc
Original Assignee
Canon Inc
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Canon Inc filed Critical Canon Inc
Priority to JP18729690A priority Critical patent/JPH0474934A/en
Publication of JPH0474934A publication Critical patent/JPH0474934A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To detect characteristics precisely irrespective of a difference in transmittivity or reflectivity between polarized components by a method wherein both of beam splitters or reflecting members having the same angle of incidence and planes of incidence intersecting perpendicularly each other and being equal in the characteristic of polarization are made to conduct reflection or transmission. CONSTITUTION:Quartz flat plates 2 and 3 are so disposed as to have the same angle of incidence and planes of incidence intersecting perpendicularly each other. Thereby a difference between two components P and S of a reflected light generated by the quartz flat plate 2 is compensated by the surface reflection of the quartz flat plate 3, so as to keep the property of polarization of a laser beam, and the light is made to enter a linear sensor 4. The width of the flux of an incident light is detected by the linear sensor 4. The quartz flat plate 2 and the quartz flat plate 8 are so disposed as to have the same angle of incidence and planes of incidence intersecting perpendicularly each other. The difference between the two components P and S of a light transmitted through the quartz flat plate 2 is compensated by transmitting the light through the quartz flat plate 8, and thereby the property of polarization of the laser beam is kept. A light of surface reflection by the quartz flat plate 8 enters an energy detector 9 and thereby the intensity of the incident light is detected. By this method, characteristics such as the shape of the beam can be measured without being affected by polarization.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明はビームの特性を測定する装置に関するものであ
る。
DETAILED DESCRIPTION OF THE INVENTION [Industrial Field of Application] The present invention relates to a device for measuring beam characteristics.

[従来の技術] 従来の構成を第2図に示す。[Conventional technology] A conventional configuration is shown in FIG.

1はレーザー発振器、2,5、8は石英平面板またはハ
ーフミラー、4、7はリニアセンサ、9はエネルギー検
出器、12はパワー検出器、13は偏光度表示器、14
はパワー表示器、15はビーム形状表示器を示す。
1 is a laser oscillator, 2, 5, and 8 are quartz flat plates or half mirrors, 4 and 7 are linear sensors, 9 is an energy detector, 12 is a power detector, 13 is a polarization degree indicator, 14
1 is a power indicator, and 15 is a beam shape indicator.

従来、レーザービーム特性(ビーム形状、偏光成分、パ
ワー等)を測定する場合、第2図に示すように、レーザ
ービームの光軸上に石英平面板(またはハーフミラー)
2,5、8を順番に設けレーザービームを分割し、各々
リニアセンサ(またはエリアセンサ)4,7、エネルギ
ー検出器9、パワー検出器12に導いて測定していた。
Conventionally, when measuring laser beam characteristics (beam shape, polarization component, power, etc.), a quartz flat plate (or half mirror) was placed on the optical axis of the laser beam, as shown in Figure 2.
2, 5, and 8 are provided in this order to split the laser beam, and guide it to the linear sensors (or area sensors) 4, 7, the energy detector 9, and the power detector 12, respectively, for measurement.

[発明が解決しようとする課題コ しかしながら、偏光成分をもったレーザービームを測定
する場合、上記従来例では石英平面板2,5、8での表
面反射後のレーザービームは水平・垂直両成分の反射率
の違いによりリニアセンサ4,7に入射する際レーザー
ビームはレーザー発振器出射直後の偏光状態を保存して
いない。このためリニアセンサ4,7はビーム形状を正
確に測定できない。
[Problems to be Solved by the Invention] However, when measuring a laser beam with polarized components, in the conventional example described above, the laser beam after surface reflection on the quartz flat plates 2, 5, and 8 has both horizontal and vertical components. Due to the difference in reflectance, the laser beam does not preserve the polarization state immediately after being emitted from the laser oscillator when it enters the linear sensors 4 and 7. For this reason, the linear sensors 4 and 7 cannot accurately measure the beam shape.

本発明は上記従来技術の欠点に鑑みなされたものであっ
て、偏光成分の透過または反射率の相違にかかわらず特
性を精度良く検出可能なビーム特性測定装置の提供を目
的とする。
The present invention has been made in view of the above-mentioned drawbacks of the prior art, and it is an object of the present invention to provide a beam characteristic measuring device capable of accurately detecting characteristics regardless of differences in transmission or reflectance of polarized light components.

[課題を解決するための手段および作用]前記目的を達
成するため、本発明によれば、入射角同一で入射面が互
いに直交する偏光特性の等しいビームスブリッタまたは
反射部材に共に反射あるいは透過させることにより、偏
光特性をもち、かつ偏光特性が変動するレーザービーム
等の特性例えばビーム形状をリアルタイムで測定できる
ようにしたものである。
[Means and effects for solving the problem] In order to achieve the above object, according to the present invention, both beams are reflected or transmitted through a beam splitter or reflecting member having the same incident angle and having the same polarization characteristics and whose incident planes are orthogonal to each other. This makes it possible to measure in real time the characteristics of a laser beam, etc., which has polarization characteristics and whose polarization characteristics vary, such as the beam shape.

ここで入射面とは、入射ビーム(の中心線)と、ビーム
に入射される面の法線とを含む平面の事をいうものとす
る。
The plane of incidence here refers to a plane that includes (the center line of) the incident beam and the normal to the plane onto which the beam is incident.

[夷施例コ 第1図は本発明の実施例の構成を表わす図面である。1
はレーザー発振器、2,3,5,6,8、10は石英平
面板またはハーフミラー等のビームスプリッタでここで
は石英平面板、4、7はリニアセンサ、9,11はエネ
ルギー検出器、13はエネルギーパワー、および偏光度
表示器、15はビーム形状表示器を示す。石英平面板2
と3は入射角が同一で入射平面が直交するように配置さ
れる。これにより石英平面板2で生ずる反射光のP,S
両成分の差異を石英平面板3の表面反射で補償し、レー
ザービームの偏光性を保存してリニアセンサ4に入射す
る。リニアセンサ4により入射光束の幅が検出される。
Embodiment FIG. 1 is a drawing showing the configuration of an embodiment of the present invention. 1
is a laser oscillator; 2, 3, 5, 6, 8, and 10 are beam splitters such as quartz flat plates or half mirrors; 4 and 7 are linear sensors; 9 and 11 are energy detectors; 13 is a quartz flat plate; Energy power and polarization degree indicators; 15 indicates a beam shape indicator; Quartz flat plate 2
and 3 are arranged so that the incident angles are the same and the incident planes are orthogonal. As a result, P and S of the reflected light generated on the quartz flat plate 2
The difference between the two components is compensated for by surface reflection of the quartz flat plate 3, and the laser beam enters the linear sensor 4 while preserving its polarization. A linear sensor 4 detects the width of the incident light beam.

石英平面板2と8は、入射角が同一で入射平面が直交す
るように配置される。石英平面板2で生ずる透過光のp
, s両成分の差異を石英平面板8を透過させることに
より補償し、レーザービームの偏光性を保存する。石英
平面板8による表面反射光はエネルギー検出器9に入射
し、入射光の強度を検出する。上記石英平面板2,3,
8、リニアセンサ4およびエネルギー検出器9からなる
検出系と同じ構成の検出系、(即ち石英平面板5,6,
10、リニアセンサ7およびエネルギー検出器11から
なる検出系)を光軸を中心に90°回転した位置に配置
しく第1図では7の方向が逆になるが効果は同じ)  
90°回転したビーム形状即ちリニアセンサ4で幅を検
出した方向とは垂直な方向の幅、および石英平面板10
による表面反射光の強度を検出する。エネルギー、パワ
ーおよび偏光度表示器13は、エネルギー検出器9と1
1の出力が入りレーザービームのエネルギー、偏光度、
パワーを計算できる。ビーム形状表示器15はリニアセ
ンサ4と7の出力を表示する。
The quartz plane plates 2 and 8 are arranged so that the incident angles are the same and the incident planes are perpendicular to each other. p of the transmitted light generated by the quartz flat plate 2
. The light reflected from the surface of the quartz flat plate 8 enters an energy detector 9, which detects the intensity of the incident light. The above quartz flat plates 2, 3,
8. A detection system having the same configuration as the detection system consisting of the linear sensor 4 and the energy detector 9 (i.e., quartz flat plates 5, 6,
10, a detection system consisting of a linear sensor 7 and an energy detector 11) is placed at a position rotated 90 degrees around the optical axis (in Figure 1, the direction of 7 is reversed, but the effect is the same)
The beam shape rotated by 90 degrees, that is, the width in the direction perpendicular to the direction in which the width is detected by the linear sensor 4, and the quartz flat plate 10.
Detects the intensity of surface reflected light. The energy, power and polarization degree indicator 13 is connected to the energy detectors 9 and 1.
1 output enters, the energy of the laser beam, the degree of polarization,
Power can be calculated. A beam shape display 15 displays the outputs of the linear sensors 4 and 7.

エネルギー検出器9.11の出力から偏光度Pを求める
には次式を計算する。レーザービームの強度を工、水平
および垂直方向の強度を工8、■、とし、エネルギー検
出器9.11の入射光のJliをそれぞれI’、1″、
エネルギー検出器9.11の入射光の水平および垂直方
向の偏光の強度を IH′、 ■’7. IH′、 I
v′各ハーフミラ−でのP、S両成分の透過率を”rp
 、T、 、反射率を訃、Rsとして、 エネルギー検出器9の入射光強度I′は、T’ −IH
’ +L’ =  IN(TSX RP)”IV(TP
 X R5)・・・・・・■ エネルギー検出器11の入射光強度I″は、I’ =I
H’ +TV″−IN (TS X Tp X Tp 
X R,)+ Iv(Tp X 7.x Tsx Rp
)・・・・・・■ 上記■、■の連立方程式を解くことにより1′とI″か
らIHとエヮが求まる。これらを偏光度を求める式 に代入して偏光度を求める。
To find the degree of polarization P from the output of the energy detector 9.11, calculate the following equation. Let the intensity of the laser beam be , and the intensities in the horizontal and vertical directions be 8, .
Let the horizontal and vertical polarization intensities of the incident light of energy detector 9.11 be IH', ■'7. IH', I
v′ The transmittance of both P and S components in each half mirror is “rp
, T, , where the reflectance is Rs, the incident light intensity I' of the energy detector 9 is T' - IH
'+L'=IN(TSX RP)"IV(TP
X R5)...■ The intensity I'' of the incident light on the energy detector 11 is I' = I
H'+TV''-IN (TS X Tp X Tp
X R, )+ Iv(Tp X 7.x Tsx Rp
)...■ By solving the above simultaneous equations ① and ②, IH and EW can be found from 1' and I''. By substituting these into the formula for calculating the degree of polarization, the degree of polarization can be calculated.

エネルギー検出器9.11の出力からエネルギーまたは
パワーIを求めるには前出の連立方程式から求めた工□
とIvを次式に代入して求める。
To find the energy or power I from the output of the energy detector 9.11, use the process found from the simultaneous equations above.
It is obtained by substituting and Iv into the following equation.

I=I  H+1  、 第3図に他の実施例を示す。第1図のエネルギー検出器
9.11の代わりにエリアセンサ16.17を配置する
ことによりレーザービーム内の偏光分布が算出できる。
I=I H+1, FIG. 3 shows another embodiment. By arranging an area sensor 16.17 in place of the energy detector 9.11 in FIG. 1, the polarization distribution within the laser beam can be calculated.

また、エリアセンサ16.17の各画素の出力を積分す
れば偏光度を算出できる。ビームの形状は、リニアセン
サ4.7の代りに、どちらかのりニアセンサの位置にエ
リアセンサを配置して検出しても良い。この場合は1つ
のセンサーでビーム全体の形状が検出できる。またエリ
アセンサをリニアセンサー4の位置に配置した場合、他
の特性を検出する必要がなければ石英平面板2.3は単
なるミラーに置き換えても良い。この場合も2つのミラ
ーは、前述説明のように反射光のp、s両成分の差異を
補償するように配置される。
Furthermore, the degree of polarization can be calculated by integrating the outputs of each pixel of the area sensors 16 and 17. The shape of the beam may be detected by placing an area sensor at the position of either linear sensor instead of the linear sensor 4.7. In this case, one sensor can detect the shape of the entire beam. Further, when the area sensor is placed at the position of the linear sensor 4, the quartz flat plate 2.3 may be replaced with a simple mirror if there is no need to detect other characteristics. In this case as well, the two mirrors are arranged so as to compensate for the difference between the p and s components of the reflected light, as described above.

リニアセンサー4.7の位置で検出されるビーム特性は
、ビーム形状以外、例えば照度分布等であっても良い。
The beam characteristics detected at the position of the linear sensor 4.7 may be other than the beam shape, such as illuminance distribution.

[発明の効果] 以上説明したように、ビームの特性を測定する測定装置
において偏光特性の等しい反射部材またはビームスプリ
ッタを入射角を等しくかつ入射面を直交させるように配
置して共に反射または透過させて検巳器で検出するよう
に配置することにより偏光の影響を受けずにビーム形状
等の特性測定できる。
[Effects of the Invention] As explained above, in a measuring device for measuring beam characteristics, reflective members or beam splitters with equal polarization characteristics are arranged so that the incident angles are equal and the incident surfaces are orthogonal, and both reflect or transmit. By arranging the beam so that it can be detected by a detector, characteristics such as beam shape can be measured without being affected by polarization.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明の実施例に係るレーサービーム測定装置
の構成図、 第2図は従来のレーザービーム測定装置の構成図、 第3図は本発明の別の実施例の構成図である。 1:レーザー発振器、 2.3.5.6.8.10:石英平面板またはハーフミ
ラ− 4,7:リニアセンサ、 9.11:エネルギー検出器、 13:エネルギー、パワーおよび 偏光度表示器、 ビーム形状表示器、 16.17・エリアセンサ。
FIG. 1 is a block diagram of a laser beam measuring device according to an embodiment of the present invention, FIG. 2 is a block diagram of a conventional laser beam measuring device, and FIG. 3 is a block diagram of another embodiment of the present invention. 1: Laser oscillator, 2.3.5.6.8.10: Quartz flat plate or half mirror 4, 7: Linear sensor, 9.11: Energy detector, 13: Energy, power and polarization degree indicator, beam Shape display, 16.17・Area sensor.

Claims (5)

【特許請求の範囲】[Claims] (1)被検査ビームを検出器で受光してビーム特性を検
出する装置において、光路中に第一の反射部材と、該第
一の反射部材と同一な偏光反射特性を有し且つ前記第一
の反射部材とビームの入射角が同一でビームの入射面が
直交するように方向づけた第二の反射部材とを有し、被
検査ビームが前記第一の反射部材と第二の反射部材とを
共に反射した後に前記検出器に入射するように配置した
ことを特徴とするビーム特性測定装置。
(1) A device for detecting beam characteristics by receiving a beam to be inspected by a detector, which includes a first reflecting member in the optical path, having the same polarization reflecting characteristics as the first reflecting member, and having the same polarization reflecting characteristics as the first reflecting member; and a second reflecting member oriented such that the incident angle of the beam is the same and the incident plane of the beam is orthogonal to each other, and the beam to be inspected is directed to the first reflecting member and the second reflecting member. A beam characteristic measuring device characterized in that the beam characteristics are arranged so as to be incident on the detector after being reflected together.
(2)被検査ビームを第一及び第二の検出器で受光して
ビーム特性を検出する装置において、第一のビームスプ
リッタと、該第一のビームスプリッタと同一な偏光反射
特性を有し且つ前記第一のビームスプリッタとビームの
入射角が同一でビームの入射面が直交するように方向づ
けて前記第一のビームスプリッタからの反射ビームの光
路中に配置された第一反射部材と、第一のビームスプリ
ッタと同一な偏光透過特性を有し且つ前記第一のビーム
スプリッタとビームの入射角が同一でビームの入射面が
直交するように方向づけて前記第一のビームスプリッタ
からの透過ビームの光路中に配置された第二のビームス
プリッタと、該第二のビームスプリッタからの透過ビー
ムの光路中に配置された第二の反射部材と、該第二の反
射部材と同一な偏光反射特性を有し且つ前記第二の反射
部材とビームの入射角が同一でビームの入射面が直交す
るように方向づけて前記第二の反射部材からの反射ビー
ムの光路中に配置された第二の反射部材とを有し、被検
査ビームの一部が前記第一のビームスプリッタと第一の
反射部材とを共に反射した後に前記第一検出器に入射し
、被検査ビームの他の一部が前記第一及び第二のビーム
スプリッタを共に透過して前記第二及び第三の反射部材
を共に反射した後に前記第二の検出器に入射するように
配置したことを特徴とするビーム特性測定装置。
(2) In a device that detects beam characteristics by receiving a beam to be inspected by first and second detectors, the first beam splitter has the same polarization reflection characteristics as the first beam splitter; a first reflecting member disposed in the optical path of the reflected beam from the first beam splitter and oriented so that the incident angle of the beam is the same as that of the first beam splitter and the incident plane of the beam is perpendicular; The optical path of the transmitted beam from the first beam splitter is such that the beam splitter has the same polarization transmission characteristics as the first beam splitter, and the incident angle of the beam is the same as that of the first beam splitter, and the beam incidence plane is orthogonal to the first beam splitter. a second beam splitter disposed within the beam splitter, a second reflective member disposed in the optical path of the transmitted beam from the second beam splitter, and a second reflective member having the same polarization reflection characteristics as the second reflective member; and a second reflecting member disposed in the optical path of the reflected beam from the second reflecting member so that the incident angle of the beam is the same as that of the second reflecting member and the beam incidence plane is perpendicular to the second reflecting member. A part of the beam to be inspected is reflected by the first beam splitter and the first reflecting member and then enters the first detector, and another part of the beam to be inspected is reflected by the first beam splitter and the first reflecting member. and a second beam splitter and are reflected by the second and third reflecting members, and then incident on the second detector.
(3)更に前記第二のビームスプリッタまたは前記第二
の反射部材によって、前記第一または第二の検出器で検
出される被検査ビームと分離されたビームを受光してビ
ームの他の特性を検出する検出器を設けたことを特徴と
する特許請求の範囲第2項記載のビーム特性測定装置。
(3) Further, the second beam splitter or the second reflecting member receives the beam separated from the beam to be inspected detected by the first or second detector, and measures other characteristics of the beam. 3. The beam characteristic measuring device according to claim 2, further comprising a detector for detecting the beam characteristics.
(4)被検査ビームを検出器で受光してビーム特性を検
出する装置において、光路中に第一のビームスプリッタ
と、該第一のビームスプリッタと同一な偏光透過または
反射特性を有し且つ前記第一のビームスプリッタとビー
ムの入射角が同一でビームの入射面が直交するように方
向づけた第二のビームスプリッタとを有し、被検査ビー
ムが前記第一及び第二のビームスプリッタを共に透過ま
たは反射した後に前記検出器に入射するように配置した
ことを特徴とするビーム特性測定装置。
(4) A device for detecting beam characteristics by receiving a beam to be inspected by a detector, which includes a first beam splitter in the optical path, and has the same polarized light transmission or reflection characteristics as the first beam splitter, and The first beam splitter and a second beam splitter are oriented such that the incident angle of the beams is the same and the plane of incidence of the beams is orthogonal to each other, and the beam to be inspected passes through both the first and second beam splitters. Alternatively, a beam characteristic measuring device is arranged such that the beam is reflected and then enters the detector.
(5)前記ビーム特性はビーム形状であることを特徴と
する特許請求の範囲第1項または第2項または第4項記
載のビーム特性測定装置。
(5) The beam characteristic measuring device according to claim 1, 2, or 4, wherein the beam characteristic is a beam shape.
JP18729690A 1990-07-17 1990-07-17 Measuring apparatus of characteristics of beam Pending JPH0474934A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP18729690A JPH0474934A (en) 1990-07-17 1990-07-17 Measuring apparatus of characteristics of beam

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18729690A JPH0474934A (en) 1990-07-17 1990-07-17 Measuring apparatus of characteristics of beam

Publications (1)

Publication Number Publication Date
JPH0474934A true JPH0474934A (en) 1992-03-10

Family

ID=16203518

Family Applications (1)

Application Number Title Priority Date Filing Date
JP18729690A Pending JPH0474934A (en) 1990-07-17 1990-07-17 Measuring apparatus of characteristics of beam

Country Status (1)

Country Link
JP (1) JPH0474934A (en)

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US8467057B1 (en) * 2008-09-15 2013-06-18 J.A. Woollam Co., Inc. Ellipsometers and polarimeters comprising polarization state compensating beam directing sample wobble compensating system, and method of use
US9044109B2 (en) 2005-04-04 2015-06-02 Pagter & Partners International B.V. Container for plants that can be filled with water
KR20190022337A (en) * 2017-08-25 2019-03-06 가부시기가이샤 디스코 Laser beam profiler unit and laser machining apparatus
JP2020106285A (en) * 2018-12-26 2020-07-09 パナソニックIpマネジメント株式会社 Light source measurement device

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US9044109B2 (en) 2005-04-04 2015-06-02 Pagter & Partners International B.V. Container for plants that can be filled with water
US8467057B1 (en) * 2008-09-15 2013-06-18 J.A. Woollam Co., Inc. Ellipsometers and polarimeters comprising polarization state compensating beam directing sample wobble compensating system, and method of use
KR20190022337A (en) * 2017-08-25 2019-03-06 가부시기가이샤 디스코 Laser beam profiler unit and laser machining apparatus
CN109454324A (en) * 2017-08-25 2019-03-12 株式会社迪思科 Laser beam analyzer unit and laser processing device
JP2019039830A (en) * 2017-08-25 2019-03-14 株式会社ディスコ Laser beam profiler unit and laser processing device
JP2020106285A (en) * 2018-12-26 2020-07-09 パナソニックIpマネジメント株式会社 Light source measurement device
US11456572B2 (en) 2018-12-26 2022-09-27 Panasonic Intellectual Property Management Co., Ltd. Light source measurement apparatus

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