JPH0449859U - - Google Patents

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Publication number
JPH0449859U
JPH0449859U JP9263890U JP9263890U JPH0449859U JP H0449859 U JPH0449859 U JP H0449859U JP 9263890 U JP9263890 U JP 9263890U JP 9263890 U JP9263890 U JP 9263890U JP H0449859 U JPH0449859 U JP H0449859U
Authority
JP
Japan
Prior art keywords
mirror
output end
optical fiber
semi
light
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.)
Granted
Application number
JP9263890U
Other languages
Japanese (ja)
Other versions
JP2503175Y2 (en
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 filed Critical
Priority to JP9263890U priority Critical patent/JP2503175Y2/en
Publication of JPH0449859U publication Critical patent/JPH0449859U/ja
Application granted granted Critical
Publication of JP2503175Y2 publication Critical patent/JP2503175Y2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Investigating Or Analyzing Materials By The Use Of Ultrasonic Waves (AREA)

Description

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

第1図は本考案レーザー超音波斜角波発生用光
源の模式図、第2図は偏光分離素子の原理図、第
3図は各出射端の遅延時間の説明図である。第4
図は従来の斜角波発生用光源の模式図である。 1……パルスレーザー、2……パルスレーザー
光、3……No.1半透明鏡、4……No.1偏光分離
素子、5……No.1鏡、6……No.2半透明鏡、7
……No.1レンズ、8……No.1遅延用光フアイバ
ー、9……No.2レンズ、10……No.2偏光分離
素子、11……No.2鏡、12……No.3レンズ、
13……No.2遅延用光フアイバー、14……No.
4レンズ、15……No.3偏光分離素子、16…
…No.3鏡、L……No.1出射端、M……No.2出
射端、N……No.3出射端、O……No.4出射端。
FIG. 1 is a schematic diagram of the light source for generating a laser ultrasonic oblique wave according to the present invention, FIG. 2 is a principle diagram of a polarization separation element, and FIG. 3 is an explanatory diagram of delay times at each output end. Fourth
The figure is a schematic diagram of a conventional light source for generating oblique waves. 1...Pulsed laser, 2...Pulsed laser light, 3...No.1 semi-transparent mirror, 4...No.1 polarization separation element, 5...No.1 mirror, 6...No.2 semi-transparent mirror ,7
...No.1 lens, 8...No.1 delay optical fiber, 9...No.2 lens, 10...No.2 polarization separation element, 11...No.2 mirror, 12...No.3 lens,
13……No.2 Optical fiber for delay, 14……No.
4 lenses, 15... No. 3 polarization separation element, 16...
…No.3 mirror, L…No.1 output end, M…No.2 output end, N…No.3 output end, O…No.4 output end.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] パルスレーザーから発生したレーザー光の光路
上に配置され上記レーザー光を2つに分岐するNo
.1半透明鏡と、上記No.1半透明鏡の透過光路上
に配置され同透過光を垂直偏波と水平偏波に分離
するNo.1偏光分離素子と、上記No.1偏光分離素
子からの垂直偏波をNo.1出射端へ導くNo.1鏡と
、上記No.1偏光分離素子からの水平偏波をNo.2
半透明鏡を介し受け適宜遅延時間を付与しNo.2
偏光分離素子を介しNo.2出射端へ導くNo.1遅延
用光フアイバーと、上記No.1半透明鏡の反射光
をNo.2鏡を介し受け上記遅延時間と異なる適宜
の遅延時間を付与しNo.3出射端へ導くNo.2遅延
用光フアイバーと、上記No.2遅延用光フアイバ
ーの出射端に配置され分離した垂直偏波を上記No
.1遅延用光フアイバーの上流のNo.2半透明鏡へ
導くNo.3偏光分離素子と、上記No.1遅延用光フ
アイバーを通り上記No.2偏光分離素子で反射さ
れる垂直偏波をNo.4出射端へ導くNo.3鏡とを具
えたことを特徴とするレーザー超音波斜角波発生
用光源。
No. placed on the optical path of the laser beam generated from the pulse laser and splitting the laser beam into two.
.1 semi-transparent mirror, a No. 1 polarization separation element that is placed on the transmitted optical path of the No. 1 semi-transparent mirror and separates the transmitted light into vertically polarized waves and horizontally polarized waves, and the above No. 1 polarization separation element. The No. 1 mirror guides the vertically polarized wave from the above to the No. 1 output end, and the horizontally polarized wave from the No. 1 polarization separation element is guided to the No. 2 mirror.
Receive through a semi-transparent mirror and give appropriate delay time No.2
A No. 1 delay optical fiber that guides the light to the No. 2 output end via a polarization separation element, and a No. 2 mirror that receives the reflected light from the No. 1 semitransparent mirror and gives an appropriate delay time different from the above delay time. The No. 2 delay optical fiber leads to the No. 3 output end, and the separated vertically polarized wave is placed at the output end of the No. 2 delay optical fiber and is guided to the No. 3 output end.
A No. 3 polarization splitting element leads the upstream of the delay optical fiber to the No. 2 semi-transparent mirror, and a vertically polarized light that passes through the No. 1 delay optical fiber and is reflected by the No. 2 polarization splitting element. A light source for generating a laser ultrasonic oblique wave, characterized by comprising a No. 3 mirror that leads to a No. 4 emission end.
JP9263890U 1990-09-03 1990-09-03 Laser Light Source for Ultrasonic Oblique Wave Generation Expired - Lifetime JP2503175Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9263890U JP2503175Y2 (en) 1990-09-03 1990-09-03 Laser Light Source for Ultrasonic Oblique Wave Generation

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9263890U JP2503175Y2 (en) 1990-09-03 1990-09-03 Laser Light Source for Ultrasonic Oblique Wave Generation

Publications (2)

Publication Number Publication Date
JPH0449859U true JPH0449859U (en) 1992-04-27
JP2503175Y2 JP2503175Y2 (en) 1996-06-26

Family

ID=31829266

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9263890U Expired - Lifetime JP2503175Y2 (en) 1990-09-03 1990-09-03 Laser Light Source for Ultrasonic Oblique Wave Generation

Country Status (1)

Country Link
JP (1) JP2503175Y2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR100906460B1 (en) * 2007-08-13 2009-07-08 주식회사 브이엠티 Multi-pulse optics with adjustable pulse energy

Also Published As

Publication number Publication date
JP2503175Y2 (en) 1996-06-26

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