ES2059530T3 - Resonador de celula de raman intracavitario. - Google Patents
Resonador de celula de raman intracavitario.Info
- Publication number
- ES2059530T3 ES2059530T3 ES88309033T ES88309033T ES2059530T3 ES 2059530 T3 ES2059530 T3 ES 2059530T3 ES 88309033 T ES88309033 T ES 88309033T ES 88309033 T ES88309033 T ES 88309033T ES 2059530 T3 ES2059530 T3 ES 2059530T3
- Authority
- ES
- Spain
- Prior art keywords
- cavity
- raman
- laser
- photons
- mirror
- 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.)
- Expired - Lifetime
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/10—Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
- H01S3/106—Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating by controlling devices placed within the cavity
- H01S3/108—Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating by controlling devices placed within the cavity using non-linear optical devices, e.g. exhibiting Brillouin or Raman scattering
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/10—Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
- H01S3/106—Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating by controlling devices placed within the cavity
- H01S3/108—Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating by controlling devices placed within the cavity using non-linear optical devices, e.g. exhibiting Brillouin or Raman scattering
- H01S3/1086—Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating by controlling devices placed within the cavity using non-linear optical devices, e.g. exhibiting Brillouin or Raman scattering using scattering effects, e.g. Raman or Brillouin effect
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Nonlinear Science (AREA)
- Engineering & Computer Science (AREA)
- Plasma & Fusion (AREA)
- Optics & Photonics (AREA)
- Lasers (AREA)
- Optical Communication System (AREA)
- Investigating, Analyzing Materials By Fluorescence Or Luminescence (AREA)
- Light Guides In General And Applications Therefor (AREA)
Abstract
UNA CAVIDAD QUE ES RESONANTE EN UNA FRECUENCIA DE BOMBEO LASER QUE SE DEFINE MEDIANTE UNA SUPERFICIE REFLECTIVA (92) Y UN ESPEJO (110). UN MEDIO RAMAN (106) ESTA CONTENIDO DENTRO DE LA CAVIDAD, ASI COMO UN LASER (90). UN Q-INTERRUPTOR (94), CUANDO NO SE DETERIOR EL Q DE LA CAVIDAD, PERMITE QUE LA FOTODENSIDAD SE INCREMENTE DENTRO DE LA CAVIDAD. CUANDO EL LIMITE RAMAN DEL MEDIO SE EXCEDE, EL MEDIO RAMAN ABSORBE Y ENTONCES IRRADIA FOTONES. LOS FOTONES IRRADIADOS SON DE MAS LONGITUD DE ONDA QUE LOS FOTONES LASER, Y TAMBIEN SE SUCEDEN PULSOS MUY CORTOS (MENORES DE NANOSEGUNDOS ). LOS FOTONES IRRADIADOS SE REFLEJAN EN UN ESPEJO (101) Y SALEN A TRAVES DE LA CAVIADAD DE UN DE LOS REFLECTROS DEFINIENDOSE UNA CAVIDAD (ESPEJO 110). EL INVENTO CAMBIA LA LONGITUD DE ONDA Y ACORTA LA DURACION DEL PULSO O PULSOS PRODUCIDOS POR EL LASER.
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US10362787A | 1987-10-02 | 1987-10-02 |
Publications (2)
Publication Number | Publication Date |
---|---|
ES2059530T3 true ES2059530T3 (es) | 1994-11-16 |
ES2059530T5 ES2059530T5 (es) | 2000-04-16 |
Family
ID=22296172
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
ES88309033T Expired - Lifetime ES2059530T5 (es) | 1987-10-02 | 1988-09-29 | Resonador de celula de raman intracavitario. |
Country Status (10)
Country | Link |
---|---|
EP (1) | EP0314308B2 (es) |
JP (1) | JP2901072B2 (es) |
KR (1) | KR920009920B1 (es) |
DE (1) | DE3851407T3 (es) |
EG (1) | EG18924A (es) |
ES (1) | ES2059530T5 (es) |
IL (1) | IL87771A (es) |
NO (1) | NO180800C (es) |
TR (1) | TR26533A (es) |
WO (1) | WO1989003131A1 (es) |
Families Citing this family (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE4111835A1 (de) * | 1991-04-11 | 1992-10-15 | Eltro Gmbh | Ramanlaser |
GB2256082A (en) * | 1991-05-24 | 1992-11-25 | Synergetic Resources Ltd | Infrared radiation source incorporating a raman medium for isotope separation |
US5251221A (en) * | 1992-08-10 | 1993-10-05 | Hughes Aircraft Company | Self aligning intracavity Raman laser |
DE4423308A1 (de) * | 1994-07-02 | 1996-01-04 | Zeiss Carl Fa | Intracavity-Raman-Laser |
Family Cites Families (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3668420A (en) * | 1970-09-25 | 1972-06-06 | Ibm | 1.5 micron raman laser |
FR2542104B1 (fr) * | 1983-03-04 | 1986-04-18 | Centre Nat Rech Scient | Procede et dispositif de creation d'impulsions lumineuses breves |
-
1988
- 1988-08-30 JP JP63509505A patent/JP2901072B2/ja not_active Expired - Lifetime
- 1988-08-30 WO PCT/US1988/002962 patent/WO1989003131A1/en unknown
- 1988-09-15 IL IL87771A patent/IL87771A/xx active Protection Beyond IP Right Term
- 1988-09-21 TR TR88/0682A patent/TR26533A/xx unknown
- 1988-09-29 ES ES88309033T patent/ES2059530T5/es not_active Expired - Lifetime
- 1988-09-29 EP EP88309033A patent/EP0314308B2/en not_active Expired - Lifetime
- 1988-09-29 DE DE3851407T patent/DE3851407T3/de not_active Expired - Lifetime
- 1988-10-02 EG EG50488A patent/EG18924A/xx active
-
1989
- 1989-06-01 KR KR8970978A patent/KR920009920B1/ko not_active IP Right Cessation
- 1989-06-01 NO NO892225A patent/NO180800C/no not_active IP Right Cessation
Also Published As
Publication number | Publication date |
---|---|
NO180800C (no) | 1997-06-25 |
EG18924A (en) | 1994-07-30 |
DE3851407T3 (de) | 2000-08-03 |
EP0314308B2 (en) | 2000-02-02 |
NO180800B (no) | 1997-03-17 |
JPH02501520A (ja) | 1990-05-24 |
NO892225D0 (no) | 1989-06-01 |
ES2059530T5 (es) | 2000-04-16 |
NO892225L (no) | 1989-06-01 |
KR890702303A (ko) | 1989-12-23 |
TR26533A (tr) | 1994-04-22 |
EP0314308A1 (en) | 1989-05-03 |
JP2901072B2 (ja) | 1999-06-02 |
DE3851407T2 (de) | 1995-01-19 |
IL87771A (en) | 1992-03-29 |
DE3851407D1 (de) | 1994-10-13 |
EP0314308B1 (en) | 1994-09-07 |
WO1989003131A1 (en) | 1989-04-06 |
KR920009920B1 (en) | 1992-11-06 |
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Legal Events
Date | Code | Title | Description |
---|---|---|---|
FG2A | Definitive protection |
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