WO2006008135A2 - Generation of radiation with stabilized frequency - Google Patents
Generation of radiation with stabilized frequency Download PDFInfo
- Publication number
- WO2006008135A2 WO2006008135A2 PCT/EP2005/007850 EP2005007850W WO2006008135A2 WO 2006008135 A2 WO2006008135 A2 WO 2006008135A2 EP 2005007850 W EP2005007850 W EP 2005007850W WO 2006008135 A2 WO2006008135 A2 WO 2006008135A2
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- frequency
- optical medium
- anyone
- linear optical
- pulses
- Prior art date
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
- H01S3/13—Stabilisation of laser output parameters, e.g. frequency or amplitude
- H01S3/131—Stabilisation of laser output parameters, e.g. frequency or amplitude by controlling the active medium, e.g. by controlling the processes or apparatus for excitation
- H01S3/1312—Stabilisation of laser output parameters, e.g. frequency or amplitude by controlling the active medium, e.g. by controlling the processes or apparatus for excitation by controlling the optical pumping
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/35—Non-linear optics
- G02F1/353—Frequency conversion, i.e. wherein a light beam is generated with frequency components different from those of the incident light beams
- G02F1/3534—Three-wave interaction, e.g. sum-difference frequency generation
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F2203/00—Function characteristic
- G02F2203/56—Frequency comb synthesizer
-
- 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
- H01S3/005—Optical devices external to the laser cavity, specially adapted for lasers, e.g. for homogenisation of the beam or for manipulating laser pulses, e.g. pulse shaping
- H01S3/0057—Temporal shaping, e.g. pulse compression, frequency chirping
-
- 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
- H01S3/13—Stabilisation of laser output parameters, e.g. frequency or amplitude
- H01S3/1307—Stabilisation of the phase
-
- 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
- H01S3/14—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range characterised by the material used as the active medium
- H01S3/16—Solid materials
- H01S3/1601—Solid materials characterised by an active (lasing) ion
- H01S3/162—Solid materials characterised by an active (lasing) ion transition metal
- H01S3/1625—Solid materials characterised by an active (lasing) ion transition metal titanium
-
- 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
- H01S3/14—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range characterised by the material used as the active medium
- H01S3/16—Solid materials
- H01S3/163—Solid materials characterised by a crystal matrix
- H01S3/1631—Solid materials characterised by a crystal matrix aluminate
- H01S3/1636—Al2O3 (Sapphire)
Definitions
- Measuring the CEO frequency f CE0 in this case relies on the heterodyne detection of the short- wavelength modes of the comb with the frequency-doubled long- wavelength modes, which can be accomplished if the frequency comb spans a full optical octave. This method has been referred to as the "f to 2f" technique.
- the CEO-measured CEO frequency f CE o may be compared to a stabilized radiofrequency and locked to it by means of a feedback loop that controls the round-trip CEO phase via the resonator dispersion or via the intra-cavity en ⁇ ergy.
- the output light of the non-linear crystal 4 is sent to a detector and stabilizing unit 10 comprising a detector
- Fig. 4 shows the out-of-loop phase noise power spectral density (PSD) and integrated CEO phase error (CEO PE) versus frequency, as a function of observation time (frequency "1 ) .
- the pulses passing through the non-linear crystal 4 were re-compressed by the delay line 8 down to 6 f s , which is few-cycle pulse, and the measured out of loop phase noise was 0.0427 ⁇ rad (from 10 ⁇ s to 35 minutes observation time) , which is approximately five times better than that of the prior art phase stabilization methods, s. Ref. [18, 22] .
- the large phase error step-like structure around the observation time corresponding to about 200 Hz (indicated by 16 in Fig. 4) is much less pronounced than that of Ref. [18] .
Landscapes
- Physics & Mathematics (AREA)
- Nonlinear Science (AREA)
- Electromagnetism (AREA)
- Optics & Photonics (AREA)
- Engineering & Computer Science (AREA)
- Plasma & Fusion (AREA)
- General Physics & Mathematics (AREA)
- Lasers (AREA)
- Optical Modulation, Optical Deflection, Nonlinear Optics, Optical Demodulation, Optical Logic Elements (AREA)
- Gyroscopes (AREA)
Abstract
Description
Claims
Priority Applications (5)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
EP05763657A EP1779479B1 (en) | 2004-07-21 | 2005-07-19 | Generation of radiation with stabilized frequency |
DE602005014244T DE602005014244D1 (en) | 2004-07-21 | 2005-07-19 | RADIATION GENERATION WITH STABILIZED FREQUENCY |
US11/572,312 US7474457B2 (en) | 2004-07-21 | 2005-07-19 | Generation of radiation with stabilized frequency |
JP2007521886A JP4718547B2 (en) | 2004-07-21 | 2005-07-19 | Generation of frequency stabilized radiation |
CA2574111A CA2574111C (en) | 2004-07-21 | 2005-07-19 | Generation of radiation with stabilized frequency |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
AT12422004 | 2004-07-21 | ||
ATA1242/2004 | 2004-07-21 |
Publications (2)
Publication Number | Publication Date |
---|---|
WO2006008135A2 true WO2006008135A2 (en) | 2006-01-26 |
WO2006008135A3 WO2006008135A3 (en) | 2006-04-13 |
Family
ID=35311804
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
PCT/EP2005/007850 WO2006008135A2 (en) | 2004-07-21 | 2005-07-19 | Generation of radiation with stabilized frequency |
Country Status (7)
Country | Link |
---|---|
US (1) | US7474457B2 (en) |
EP (1) | EP1779479B1 (en) |
JP (1) | JP4718547B2 (en) |
CN (1) | CN100483871C (en) |
CA (1) | CA2574111C (en) |
DE (1) | DE602005014244D1 (en) |
WO (1) | WO2006008135A2 (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2009000079A1 (en) * | 2007-06-26 | 2008-12-31 | Universite Laval | Referencing of the beating spectra of frequency combs |
EP2101161A1 (en) | 2008-03-13 | 2009-09-16 | Szegedi Tudomanyegyetem | Bandwidth-independent method and setup for measuring and stabilizing the carrier-envelope phase drift of laser pulses |
US7907332B2 (en) * | 2006-05-26 | 2011-03-15 | Osaka University | Wide-band ultrashort-pulse optical oscillator utilizing chirped pulse amplification |
US8462825B2 (en) * | 2006-12-01 | 2013-06-11 | Max-Planck-Gesellschaft Zur Forderung Der Wissenschaften E.V. | Method and device for carrier envelope phase stabilisation |
Families Citing this family (25)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2007070428A1 (en) * | 2005-12-09 | 2007-06-21 | Massachusetts Institute Of Technology | Carrier-envelope phase shift using linear media |
US7873272B2 (en) * | 2006-11-13 | 2011-01-18 | Alcatel-Lucent Usa Inc. | Optical pulse characterization using phase modulation |
US8018979B2 (en) * | 2007-10-04 | 2011-09-13 | Femtolasers Produktions Gmbh | Mode-locked short pulse laser resonator and short pulse laser arrangement |
KR100942380B1 (en) * | 2007-11-23 | 2010-02-12 | 광주과학기술원 | Apparatus and Method for stabilizing carrier-envelope phase of laser pulses using direct locking method |
US8462427B2 (en) * | 2009-07-24 | 2013-06-11 | Coherent, Inc. | Carrier envelope phase stabilization of an optical amplifier |
CN101764346B (en) * | 2010-02-12 | 2012-10-24 | 华东师范大学 | High-power laser pulse carrier envelope phase locking method |
DE102010019814A1 (en) * | 2010-05-05 | 2011-11-10 | Friedrich-Schiller-Universität Jena | Device for phase evaluation of few-cycle-pulses of laser radiation in stereo-flight time spectrometer in laser technology, has detectors arranged downstream of integrators connected with evaluation unit for calculating phase of pulses |
DE102010048576B9 (en) * | 2010-10-18 | 2012-11-15 | Toptica Photonics Ag | Laser device for generating a CEO-free frequency comb |
CN102013626B (en) * | 2010-11-10 | 2011-12-07 | 山西大学 | Band selection device for femtosecond laser output by optical frequency comb |
US8774238B2 (en) * | 2011-06-30 | 2014-07-08 | Coherent, Inc. | Mode-locked optically pumped semiconductor laser |
US8411354B2 (en) | 2011-08-05 | 2013-04-02 | Coherent, Inc. | Carrier-envelope-phase stabilization of a master oscillator optical amplifier system |
BR112014008853A2 (en) * | 2011-10-11 | 2017-04-25 | Univ Do Porto | method and device for the simultaneous compression and characterization of ultrashort laser pulses |
JP6118507B2 (en) * | 2012-04-19 | 2017-04-19 | 学校法人慶應義塾 | Spectrometer |
JP6254356B2 (en) * | 2013-04-16 | 2017-12-27 | 株式会社ミツトヨ | Optical frequency comb generator and optical frequency comb frequency stabilization method |
EP2866311B8 (en) | 2013-10-25 | 2018-06-27 | Ludwig-Maximilians-Universität München | Method and device for controlling a carrier-envelope phase and/or an intensity of output pulses of a pulse laser device |
US9240663B2 (en) * | 2013-11-14 | 2016-01-19 | Coherent, Inc. | Tunable femtosecond laser-pulse source including a super-continuum generator |
JP2015132774A (en) * | 2014-01-15 | 2015-07-23 | 日本電信電話株式会社 | wavelength conversion light source |
CN104538832A (en) * | 2014-11-19 | 2015-04-22 | 中国科学院光电研究院 | Pulse laser time domain frequency doubling device |
CN104935291B (en) * | 2015-06-25 | 2017-12-26 | 北京无线电计量测试研究所 | A kind of Low phase noise sapphire microwave oscillator |
EP3314707A4 (en) * | 2015-06-26 | 2019-02-20 | Mezmeriz, Inc. | Beat signal bandwidth compression method, apparatus, and applications |
EP3518354A1 (en) | 2018-01-25 | 2019-07-31 | Max-Planck-Gesellschaft zur Förderung der Wissenschaften e.V. | Device and method for generating laser pulses by kerr lens based mode locking with a loss-modulation device as a kerr medium |
CN109683424B (en) * | 2018-12-27 | 2020-10-27 | 中国科学技术大学 | Multi-frequency ultrashort laser pulse train generating device |
JP7448939B2 (en) * | 2020-03-10 | 2024-03-13 | 東海光学株式会社 | Delay mirror and delay mirror system |
CN112393809B (en) * | 2020-11-19 | 2021-10-19 | 中国科学技术大学 | Self-interference-based method for measuring optical frequency difference between two independent lasers |
GB202212004D0 (en) * | 2022-08-17 | 2022-09-28 | Ucl Business Ltd | Optical frequency comb generation apparatus and method |
Family Cites Families (3)
Publication number | Priority date | Publication date | Assignee | Title |
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JPH0212227A (en) * | 1988-06-30 | 1990-01-17 | Hamamatsu Photonics Kk | Light pulse generating device |
US6034976A (en) * | 1998-03-09 | 2000-03-07 | State Of Oregon Acting By And Through The State Board Of Higher Education On Behalf Of The University Of Oregon | Method and apparatus for laser frequency stabilization |
US6724788B1 (en) * | 2000-09-06 | 2004-04-20 | Max-Planck-Gesellschaft Zur Forderung Der Wissenschaften E.V. | Method and device for generating radiation with stabilized frequency |
-
2005
- 2005-07-19 WO PCT/EP2005/007850 patent/WO2006008135A2/en active Application Filing
- 2005-07-19 EP EP05763657A patent/EP1779479B1/en not_active Not-in-force
- 2005-07-19 CN CNB2005800248078A patent/CN100483871C/en not_active Expired - Fee Related
- 2005-07-19 JP JP2007521886A patent/JP4718547B2/en not_active Expired - Fee Related
- 2005-07-19 DE DE602005014244T patent/DE602005014244D1/en active Active
- 2005-07-19 CA CA2574111A patent/CA2574111C/en not_active Expired - Fee Related
- 2005-07-19 US US11/572,312 patent/US7474457B2/en not_active Expired - Fee Related
Non-Patent Citations (4)
Title |
---|
FUJI T ET AL: "Self-stabilization of carrier-envelope offset phase by use of difference-frequency generation" OPTICS LETTERS OPT. SOC. AMERICA USA, vol. 29, no. 6, 15 March 2004 (2004-03-15), pages 632-634, XP002356037 ISSN: 0146-9592 cited in the application * |
TAKAO FUJI ET AL: "Attosecond control of optical waveforms" NEW JOURNAL OF PHYSICS DEUTSCHE PHYSIKALISCHE GESELLSCHAFT & IOP PUBLISHING LTD UK, vol. 7, no. 1, January 2005 (2005-01), XP002356038 ISSN: 1367-2630 * |
TRITSCHLER T ET AL: "Role of the carrier-envelope phase in extreme nonlinear optics in ZnO" PROCEEDINGS OF THE SPIE - THE INTERNATIONAL SOCIETY FOR OPTICAL ENGINEERING SPIE-INT. SOC. OPT. ENG USA, vol. 4992, 2003, pages 33-42, XP002356181 ISSN: 0277-786X * |
ZIMMERMANN M ET AL: "Optical clockwork with an offset-free difference-frequency comb: accuracy of sum- and difference-frequency generation" OPTICS LETTERS, OSA, OPTICAL SOCIETY OF AMERICA, WASHINGTON, DC, US, vol. 29, no. 3, 1 February 2004 (2004-02-01), pages 310-312, XP002336000 ISSN: 0146-9592 * |
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US7907332B2 (en) * | 2006-05-26 | 2011-03-15 | Osaka University | Wide-band ultrashort-pulse optical oscillator utilizing chirped pulse amplification |
US8462825B2 (en) * | 2006-12-01 | 2013-06-11 | Max-Planck-Gesellschaft Zur Forderung Der Wissenschaften E.V. | Method and device for carrier envelope phase stabilisation |
WO2009000079A1 (en) * | 2007-06-26 | 2008-12-31 | Universite Laval | Referencing of the beating spectra of frequency combs |
US8477314B2 (en) | 2007-06-26 | 2013-07-02 | UNIVERSITé LAVAL | Referencing of the beating spectra of frequency combs |
US8625101B2 (en) | 2007-06-26 | 2014-01-07 | UNIVERSITé LAVAL | Referencing of the beating spectra of frequency combs |
EP2101161A1 (en) | 2008-03-13 | 2009-09-16 | Szegedi Tudomanyegyetem | Bandwidth-independent method and setup for measuring and stabilizing the carrier-envelope phase drift of laser pulses |
Also Published As
Publication number | Publication date |
---|---|
US20080049301A1 (en) | 2008-02-28 |
CN100483871C (en) | 2009-04-29 |
JP4718547B2 (en) | 2011-07-06 |
DE602005014244D1 (en) | 2009-06-10 |
EP1779479A2 (en) | 2007-05-02 |
JP2008507143A (en) | 2008-03-06 |
EP1779479B1 (en) | 2009-04-29 |
WO2006008135A3 (en) | 2006-04-13 |
CA2574111C (en) | 2012-11-27 |
US7474457B2 (en) | 2009-01-06 |
CN1989665A (en) | 2007-06-27 |
CA2574111A1 (en) | 2006-01-26 |
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