PL400752A1 - Compression method for spectral short laser pulse light having a broad spectrum, and the optical system for the compression - Google Patents

Compression method for spectral short laser pulse light having a broad spectrum, and the optical system for the compression

Info

Publication number
PL400752A1
PL400752A1 PL400752A PL40075212A PL400752A1 PL 400752 A1 PL400752 A1 PL 400752A1 PL 400752 A PL400752 A PL 400752A PL 40075212 A PL40075212 A PL 40075212A PL 400752 A1 PL400752 A1 PL 400752A1
Authority
PL
Poland
Prior art keywords
light
pulse
compression
optical system
twitter
Prior art date
Application number
PL400752A
Other languages
Polish (pl)
Other versions
PL220928B1 (en
Inventor
Michal Nejbauer
Yuriy Stepanenko
Czesław Radzewicz
Paweł Wnuk
Piotr Skibiński
Michał Laskownicki
Original Assignee
Instytut Chemii Fizycznej Polskiej Akademii Nauk
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 Instytut Chemii Fizycznej Polskiej Akademii Nauk filed Critical Instytut Chemii Fizycznej Polskiej Akademii Nauk
Priority to PL400752A priority Critical patent/PL220928B1/en
Priority to GB1315047.9A priority patent/GB2506014B/en
Publication of PL400752A1 publication Critical patent/PL400752A1/en
Publication of PL220928B1 publication Critical patent/PL220928B1/en

Links

Classifications

    • 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
    • G02F1/37—Non-linear optics for second-harmonic generation
    • 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
    • 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
    • G02F2201/00—Constructional arrangements not provided for in groups G02F1/00 - G02F7/00
    • G02F2201/30—Constructional arrangements not provided for in groups G02F1/00 - G02F7/00 grating
    • G02F2201/307—Reflective grating, i.e. Bragg grating
    • 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
    • G02F2203/26—Pulse shaping; Apparatus or methods therefor
    • 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
    • H01S3/0092—Nonlinear frequency conversion, e.g. second harmonic generation [SHG] or sum- or difference-frequency generation outside the laser cavity

Landscapes

  • Physics & Mathematics (AREA)
  • Nonlinear Science (AREA)
  • Electromagnetism (AREA)
  • Optics & Photonics (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • General Physics & Mathematics (AREA)
  • Optical Modulation, Optical Deflection, Nonlinear Optics, Optical Demodulation, Optical Logic Elements (AREA)

Abstract

Przedmiotem wynalazku jest sposób kompresji spektralnej krótkich impulsów laserowych swiatla o szerokim widmie, obejmujacy optyczny proces konwersji swiatla w krysztale nieliniowym, przedstawiony na schemacie charakteryzujacy sie tym, ze obejmuje nastepujace etapy: a) impuls laserowy dzieli sie na plytce swiatlodzielacej z wytworzeniem dwóch kopii impulsu swiatla, przy czym b) jedna kopie impulsu swiatla odbija sie od jednej ze stron elementu ze struktura Bragga nadajac impulsowi swiergot zgodny z charakterystyka tego elementu ze struktura Bragga, natomiast druga kopie impulsu swiatla odbija sie od drugiej strony tego samego elementu ze struktura Bragga ze swiergotem nadajac impulsowi swiergot o przeciwnym znaku, a nastepnie c) obydwie kopie impulsu padaja na krysztal nieliniowy, w którym sumuje sie czestosci tych dwóch impulsów swiatla ze swiergotem liniowym i otrzymuje sie zadany waskopasmowy impuls swiatla. Niniejszy wynalazek obejmuje ponadto uklad optyczny do realizacji tego sposobu.The subject of the invention is a method of spectral compression of short laser pulses of light with a wide spectrum, including the optical conversion process of light in a non-linear crystal, presented in the diagram, characterized by the fact that it includes the following steps: a) the laser pulse is divided on the light splitting plate to produce two copies of the light pulse , where b) one copy of the light pulse reflects on one side of the Bragg structure element, giving the pulse a twitter in accordance with the characteristics of this element with the Bragg structure, while the other copy of the light pulse reflects on the other side of the same element with the Bragg structure with a chirping sound to the pulse a twitter of the opposite sign, and then c) both copies of the pulse fall on a nonlinear crystal in which the frequencies of these two light pulses are summed with a linear twitter and a given wideband light pulse is obtained. The present invention further comprises an optical system for carrying out the method.

PL400752A 2012-09-12 2012-09-12 Compression method for spectral short laser pulse light having a broad spectrum, and the optical system for the compression PL220928B1 (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
PL400752A PL220928B1 (en) 2012-09-12 2012-09-12 Compression method for spectral short laser pulse light having a broad spectrum, and the optical system for the compression
GB1315047.9A GB2506014B (en) 2012-09-12 2013-08-22 Method for spectral compression of short broad-bandwidth laser light pulses and optical system for the same

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
PL400752A PL220928B1 (en) 2012-09-12 2012-09-12 Compression method for spectral short laser pulse light having a broad spectrum, and the optical system for the compression

Publications (2)

Publication Number Publication Date
PL400752A1 true PL400752A1 (en) 2014-03-17
PL220928B1 PL220928B1 (en) 2016-01-29

Family

ID=49302080

Family Applications (1)

Application Number Title Priority Date Filing Date
PL400752A PL220928B1 (en) 2012-09-12 2012-09-12 Compression method for spectral short laser pulse light having a broad spectrum, and the optical system for the compression

Country Status (2)

Country Link
GB (1) GB2506014B (en)
PL (1) PL220928B1 (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US9419407B2 (en) 2014-09-25 2016-08-16 Kla-Tencor Corporation Laser assembly and inspection system using monolithic bandwidth narrowing apparatus
CN111542975A (en) * 2017-12-04 2020-08-14 维多利亚林克有限公司 Optical system for narrowing the bandwidth of radiation
JP7760122B2 (en) * 2021-12-20 2025-10-27 国立大学法人横浜国立大学 Terahertz waveform detection device and terahertz waveform detection method

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6198568B1 (en) * 1997-04-25 2001-03-06 Imra America, Inc. Use of Chirped Quasi-phase-matched materials in chirped pulse amplification systems
WO2007142843A2 (en) * 2006-05-24 2007-12-13 Cornell Research Foundation, Inc. Chirped-pulse quadratic nonlinearity-based high-energy pulse compressor

Also Published As

Publication number Publication date
GB2506014A (en) 2014-03-19
GB201315047D0 (en) 2013-10-02
PL220928B1 (en) 2016-01-29
GB2506014B (en) 2017-09-13

Similar Documents

Publication Publication Date Title
IL253931B (en) Transient bragg gratings in optical waveguides and their applications
CO2018000967A2 (en) Bispecific antibodies with tetravalence for a co-stimulator fnt receptor
MX2019003768A (en) HPV SPECIFIC BINDING MOLECULES.
JP2016065871A5 (en)
AR087564A1 (en) OPTIMAL MATRIXES OF MIXING AND USE OF DECORRELATORS IN THE SPACE AUDIO PROCESSING
BRPI0607690A2 (en) systems, methods and equipment for high band excitation generation
US9366939B2 (en) Method for generating ultrashort femtosecond pulses in optical parametric oscillator pumped by long pulses
EP2564477A4 (en) Multiple wavelength raman laser
Biswas et al. Thirring optical solitons with Kerr law nonlinearity
EP2779330A3 (en) Soliton pulse optical fiber laser system
PL400752A1 (en) Compression method for spectral short laser pulse light having a broad spectrum, and the optical system for the compression
RU2014118921A (en) HARDWARE AND SOFTWARE COMPLEX FOR MANAGEMENT OF INNOVATIVE DEVELOPMENT OF THE ENTERPRISE IN THE FIELD OF OIL PRODUCTION AND REFINING
Lozovoy et al. Phase-only synthesis of ultrafast stretched square pulses
Sapaev et al. General second-harmonic pulse shaping in grating-engineered quasi-phase-matched nonlinear crystals
Zhou et al. Optical soliton perturbation with time-and space-dependent dissipation (or gain) and nonlinear dispersion in Kerr and non-Kerr media
Boscolo et al. Design and applications of in-cavity pulse shaping by spectral sculpturing in mode-locked fibre lasers
LT2012008A (en) Method and device for sum-frequency generation of light pulses
Zhao et al. The implementation of temporal synthetic aperture imaging for ultrafast optical processing
CN203535349U (en) Multicolor femtosecond laser generating device
Xu et al. Relaxed dispersion requirement in the generation of chirped RF signals based on frequency-to-time mapping
LT2008089A (en) Method and device for combining laser beams
RU2008139197A (en) METHOD FOR CONVERTING ULTRA-SHORT LASER PULSES INTO THE SECOND HARMONIC
Hussain et al. Design and characterization simulation of Ti: Sapphire‐based femtosecond laser system using Lab2 tools in the NI LabVIEW
LT2013501A (en) Method and device for time - multiplexing of light pulses
LT2012068A (en) Method and device for sum-frquency generation of light pulses.