LT2012090A - Method for generating several wavelength radiation in optical resonator, laser source and laser system - Google Patents

Method for generating several wavelength radiation in optical resonator, laser source and laser system

Info

Publication number
LT2012090A
LT2012090A LT2012090A LT2012090A LT2012090A LT 2012090 A LT2012090 A LT 2012090A LT 2012090 A LT2012090 A LT 2012090A LT 2012090 A LT2012090 A LT 2012090A LT 2012090 A LT2012090 A LT 2012090A
Authority
LT
Lithuania
Prior art keywords
wavelengths
laser
laser source
wavelength radiation
optical
Prior art date
Application number
LT2012090A
Other languages
Lithuanian (lt)
Inventor
KA Jonas JONUÅ
Original Assignee
Integrated Optics, Uab
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 Integrated Optics, Uab filed Critical Integrated Optics, Uab
Priority to LT2012090A priority Critical patent/LT2012090A/en
Priority to PCT/IB2012/057370 priority patent/WO2014057316A1/en
Publication of LT2012090A publication Critical patent/LT2012090A/en

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
    • H01S3/05—Construction or shape of optical resonators; Accommodation of active medium therein; Shape of active medium
    • H01S3/08—Construction or shape of optical resonators or components thereof
    • H01S3/08004—Construction or shape of optical resonators or components thereof incorporating a dispersive element, e.g. a prism for wavelength selection
    • 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
    • H01S3/05—Construction or shape of optical resonators; Accommodation of active medium therein; Shape of active medium
    • H01S3/08—Construction or shape of optical resonators or components thereof
    • H01S3/081—Construction or shape of optical resonators or components thereof comprising three or more reflectors
    • H01S3/082—Construction or shape of optical resonators or components thereof comprising three or more reflectors defining a plurality of resonators, e.g. for mode selection or suppression
    • H01S3/0823—Construction or shape of optical resonators or components thereof comprising three or more reflectors defining a plurality of resonators, e.g. for mode selection or suppression incorporating a dispersive element, e.g. a prism for wavelength selection
    • 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
    • H01S3/109—Frequency multiplication, e.g. 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
    • H01S3/14—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
    • H01S3/1603—Solid materials characterised by an active (lasing) ion rare earth
    • H01S3/1611—Solid materials characterised by an active (lasing) ion rare earth neodymium
    • 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
    • H01S3/164—Solid materials characterised by a crystal matrix garnet
    • H01S3/1643—YAG

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • Optics & Photonics (AREA)
  • Lasers (AREA)

Abstract

An object of the present invention is to provide a laser source capable of simultaneously generating several wavelength radiation at desired power ratio between each other. Said radiation of two or more wavelengths can be used for mixing of said wavelengths in a non-linear optical media in order to achieve different wavelength radiation than those amplified in the gain media. In the most preferred embodiment, a laser source comprises two or more reflective surfaces, arranged in an optical cavity (7), having essentially a single optical axis. Tuning of the laser is performed by moving or tilting the optical substrates comprising the reflective surfaces with respect to the axis of the cavity. As a result, desired ratio or proportions of average power are achieved for each of said wavelengths. Having the ability to change the power ratio is important for achieving simultaneous generation of several wavelengths in a single gain media, thus avoiding depletion of the exited state by the dominant wavelength.
LT2012090A 2012-10-10 2012-10-10 Method for generating several wavelength radiation in optical resonator, laser source and laser system LT2012090A (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
LT2012090A LT2012090A (en) 2012-10-10 2012-10-10 Method for generating several wavelength radiation in optical resonator, laser source and laser system
PCT/IB2012/057370 WO2014057316A1 (en) 2012-10-10 2012-12-17 A method for generating or amplifying several wavelength laser radiation in an optical cavity, a laser source and a laser system

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
LT2012090A LT2012090A (en) 2012-10-10 2012-10-10 Method for generating several wavelength radiation in optical resonator, laser source and laser system

Publications (1)

Publication Number Publication Date
LT2012090A true LT2012090A (en) 2014-04-25

Family

ID=47630437

Family Applications (1)

Application Number Title Priority Date Filing Date
LT2012090A LT2012090A (en) 2012-10-10 2012-10-10 Method for generating several wavelength radiation in optical resonator, laser source and laser system

Country Status (2)

Country Link
LT (1) LT2012090A (en)
WO (1) WO2014057316A1 (en)

Family Cites Families (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE3704338C2 (en) * 1987-02-12 1995-04-06 Gsf Forschungszentrum Umwelt Device for generating different laser wavelengths from the same laser medium
FR2658367B1 (en) * 1990-02-13 1992-06-05 Sagem LASER PROVIDING TWO WAVES AT DIFFERENT FREQUENCIES.
US5408481A (en) * 1992-10-26 1995-04-18 The United States Of America As Represented By The Secretary Of The Navy Intracavity sum frequency generation using a tunable laser containing an active mirror
US5345457A (en) 1993-02-02 1994-09-06 Schwartz Electro-Optics, Inc. Dual wavelength laser system with intracavity sum frequency mixing
US20090304033A1 (en) * 2006-03-13 2009-12-10 Lighthouse Technologies Pty Ltd Laser for generating multiple wavelengths
US7848381B2 (en) 2008-02-15 2010-12-07 The United States Of America As Represented By The Administrator Of The National Aeronautics And Space Administration Multiple-wavelength tunable laser

Also Published As

Publication number Publication date
WO2014057316A1 (en) 2014-04-17

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Legal Events

Date Code Title Description
BB1A Patent application published

Effective date: 20140425