WO1995025367A1 - Laser oscillator system - Google Patents

Laser oscillator system Download PDF

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Publication number
WO1995025367A1
WO1995025367A1 PCT/GB1995/000524 GB9500524W WO9525367A1 WO 1995025367 A1 WO1995025367 A1 WO 1995025367A1 GB 9500524 W GB9500524 W GB 9500524W WO 9525367 A1 WO9525367 A1 WO 9525367A1
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WO
WIPO (PCT)
Prior art keywords
laser oscillator
optical
linear
linear optical
optical device
Prior art date
Application number
PCT/GB1995/000524
Other languages
French (fr)
Inventor
Michael John Damzen
Original Assignee
The Secretary Of State For Defence
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 The Secretary Of State For Defence filed Critical The Secretary Of State For Defence
Priority to AU18574/95A priority Critical patent/AU1857495A/en
Publication of WO1995025367A1 publication Critical patent/WO1995025367A1/en

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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
    • H01S3/10076—Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating using optical phase conjugation, e.g. phase conjugate reflection
    • 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
    • H01S3/083—Ring lasers

Definitions

  • This invention relates to a laser oscillator system and in particular to one which incorporates a holographic volume diffraction element.
  • Laser systems generally require the incorporation of separate spatial and spectral control elements into the laser cavity in order to achieve high spatial quality and narrow linewidth operation.
  • these control elements are passive elements and as such are unable to adapt to physical changes in the laser system which can occur during its operation. These changes lead to a phase distortion of the intra-cavity beam and hence a degradation in one or both of the beam quality and the energy output of the system.
  • Conventional laser systems are therefore sensitive to such physical changes.
  • a phase conjugating stimulated Brillouin (SBS) device within the laser cavity which is able to react to and compensate for this phase distortion.
  • SBS phase conjugating stimulated Brillouin
  • the efficiency of such systems is limited both by the practically achievable reflectivity of the SBS device and the appearance of nonlinearities within the device at high operating powers which are detrimental to its behaviour.
  • the SBS device also induces a frequency shift in the phase conjugated laser line which prevents the system operating on a narrow linewidth even with the provision of expensive spectral control elements within the cavity.
  • one or more optical gain elements for producing light emission comprising: a non-linear optical device capable of providing a phase conjugate output, being together configured to provide an optical ring circuit; and an output coupler;
  • the non-linear optical device is adapted to produce a volume diffraction grating by the self-interaction of the light emission within the device, the diffraction grating being capable of diffracting a part of the light emission into the ring to be amplified through stimulated emission within the one or more optical gain elements and wherein a non-reciprocal transmission device is interposed between the one or more gain elements and the non-linear optical device.
  • This provides a laser oscillator which is able to react to and compensate for phase distortions within the oscillator which may occur particularly at high operating powers.
  • the holographic volume diffraction grating contains any phase information introduced onto the self-interacting emission by phase distortions within the oscillator and so changes as the phase distortions change.
  • the phase information is transferred to the diffracted emission but as a phase conjugate.
  • this phase conjugated diffracted emission travels around the ring it experiences substantially equal but opposite phase distortions to produce an output from the output coupler which is substantially free of phase distortion.
  • the laser oscillator according to the present invention also has the advantage that narrow linewidth operation can be achieved without the need for expensive spectral control elements.
  • the non-reciprocal transmission device is configured to have a maximum transmission for that portion of the laser emission diffracted by the diffraction grating, thereby maximising the efficiency of the laser oscillator.
  • the one or more optical gain elements of the laser oscillator can be pumped in a pulsed mode of operation to provide a self Q-switched oscillator. This occurs because of the parametric growth of the diffraction grating and has the advantage that an active Q-switching device within the oscillator is not required.
  • the non-linear optical device may be formed from an optical gain material such as Nd:YAG.
  • an additional fixed phase distortion is introduced to the phase conjugated diffracted emission when an optical gain medium is used in the non-linear optical device. This additional phase distortion is not compensated for by the travel of the diffracted emission around the ring. It is therefore preferable that the non-reciprocal transmission device is adapted to provide the emission passing through it for one direction of travel only with a phase shift to compensate for and substantially remove the effects of this additional phase distortion.
  • the non-reciprocal transmission device is adapted to introduce a phase shift of radians to the laser emission passing through it in one direction.
  • thermal effects within the laser oscillator according to the present invention can lead to the problem of thermally-induced depolarisation of the laser radiation within the optical gain elements which, in turn, results in beam quality degradation and/or energy loss. This will be the case particularly where the laser oscillator is employed in high average power scaling.
  • the laser oscillator additionally comprises a depolarisation compensator adapted to provide in use orthogonal elliptically, most preferably circularly, polarised light for self-interaction within the non-linear optical device.
  • the depolarisation compensator may for example comprise two quarter wave retardation plates having the non-linear optical device disposed therebetween.
  • the depolarisation compensator may additionally comprise an optical element, for example a quarter wave retardation plate or a 45° Faraday rotator, disposed between the one or more optical gain elements and the non-reciprocal transmission device and adapted to provide linearly polarised light at the non-reciprocal transmission device.
  • an optical element for example a quarter wave retardation plate or a 45° Faraday rotator, disposed between the one or more optical gain elements and the non-reciprocal transmission device and adapted to provide linearly polarised light at the non-reciprocal transmission device.
  • Figure 1 shows a schematic representation of a laser oscillator according to the present invention.
  • Figure 2 shows a non-reciprocal transmission device for use with a non-linear optical device when formed from a laser medium.
  • Figure 3 shows a schematic representation of laser oscillator of Figure 1 further incorporating a depolarisation compensator.
  • spontaneous emission from an optical gain element GE which for example can be a single gain element which may comprise a flash lamp pumped Nd:YAG rod, produces a beam E 1 .
  • This beam is reflected by the mirror M ⁇ to pass through the non-reciprocal transmission device NRTD which is configured to have the direction of maximum transmission in the direction of travel of E (as shown in Figure 1 by the solid line within the non-reciprocal transmission device NRTD).
  • the emergent beam E is reflected by the mirror M 2 towards the non-linear optical device NLOD.
  • this beam, E ⁇ passes through the non-linear optical device NLOD undiffracted and is incident on the output coupler OC, which may for example be a partially transmitting mirror, to produce the reflected beam E 2 which is directed towards the non-linear optical device NLOD.
  • the beam E 2 follows the reciprocal path of E l f passing through the non-reciprocal transmission device NRTD in the reciprocal direction (as shown in Figure 1 by the broken line) to provide an optimum attenuation of the beam E 2 .
  • This attenuated beam E 2 is then amplified by the gain element GE to produce the amplified beam E 3 which is then directed towards the non-linear optical device NLOD by the mirrors M 3 and M 4 .
  • the two beams E 2 and E 3 interfere within the non-linear optical device NLOD to produce a volume diffraction grating containing information on any phase distortions induced in the two beams by the oscillator.
  • a portion of a beam travelling in the direction of E 1 is diffracted to produce a beam E 4 thereby completing the ring.
  • the phase conjugate of the phase information contained in the diffraction grating is transferred onto the beam E 4 by the diffraction.
  • This beam E 4 follows the reciprocal path of E 3 and is amplified within the gain element GE.
  • This amplified beam E 4 then travels around the ring and experiences substantially equal but opposite phase distortions to produce a substantially distortion free laser output from the output coupler OC.
  • the non-linear optical device NLOD comprises an optical gain material, for example a flash lamp pumped Nd:YAG rod, operating at the peak of its spectral response then an additional fixed phase distortion of Tf radians is imparted to the diffracted beam E 4 when it is diffracted.
  • an optical gain material for example a flash lamp pumped Nd:YAG rod
  • an additional fixed phase distortion of Tf radians is imparted to the diffracted beam E 4 when it is diffracted.
  • a non-reciprocal transmission device NRTD of the type shown in Figure 2 can be used. This provides not only the Tf phase compensation but also control of the amplitude of transmission.
  • the non-reciprocal transmission device NRTD shown in Figure 2 comprises a Faraday rotator FR configured to produce a 45° rotation of the angle of the polarisation state of input radiation and a half wave retardation plate HWP that produces a rotation of linear polarised light by an angle 2 ⁇ , where ⁇ is the angle between the input polarisation state and a principal axis of the HWP.
  • ⁇ is the angle between the input polarisation state and a principal axis of the HWP.
  • the Faraday rotator FR and the half wave retardation plate HWP provides a total angle of rotation of polarised light of 45° + 2 ⁇ in one direction and of 45° - 2 ⁇ in the other direction.
  • the depolarisation compensator here comprises quarter wave retardation plates W 1 and W 2 disposed so as to provide beams E ⁇ and E 2 which are orthogonally circularly polarised when counter propagating within the non-linear optical device NLOD.
  • This arrangement produces vectorial phase conjugation of the beam E 3 with an arbitrary polarisation state.
  • the beam E 3 is a depolarised version of the beam E 2 due to the presence of the optical gain element GE.
  • the generated vector phase conjugate beam E 4 will then compensate for depolarisation when passing back through the gain element GE.
  • the depolarisation compensator here additionally comprises a quarter wave retardation plate W 3 interposed between the optical gain element GE and the non-reciprocal transmission device NRTD.
  • This optical element W 3 acts to return the polarisation of E 4 to a linear state for efficient transmission through the non-reciprocal transmission device NRTD which here acts to form a near uni-directional output from the output coupler OC and to optimise the relative beam intensities at non-linear optical device NLOD for optimum diffraction grating formation.

Abstract

A laser oscillator ring comprising one or more optical gain elements GE for producing light emission E1-4; a non-linear optical device NLOD capable of providing a phase conjugate output, these being together configured to provide an optical ring circuit; and an output coupler OC through which laser emission exits the ring circuit. The non-linear optical device NLOD is adapted to produce a volume diffraction grating by the self-interaction of the light emission within the device which is capable of diffracting part of the light emission into the ring to be amplified through stimulated emission within the one or more optical gain elements GE. A non-reciprocal transmission device NRTD is interposed between the one or more gain elements and the non-linear optical device which provides preferential passage of the light emission in one direction of travel around the ring circuit.

Description

Laser Oscillator System
This invention relates to a laser oscillator system and in particular to one which incorporates a holographic volume diffraction element.
Laser systems generally require the incorporation of separate spatial and spectral control elements into the laser cavity in order to achieve high spatial quality and narrow linewidth operation. Conventionally these control elements are passive elements and as such are unable to adapt to physical changes in the laser system which can occur during its operation. These changes lead to a phase distortion of the intra-cavity beam and hence a degradation in one or both of the beam quality and the energy output of the system. Conventional laser systems are therefore sensitive to such physical changes.
One known laser system utilises a phase conjugating stimulated Brillouin (SBS) device within the laser cavity which is able to react to and compensate for this phase distortion. Unfortunately, the efficiency of such systems is limited both by the practically achievable reflectivity of the SBS device and the appearance of nonlinearities within the device at high operating powers which are detrimental to its behaviour. A further disadvantage is that the SBS device also induces a frequency shift in the phase conjugated laser line which prevents the system operating on a narrow linewidth even with the provision of expensive spectral control elements within the cavity. According to the present invention there is provided a laser oscillator comprising:
one or more optical gain elements for producing light emission; a non-linear optical device capable of providing a phase conjugate output, being together configured to provide an optical ring circuit; and an output coupler;
wherein the non-linear optical device is adapted to produce a volume diffraction grating by the self-interaction of the light emission within the device, the diffraction grating being capable of diffracting a part of the light emission into the ring to be amplified through stimulated emission within the one or more optical gain elements and wherein a non-reciprocal transmission device is interposed between the one or more gain elements and the non-linear optical device.
This provides a laser oscillator which is able to react to and compensate for phase distortions within the oscillator which may occur particularly at high operating powers. This is because the holographic volume diffraction grating contains any phase information introduced onto the self-interacting emission by phase distortions within the oscillator and so changes as the phase distortions change. The phase information is transferred to the diffracted emission but as a phase conjugate. As this phase conjugated diffracted emission travels around the ring it experiences substantially equal but opposite phase distortions to produce an output from the output coupler which is substantially free of phase distortion. Furthermore, as no frequency shifting of the phase conjugated diffracted light occurs the laser oscillator according to the present invention also has the advantage that narrow linewidth operation can be achieved without the need for expensive spectral control elements.
Most preferably, the non-reciprocal transmission device is configured to have a maximum transmission for that portion of the laser emission diffracted by the diffraction grating, thereby maximising the efficiency of the laser oscillator.
Most usefully, the one or more optical gain elements of the laser oscillator can be pumped in a pulsed mode of operation to provide a self Q-switched oscillator. This occurs because of the parametric growth of the diffraction grating and has the advantage that an active Q-switching device within the oscillator is not required.
In order to enhance the gain of the laser oscillator the non-linear optical device may be formed from an optical gain material such as Nd:YAG. However, an additional fixed phase distortion is introduced to the phase conjugated diffracted emission when an optical gain medium is used in the non-linear optical device. This additional phase distortion is not compensated for by the travel of the diffracted emission around the ring. It is therefore preferable that the non-reciprocal transmission device is adapted to provide the emission passing through it for one direction of travel only with a phase shift to compensate for and substantially remove the effects of this additional phase distortion. When the optical gain material of the non-linear optical device is operated at or close to the peak of the gain in its spectral response then the additional fixed phase distortion is substantially Tl radians and therefore the non-reciprocal transmission device is adapted to introduce a phase shift of radians to the laser emission passing through it in one direction.
Furthermore, thermal effects within the laser oscillator according to the present invention can lead to the problem of thermally-induced depolarisation of the laser radiation within the optical gain elements which, in turn, results in beam quality degradation and/or energy loss. This will be the case particularly where the laser oscillator is employed in high average power scaling.
In order to alleviate this problem it is advantageous if the laser oscillator additionally comprises a depolarisation compensator adapted to provide in use orthogonal elliptically, most preferably circularly, polarised light for self-interaction within the non-linear optical device. Thus the depolarisation compensator may for example comprise two quarter wave retardation plates having the non-linear optical device disposed therebetween.
Usefully the depolarisation compensator may additionally comprise an optical element, for example a quarter wave retardation plate or a 45° Faraday rotator, disposed between the one or more optical gain elements and the non-reciprocal transmission device and adapted to provide linearly polarised light at the non-reciprocal transmission device. This has the advantage that the non-reciprocal transmission device has only to operate with linearly polarised light thereby facilitating the optimisation of its transmission characteristics to maximise the efficiency of the laser oscillator.
Embodiments of the invention will now be described, by way of example only, with reference to the accompanying drawings in which:
Figure 1 shows a schematic representation of a laser oscillator according to the present invention.
Figure 2 shows a non-reciprocal transmission device for use with a non-linear optical device when formed from a laser medium.
Figure 3 shows a schematic representation of laser oscillator of Figure 1 further incorporating a depolarisation compensator.
Referring now to Figure 1, initially, spontaneous emission from an optical gain element GE, which for example can be a single gain element which may comprise a flash lamp pumped Nd:YAG rod, produces a beam E1. This beam is reflected by the mirror Mχ to pass through the non-reciprocal transmission device NRTD which is configured to have the direction of maximum transmission in the direction of travel of E (as shown in Figure 1 by the solid line within the non-reciprocal transmission device NRTD). The emergent beam E , is reflected by the mirror M2 towards the non-linear optical device NLOD. Substantially all of this beam, Eχ, passes through the non-linear optical device NLOD undiffracted and is incident on the output coupler OC, which may for example be a partially transmitting mirror, to produce the reflected beam E2 which is directed towards the non-linear optical device NLOD. The beam E2 follows the reciprocal path of El f passing through the non-reciprocal transmission device NRTD in the reciprocal direction (as shown in Figure 1 by the broken line) to provide an optimum attenuation of the beam E2. This attenuated beam E2 is then amplified by the gain element GE to produce the amplified beam E3 which is then directed towards the non-linear optical device NLOD by the mirrors M3 and M4.
The two beams E2 and E3 interfere within the non-linear optical device NLOD to produce a volume diffraction grating containing information on any phase distortions induced in the two beams by the oscillator. A portion of a beam travelling in the direction of E1 is diffracted to produce a beam E4 thereby completing the ring. The phase conjugate of the phase information contained in the diffraction grating is transferred onto the beam E4 by the diffraction. This beam E4 follows the reciprocal path of E3 and is amplified within the gain element GE. This amplified beam E4 then travels around the ring and experiences substantially equal but opposite phase distortions to produce a substantially distortion free laser output from the output coupler OC.
When the non-linear optical device NLOD comprises an optical gain material, for example a flash lamp pumped Nd:YAG rod, operating at the peak of its spectral response then an additional fixed phase distortion of Tf radians is imparted to the diffracted beam E4 when it is diffracted. In order to compensate for this a non-reciprocal transmission device NRTD of the type shown in Figure 2 can be used. This provides not only the Tf phase compensation but also control of the amplitude of transmission. The non-reciprocal transmission device NRTD shown in Figure 2 comprises a Faraday rotator FR configured to produce a 45° rotation of the angle of the polarisation state of input radiation and a half wave retardation plate HWP that produces a rotation of linear polarised light by an angle 2θ, where θ is the angle between the input polarisation state and a principal axis of the HWP. Together the Faraday rotator FR and the half wave retardation plate HWP provides a total angle of rotation of polarised light of 45° + 2Θ in one direction and of 45° - 2θ in the other direction.
By placing the Faraday rotator FR and the half wave retardation plate HWP between a pair of linear polarisers (Pχ and P2) it is thereby possible to control the transmission in different directions by varying θ. For example, if the linear polarisers Pχ, P2 have their axes of transmission parallel to one another then when θ=22.5° transmission is unity in one direction and zero in the other. Since the laser oscillator requires transmission in one direction to be high and in the other to be low but non-zero then θ is arranged to be 22.5° + o where O is a small angular offset. It will be understood by those skilled in the art that the amplitude of transmission is independent of whether T is positive or negative but that the transmission in the low transmission direction is relatively shifted by either 0 or Tf radians for the positive or negative cases respectively.
Effects of the depolarisation of the light circulating within the laser oscillator of Figure 1 may be alleviated by incorporating a depolarisation compensator within the laser oscillator as shown in Figure 3 where the symbols t 3 C• 3 represent respectively linearly clockwise and anti-clockwise circularly polarised light. The depolarisation compensator here comprises quarter wave retardation plates W1 and W2 disposed so as to provide beams Eχ and E2 which are orthogonally circularly polarised when counter propagating within the non-linear optical device NLOD.
This arrangement produces vectorial phase conjugation of the beam E3 with an arbitrary polarisation state. In this arrangement the beam E3 is a depolarised version of the beam E2 due to the presence of the optical gain element GE. The generated vector phase conjugate beam E4 will then compensate for depolarisation when passing back through the gain element GE.
The depolarisation compensator here additionally comprises a quarter wave retardation plate W3 interposed between the optical gain element GE and the non-reciprocal transmission device NRTD. This optical element W3 acts to return the polarisation of E4 to a linear state for efficient transmission through the non-reciprocal transmission device NRTD which here acts to form a near uni-directional output from the output coupler OC and to optimise the relative beam intensities at non-linear optical device NLOD for optimum diffraction grating formation.

Claims

1. A laser oscillator comprising:
one or more optical gain elements for producing light emission; a non-linear optical device capable of providing a phase conjugate output, being together configured to provide an optical ring circuit; and an output coupler;
wherein the non-linear optical device is adapted to produce a volume diffraction grating by the self-interaction of the light emission within the device, the diffraction grating being capable of diffracting a part of the light emission into the ring to be amplified through stimulated emission within the one or more optical gain elements and wherein a non-reciprocal transmission device is interposed between the one or more gain elements and the non-linear optical device.
2. A laser oscillator as claimed in claim 1 wherein the one or more optical gain elements are operable in a pulsed mode.
3. A laser oscillator as claimed in claim 1 or claim 2 wherein the non-linear optical device is formed from an optical gain material.
4. A laser oscillator as claimed in claim 3 wherein the non-reciprocal transmission device is adapted to provide a phase shift to emission travelling through it in one direction only.
5. A laser oscillator as claimed in claim 3 or claim 4 wherein the non-linear optical device is adapted to operate at or close to the peak of the gain in its spectral response.
6. A laser oscillator as claimed in any preceding claim wherein there is additionally provided a depolarisation compensator adapted to provide in use orthogonal elliptically polarised light for self-interaction within the non-linear optical device.
7. A laser oscillator as claimed in claim 6 wherein the depolarisation compensator is adapted to provide circularly polarised light.
8. A laser oscillator as claimed in claim 7 wherein the depolarisation compensator comprises two quarter wave retardation plates having disposed therebetween the non-linear optical device.
9. A laser oscillator as claimed in claim 6, claim 7 or claim 8 wherein the depolarisation compensator additionally comprises an optical element disposed between the one or more optical gain elements and the non-reciprocal transmission device and adapted to provide linearly polarised light at the non-reciprocal transmission device.
10. A laser oscillator as claimed in claim 9 wherein the optical element is a 45° Faraday rotator.
11. A laser oscillator as claimed in claim 9 wherein the optical element is a quarter wave retardation plate.
12. A non-reciprocal transmission device comprising a Faraday rotator and half wave retardation plate disposed between a pair of linear polarisers.
13. A non-reciprocal transmission device as claimed in claim 11 wherein the Faraday rotator is adapted to produce a 45° rotation of the angle of polarisation of an input beam, and the pair of linear polarisers being configured to have their axes of transmission mutually parallel.
PCT/GB1995/000524 1994-03-15 1995-03-10 Laser oscillator system WO1995025367A1 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
AU18574/95A AU1857495A (en) 1994-03-15 1995-03-10 Laser oscillator system

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
GB9404987.1 1994-03-15
GB9404987A GB9404987D0 (en) 1994-03-15 1994-03-15 Improvements in or relating to laser systems

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WO1995025367A1 true WO1995025367A1 (en) 1995-09-21

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WO (1) WO1995025367A1 (en)

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1997021260A1 (en) * 1995-12-01 1997-06-12 The University Of Sydney Distributed feedback ring laser
FR2764744A1 (en) * 1997-06-17 1998-12-18 Michel Ouhayoun FOUR-WAVE MIXTURE CONJUGATION MIRROR LASER AND METHOD FOR RENOVATION OF A CLASSIC LASER BY TRANSFORMATION INTO A PHASE CONJUGATION MIRROR LASER
AU705786B2 (en) * 1995-12-01 1999-06-03 University Of Sydney, The Distributed feedback ring laser
WO2007138013A1 (en) * 2006-05-30 2007-12-06 Thales Laser source for lidar application
JP2009541983A (en) * 2006-06-21 2009-11-26 インペリアル・イノベイションズ・リミテッド Laser radiation coherent coupling apparatus and method
EP2637265A1 (en) * 2012-03-05 2013-09-11 Menlo Systems GmbH Laser with non-linear optical loop mirror
EP2846421A1 (en) * 2013-09-06 2015-03-11 Menlo Systems GmbH Laser with non-linear optical loop mirror

Non-Patent Citations (4)

* Cited by examiner, † Cited by third party
Title
M.J.DAMZEN ET AL.: "SPATIAL CHARACTERISTICS OF A LASER OSCILLATOR FORMEDF BY OPTICALLY-WRITTEN HOLOGRAPHIC GAIN-GRATING", OPTICS COMMUNICATIONS, vol. 110, no. 1-2, 1 August 1994 (1994-08-01), AMSTERDAM NL, pages 152 - 156 *
M.S.BARASHKOV ET AL.: "STIMULATED EMISSION IN A SOLID-STATE RING LASER WITH A STIMULATED BRILLOUIN SCATTERING MIRROR", SOVIET JOURNAL OF QUANTUM ELECTRONICS, vol. 20, no. 6, June 1990 (1990-06-01), NEW YORK US, pages 631 - 633 *
R.P.M.GREEN ET AL.: "HOLOGRAPHIC LASER RESONATORS IN Nd:YAG", OPTICS LETTERS., vol. 19, no. 6, 15 March 1994 (1994-03-15), NEW YORK US, pages 393 - 395 *
T.J.KARR: "POWER AND STABILITY OF PHASE-CONJUGATE LASERS", JOURNAL OF THE OPTICAL SOCIETY OF AMERICA, vol. 73, no. 5, May 1983 (1983-05-01), NEW YORK US, pages 600 - 609 *

Cited By (12)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1997021260A1 (en) * 1995-12-01 1997-06-12 The University Of Sydney Distributed feedback ring laser
AU705786B2 (en) * 1995-12-01 1999-06-03 University Of Sydney, The Distributed feedback ring laser
US6272165B1 (en) 1995-12-01 2001-08-07 The University Of Sydney Distributed feedback ring laser
FR2764744A1 (en) * 1997-06-17 1998-12-18 Michel Ouhayoun FOUR-WAVE MIXTURE CONJUGATION MIRROR LASER AND METHOD FOR RENOVATION OF A CLASSIC LASER BY TRANSFORMATION INTO A PHASE CONJUGATION MIRROR LASER
WO1998058429A1 (en) * 1997-06-17 1998-12-23 Michel Ouhayoun Phase-conjugation laser mirror with four-wave mixing
WO2007138013A1 (en) * 2006-05-30 2007-12-06 Thales Laser source for lidar application
FR2901923A1 (en) * 2006-05-30 2007-12-07 Thales Sa LASER SOURCE FOR LIDAR APPLICATION
JP2009541983A (en) * 2006-06-21 2009-11-26 インペリアル・イノベイションズ・リミテッド Laser radiation coherent coupling apparatus and method
US7876796B2 (en) 2006-06-21 2011-01-25 Imperial Innovations Limited Method and apparatus for coherently combining laser emission
EP2637265A1 (en) * 2012-03-05 2013-09-11 Menlo Systems GmbH Laser with non-linear optical loop mirror
EP2846421A1 (en) * 2013-09-06 2015-03-11 Menlo Systems GmbH Laser with non-linear optical loop mirror
US9276372B2 (en) 2013-09-06 2016-03-01 Menlo Systems Gmbh Laser with non-linear optical loop mirror

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AU1857495A (en) 1995-10-03

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