USH882H - Multiple-section pulsed gas laser - Google Patents

Multiple-section pulsed gas laser Download PDF

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Publication number
USH882H
USH882H US07/359,602 US35960289A USH882H US H882 H USH882 H US H882H US 35960289 A US35960289 A US 35960289A US H882 H USH882 H US H882H
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United States
Prior art keywords
gas
laser
enclosures
enclosure
section
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Abandoned
Application number
US07/359,602
Inventor
Clifton S. Fox
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United States Department of the Army
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United States Department of the Army
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Application filed by United States Department of the Army filed Critical United States Department of the Army
Priority to US07/359,602 priority Critical patent/USH882H/en
Assigned to UNITED STATES OF AMERICA, THE, AS REPRESENTED BY THE SECRETARY OF THE ARMY reassignment UNITED STATES OF AMERICA, THE, AS REPRESENTED BY THE SECRETARY OF THE ARMY ASSIGNMENT OF ASSIGNORS INTEREST. Assignors: FOX, CLIFTON S.
Application granted granted Critical
Publication of USH882H publication Critical patent/USH882H/en
Abandoned legal-status Critical Current

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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES 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
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/05Construction or shape of optical resonators; Accommodation of active medium therein; Shape of active medium
    • H01S3/06Construction or shape of active medium
    • H01S3/07Construction or shape of active medium consisting of a plurality of parts, e.g. segments
    • H01S3/073Gas lasers comprising separate discharge sections in one cavity, e.g. hybrid lasers

Definitions

  • This invention is in the field of pulsed gas laser, and is particularly concerned with lasers capable of providing pulses of laser light at different wavelengths, and/or pulse shapes and power levels from a single laser cavity.
  • lasers capable of providing pulses of laser light at different wavelengths, and/or pulse shapes and power levels from a single laser cavity.
  • it is necessary to either use multiple lasers, or some means to tune a single laser discharge section.
  • Multiple lasers require various beam-combining means to obtain an output beam on a particular path; these means are both costly and use space.
  • a laser consisting of a discharge section with a tuning mechanism has severe limitations of interpulse time, spectral range, and discharge characteristics, since only a single gas mixture can be used at one time and recovery or recirculation time is needed between pulses.
  • the instant invention overcomes these disadvantages.
  • the invention is a multiple-section pulsed gas laser with a plurality of gas-tight enclosures in a single optical cavity.
  • the enclosures are filled with gases, either neat or mixtures, capable of lasing.
  • gases or mixtures may be used.
  • more than one enclosure may contain the same gas or mixture, if higher power or pulse rates are desired.
  • FIGURE is a schematic representation of the invention, partly in section.
  • housing 1 This housing consists of an elongated tube 2 with transparent end caps 3 and 4. Within the housing are enclosures 5,6, and 7 defined by tube 2, end caps 3 and 4 and transparent plugs 8 and 9. Each of enclosures 5,6, and 7 contain a gaseous material such as a neat gas or mixture of gases capable of lasing when appropriately excited (pumped). Obviously, the same gas or mixture may be used in more than one enclosure, at the same or different pressure. Housing 1 is within an optical cavity defined by mirrors 10 (100% reflective) and 11 (partially reflective) and having an optical axis 12; each of enclosures 5, 6, and 7 is colinear with axis 12.
  • the gas (or gasses) in enclosures 5,6, and 7 are pumped from pulse generators 13,14, and 15 via switches 16,17, and 18 connected to discharge terminals 19,20, and 21.
  • the discharge current returns through grounded terminals 22, 23, and 24.
  • the (13,14,15)/(16,17,18) combination is merely representative, and that some means obvious to ones skilled in the art may be used therefor; depending upon the particular manner in which lasing in enclosures 5,6, and 7 is desired.
  • the combination mentioned above may be computer controlled such that 5,6, and 7 may be operated simultaneously or in any desired sequence or combination.
  • desired pulse generators 13,14, and 15 are connected to discharge electrodes 19,20, and 21 as desired by switches 16,17 and 18 to pump the gaseous material in each selected enclosure. Lasing occurs in the pumped gaseous material(s) and an output beam passes along axis 12 out through output mirror 11.
  • end caps 3 and 4 and plugs 8 and 9 may be set at Brewster's angle for a given polarization of the laser output.
  • the advantages of this invention over the prior art can be seen. Specifically, the use of multiple, independent-discharge section in a single laser cavity eliminates the need for external beam combining optics and saves associated cost and space. Interpulse time can be made as short as desired because different discharge sections may be used to generate sequential pulses rather than having to wait for gas recovery within a single discharge section. Also, flexibility is gained in spectral coverage and pulse characteristic because different gas mixture (including isotopes), different gas pressures and different gain lengths may be used in each section. More optical output coupling can also be achieved for low gain spectral lines by making the gain sections longer for those lines than for higher gain laser lines.

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

Abstract

Several gas-tight enclosures share a common optical cavity. The enclosures may be filled with neat gases or mixtures of gasses. The same gas or mixture, at the same or a different pressure, may occur in more than one enclosure. The gas or gasses in the various enclosures may be pulsed to lase in any desired sequence, simultaneously, or in any combination.

Description

The invention described herein may be manufactured, used, and licensed by the U.S. Government for Governmental purposes without the payment of any royalties thereon.
BACKGROUND OF THE INVENTION
This invention is in the field of pulsed gas laser, and is particularly concerned with lasers capable of providing pulses of laser light at different wavelengths, and/or pulse shapes and power levels from a single laser cavity. Presently, in order to obtain multiple laser wavelengths and/or pulse characteristics, it is necessary to either use multiple lasers, or some means to tune a single laser discharge section. Unfortunately, both of these techniques have disadvantages. Multiple lasers require various beam-combining means to obtain an output beam on a particular path; these means are both costly and use space. A laser consisting of a discharge section with a tuning mechanism has severe limitations of interpulse time, spectral range, and discharge characteristics, since only a single gas mixture can be used at one time and recovery or recirculation time is needed between pulses. The instant invention overcomes these disadvantages.
SUMMARY OF THE INVENTION
The invention is a multiple-section pulsed gas laser with a plurality of gas-tight enclosures in a single optical cavity. The enclosures are filled with gases, either neat or mixtures, capable of lasing. For different spectra or pulse characteristics, different gases or mixtures may be used. Alternatively, more than one enclosure may contain the same gas or mixture, if higher power or pulse rates are desired.
BRIEF DESCRIPTION OF THE DRAWINGS
The single drawing FIGURE is a schematic representation of the invention, partly in section.
DESCRIPTION OF PREFERRED EMBODIMENTS
Referring now to the drawing, we see a housing generally designated 1. This housing consists of an elongated tube 2 with transparent end caps 3 and 4. Within the housing are enclosures 5,6, and 7 defined by tube 2, end caps 3 and 4 and transparent plugs 8 and 9. Each of enclosures 5,6, and 7 contain a gaseous material such as a neat gas or mixture of gases capable of lasing when appropriately excited (pumped). Obviously, the same gas or mixture may be used in more than one enclosure, at the same or different pressure. Housing 1 is within an optical cavity defined by mirrors 10 (100% reflective) and 11 (partially reflective) and having an optical axis 12; each of enclosures 5, 6, and 7 is colinear with axis 12. The gas (or gasses) in enclosures 5,6, and 7 are pumped from pulse generators 13,14, and 15 via switches 16,17, and 18 connected to discharge terminals 19,20, and 21. The discharge current returns through grounded terminals 22, 23, and 24. It should be understood that the (13,14,15)/(16,17,18) combination is merely representative, and that some means obvious to ones skilled in the art may be used therefor; depending upon the particular manner in which lasing in enclosures 5,6, and 7 is desired. For example, the combination mentioned above may be computer controlled such that 5,6, and 7 may be operated simultaneously or in any desired sequence or combination.
Operation of the invention laser is straightforward: desired pulse generators 13,14, and 15 are connected to discharge electrodes 19,20, and 21 as desired by switches 16,17 and 18 to pump the gaseous material in each selected enclosure. Lasing occurs in the pumped gaseous material(s) and an output beam passes along axis 12 out through output mirror 11. Although not shown, it should be obvious that end caps 3 and 4 and plugs 8 and 9 may be set at Brewster's angle for a given polarization of the laser output.
In view of the above description, the advantages of this invention over the prior art can be seen. Specifically, the use of multiple, independent-discharge section in a single laser cavity eliminates the need for external beam combining optics and saves associated cost and space. Interpulse time can be made as short as desired because different discharge sections may be used to generate sequential pulses rather than having to wait for gas recovery within a single discharge section. Also, flexibility is gained in spectral coverage and pulse characteristic because different gas mixture (including isotopes), different gas pressures and different gain lengths may be used in each section. More optical output coupling can also be achieved for low gain spectral lines by making the gain sections longer for those lines than for higher gain laser lines.

Claims (4)

I claim:
1. A multiple-section pulsed gas laser consisting of an optical cavity with an optical axis therein, a plurality of gas tight enclosures colinear to said axis, a gaseous material capable of lasing in each of said enclosures, and individual selectable means for pumping the material in a respective enclosure to cause lasing of the material therein.
2. The laser as set forth in claim 1 wherein a material in a particular enclosure is neat gas.
3. The laser as set forth in claim 1 wherein a material in a particular enclosure is a mixture of gasses.
4. The laser as set forth in claim 1 wherein more than one enclosure contains the same material.
US07/359,602 1989-06-01 1989-06-01 Multiple-section pulsed gas laser Abandoned USH882H (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
US07/359,602 USH882H (en) 1989-06-01 1989-06-01 Multiple-section pulsed gas laser

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
US07/359,602 USH882H (en) 1989-06-01 1989-06-01 Multiple-section pulsed gas laser

Publications (1)

Publication Number Publication Date
USH882H true USH882H (en) 1991-01-01

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Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5111334A (en) * 1990-01-27 1992-05-05 Alcatel N.V. Multi-stage fiber-optic amplifier
DE4230495A1 (en) * 1992-09-11 1994-03-17 Bergmann Hans Wilhelm Changing the power output of laser arrangements - comprises synchronising excitation of the oscillator and amplifiers to continuously change power output
DE4230496A1 (en) * 1992-09-11 1994-03-17 Bergmann Hans Wilhelm Precision working of sheet with pulsed laser beam - using the amplified low divergent portion of the beam
US5528619A (en) * 1994-05-13 1996-06-18 Deutsche Forschungsanstalt Fuer Luft-Und Raumfahrt E.V. Gas discharge structure
US20050094697A1 (en) * 2003-01-30 2005-05-05 Rofin Sinar Laser Gmbh Stripline laser
WO2005070160A3 (en) * 2004-01-12 2007-07-12 Litelaser L L C Multi-path laser system
US20070195839A1 (en) * 2004-08-30 2007-08-23 Litelaser Llc Laser system
US20150303651A1 (en) * 2013-10-18 2015-10-22 Bae Systems Information And Electronic Systems Integration Inc. Ultra fast semiconductor laser

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3460053A (en) * 1966-11-08 1969-08-05 Us Air Force Means for producing long gas discharges
JPS5553472A (en) * 1978-10-13 1980-04-18 Matsushita Electric Ind Co Ltd Series discharge tube
US4481632A (en) * 1981-09-12 1984-11-06 Messer Griesheim Gmbh Laser, particularly CO2 gas transport laser
JPS61283184A (en) * 1985-06-10 1986-12-13 Mitsubishi Electric Corp Silent discharge gas laser device

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3460053A (en) * 1966-11-08 1969-08-05 Us Air Force Means for producing long gas discharges
JPS5553472A (en) * 1978-10-13 1980-04-18 Matsushita Electric Ind Co Ltd Series discharge tube
US4481632A (en) * 1981-09-12 1984-11-06 Messer Griesheim Gmbh Laser, particularly CO2 gas transport laser
JPS61283184A (en) * 1985-06-10 1986-12-13 Mitsubishi Electric Corp Silent discharge gas laser device

Cited By (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5111334A (en) * 1990-01-27 1992-05-05 Alcatel N.V. Multi-stage fiber-optic amplifier
DE4230495A1 (en) * 1992-09-11 1994-03-17 Bergmann Hans Wilhelm Changing the power output of laser arrangements - comprises synchronising excitation of the oscillator and amplifiers to continuously change power output
DE4230496A1 (en) * 1992-09-11 1994-03-17 Bergmann Hans Wilhelm Precision working of sheet with pulsed laser beam - using the amplified low divergent portion of the beam
US5528619A (en) * 1994-05-13 1996-06-18 Deutsche Forschungsanstalt Fuer Luft-Und Raumfahrt E.V. Gas discharge structure
US20050094697A1 (en) * 2003-01-30 2005-05-05 Rofin Sinar Laser Gmbh Stripline laser
WO2005070160A3 (en) * 2004-01-12 2007-07-12 Litelaser L L C Multi-path laser system
US20070195839A1 (en) * 2004-08-30 2007-08-23 Litelaser Llc Laser system
US7583717B2 (en) 2004-08-30 2009-09-01 Videojet Technologies Inc Laser system
US20150303651A1 (en) * 2013-10-18 2015-10-22 Bae Systems Information And Electronic Systems Integration Inc. Ultra fast semiconductor laser
US9601895B2 (en) * 2013-10-18 2017-03-21 Bae Systems Information And Electronic Systems Integration Inc. Ultra fast semiconductor laser

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Owner name: UNITED STATES OF AMERICA, THE, AS REPRESENTED BY T

Free format text: ASSIGNMENT OF ASSIGNORS INTEREST.;ASSIGNOR:FOX, CLIFTON S.;REEL/FRAME:005252/0498

Effective date: 19890601

STCF Information on status: patent grant

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