USH882H - Multiple-section pulsed gas laser - Google Patents
Multiple-section pulsed gas laser Download PDFInfo
- 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
- Authority
- US
- United States
- Prior art keywords
- gas
- laser
- enclosures
- enclosure
- section
- Prior art date
- Legal status (The legal status 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 status listed.)
- Abandoned
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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
- H01S3/05—Construction or shape of optical resonators; Accommodation of active medium therein; Shape of active medium
- H01S3/06—Construction or shape of active medium
- H01S3/07—Construction or shape of active medium consisting of a plurality of parts, e.g. segments
- H01S3/073—Gas 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.
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.
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.
The single drawing FIGURE is a schematic representation of the invention, partly in section.
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)
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.
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 |
Family
ID=23414533
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| US07/359,602 Abandoned USH882H (en) | 1989-06-01 | 1989-06-01 | Multiple-section pulsed gas laser |
Country Status (1)
| Country | Link |
|---|---|
| US (1) | USH882H (en) |
Cited By (8)
| 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)
| 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 |
-
1989
- 1989-06-01 US US07/359,602 patent/USH882H/en not_active Abandoned
Patent Citations (4)
| 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)
| 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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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| AS | Assignment |
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 |
Free format text: PATENTED CASE |