US4626792A
Expired / Lapsed
US
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Pure crystal exciton laser amplifier and method of operation
Assignee: Cornell Research Foundation Inc
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Filing: 1984-01-10
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Granted: 1986-12-02
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Expires: 2004-01-10
Abstract
Abstract A laser amplifier and method as disclosed wherein excitons in a pure insulator or semiconductor crystal are triggered by incident resonant laser radiation. The excitons are created by an external intermittent radiative source, and stimulated decay produces light output at a wavelength characteristic of the crystal. The radiative source produces light at the same wavelength as the light output produced by stimulated exciton decay, thereby producing an amplified output.
Inventors
- 👤 Richard L. Liboff
- 👤 Kung C. Liu
Bibliographic Details
Application Number
—
Jurisdiction
US
Data Source
google_patents
Last Synchronized
2026-10-30 23:20
CPC Classifications
H; H01; H01S; H01S3/00; H01S3/23; H01S3/2375; H01S3/09; H01S3/091; H01S3/0915; H01S3/092; H01S3/14; H01S3/16; H01S3/2308
Claims Analysis
Total Claims: 13
Claim 1
Independent Claim
225 words
A laser amplifier comprising: a source of intense, monochromatic, coherent radiation to be amplified, said radiation have a selected wavelength; a laser rod having an axial first and second ends, and being axially aligned with said source of radiation, said first end being adapted to receive said radiation to be amplified, said laser rod comprising a pure, undoped crystal in which the recombination of excitons produces a characteristic output radiation having said selected wavelength; pumping means for producing electron population inversion within said laser rod and to a recombination energy level for the production of excitons within said laser rod the pure crystal laser rod providing a sufficiently high exciton density to assure a nonboson quality in said excitons; and means for alternately activating said pumping means and said source of radiation to first produce said high density of excitons in said laser rod and then to cause said radiation to be amplified to impinge on said first end of said laser rod to stimulate decay of said high density, nonboson quality excitons, such decay producing photons of said characteristic wavelength and resulting in intense monochromatic, coherent output radiation at said characteristic wavelength at said second end of said laser rod, said output radiation being at a greater intensity than, and at the same wavelength as, said source radiation, whereby said source radiation is amplified.
Claim 2
Dependent Claim
225 words
A laser amplifier comprising: a source of intense, monochromatic, coherent radiation to be amplified, said radiation have a selected wavelength; a laser rod having an axial first and second ends, and being axially aligned with said source of radiation, said first end being adapted to receive said radiation to be amplified, said laser rod comprising a pure, undoped crystal in which the recombination of excitons produces a characteristic output radiation having said selected wavelength; pumping means for producing electron population inversion within said laser rod and to a recombination energy level for the production of excitons within said laser rod the pure crystal laser rod providing a sufficiently high exciton density to assure a nonboson quality in said excitons; and means for alternately activating said pumping means and said source of radiation to first produce said high density of excitons in said laser rod and then to cause said radiation to be amplified to impinge on said first end of said laser rod to stimulate decay of said high density, nonboson quality excitons, such decay producing photons of said characteristic wavelength and resulting in intense monochromatic, coherent output radiation at said characteristic wavelength at said second end of said laser rod, said output radiation being at a greater intensity than, and at the same wavelength as, said source radiation, whereby said source radiation is amplified.
Claim 3
Dependent Claim
12 words
The laser amplifier of claim 1, wherein said laser rod is ZnS.
Claim 4
Dependent Claim
15 words
The laser amplifier of claim 1, wherein said source of radiation is a dye laser.
Claim 5
Dependent Claim
14 words
The laser amplifier of claim 1, wherein said pumping means comprises a flash lamp.
Claim 6
Dependent Claim
14 words
The laser amplifier of claim 4, wherein said flash lamp is a Xenon lamp.
Claim 7
Dependent Claim
16 words
The laser amplifier of claim 1, wherein said source of radiation is an intermittent, pulsed source.
Claim 8
Dependent Claim
12 words
The laser amplifier of claim 4, wherein said pumping means is intermittent.
Claim 9
Dependent Claim
43 words
The laser amplifier of claim 7, wherein said means for alternately activating said pumping means and said source of radiation comprises modulator means connected to said pumping means for activating said pumping means τ radians out of phase with said source of radiation.
Claim 10
Dependent Claim
36 words
The laser amplifier of claim 8, further including power supply means connected to drive said pumping means, said modulator means triggering said power supply to produce an alternating on and off profile for said pumping means.
Claim 11
Dependent Claim
23 words
The laser amplifier of claim 9 wherein the period of said modulator means is on the order of a lifetime of an exciton.
Claim 12
Dependent Claim
18 words
The laser amplifier of claim 10, wherein the period of said modulator means is approximately 10 -6 sec.
Claim 13
Dependent Claim
25 words
The laser amplifier of claim 11, wherein said laser rod is at about the temperature of liquid helium to enhance the nonboson quality of excitons.
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USPTO Annuity & Maintenance Windows
| Annuity Stage | Window Opens | Payment Deadline | Surcharge Period Until | Estimated Fee | Status |
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| 3.5 Years (Year 4) | 1989-12-01 | 1990-06-02 | 1990-12-02 | $2000.00 | Window Closed / Lapsed |
| 7.5 Years (Year 8) | 1993-12-01 | 1994-06-02 | 1994-12-02 | $3760.00 | Window Closed / Lapsed |
| 11.5 Years (Year 12) | 1997-12-01 | 1998-06-02 | 1998-12-02 | $7700.00 | Window Closed / Lapsed |