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US4626792A Expired / Lapsed US ⏱️ 0.0 years remaining

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
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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.

References Cited (Backward Citations)

US3142760A Cited
US3292102A Cited
US3312905A Cited
US3333206A Cited
US3484714A Cited
US3513402A Cited
US4081764A Cited
US3991386A Cited
US4205329A Cited
US4490822A Cited
US4528464A Cited

USPTO Annuity & Maintenance Windows

Annuity Stage Window Opens Payment Deadline Surcharge Period Until Estimated Fee Status
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

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