Patent US4846561A successfully refreshed from Google Patents.
← Back to Patent Explorer
US4846561A Expired / Lapsed US ⏱️ 0.0 years remaining

Monolithic optical power limiter based on two-photon absorption

Assignee: CENTER FOR RESEARCH IN ELECTRO-OPTICS AND LASERS (CREOL)
•
Filing: 1988-06-21
•
Granted: 1989-07-11
•
Expires: 2008-06-21
📄 Original PDF 🌐 Google Patents 🔄 Sync Now

Abstract

Abstract Collimated incident optical radiation which might contain high-intensity or high-power radiation is focused into the body of a limiter by a first lens formed at one end of the limiter. The body is a cylinder of revolution with an axis along the optical axis between radiation and a sensitive detector. Radiation of normal intensity or power freely passes through the body and is recollimated by a second lens formed at the other end of the limiter from the first lens. The body is made of material which is subject to two-photon absorption such that high-intensity or high-power radiation undergoes absorption and is consequently self-defocused such that it is diverted from the optical path. For visible light, the material may be ZeSe or ZnS; for ultraviolet, copper chloride; for infrared, HgCgTe.

Inventors

  • 👤 Marion J. Soileau, Jr.
  • 👤 Eric W. Van Stryland

Bibliographic Details

Application Number —
Jurisdiction US
Data Source google_patents
Last Synchronized 2026-10-31 02:21
CPC Classifications
G; G02; G02B; G02B5/00; G02B5/20; G02B5/22; G02B5/23; G02F; G02F1/00; G02F1/35; G02F1/3526

Claims Analysis

Total Claims: 8
Claim 1
Independent Claim 156 words
A unitary device for protecting a sensitive optical detector from high-power or high-intensity radiation of a particular wavelength or band of wavelengths, wherein said device is in the form of a cooled cylindrical body with a longitudinal axis and with positive lenses on either end of said body along said axis, whereby said body is made of a material subject to two-photon absorption of incident radiation and is chosen from the group consisting of: ZnSe, ZnS, copper chloride, and Hg 1-x Cd x Te, and whereby said body is placed with its axis colinear with the optical axis is an optical system such that incident radiation below a threshold intensity or power level mostly transmits through said body but incident radiation above said level undergoes two-photon absorption with consequent self-defocusing in said body whereby the self-defocussed radiation is diverted from said detector, and the radiation which transmits through said body is limited to said threshold level.
Claim 2
Dependent Claim 156 words
A unitary device for protecting a sensitive optical detector from high-power or high-intensity radiation of a particular wavelength or band of wavelengths, wherein said device is in the form of a cooled cylindrical body with a longitudinal axis and with positive lenses on either end of said body along said axis, whereby said body is made of a material subject to two-photon absorption of incident radiation and is chosen from the group consisting of: ZnSe, ZnS, copper chloride, and Hg 1-x Cd x Te, and whereby said body is placed with its axis colinear with the optical axis is an optical system such that incident radiation below a threshold intensity or power level mostly transmits through said body but incident radiation above said level undergoes two-photon absorption with consequent self-defocusing in said body whereby the self-defocussed radiation is diverted from said detector, and the radiation which transmits through said body is limited to said threshold level.
Claim 3
Dependent Claim 22 words
The device as set forth in claim 1 wherein the length of said body is twice the focal length of said lenses.
Claim 4
Dependent Claim 37 words
The device as set forth in claim 1 wherein x is determined from the following formula: Eg=-0.302+1.93x+5.35(10.sup.-4)T(1-2x)-0.810x.sup.2 +0.832x.sup.3 and wherein Eg is the energy gap corresponding to said particular wavelength and T is temperature in degrees Kelvin.
Claim 5
Dependent Claim 37 words
The device as set forth in claim 2 wherein x is determined from the following formula: Eg=-0.302+1.93x+5.35(10.sup.-4)T(1-2x)-0.810x.sup.2 +0.832x.sup.3 and wherein Eg is the energy gap corresponding to said particular wavelength and T is temperature in degrees Kelvin.
Claim 6
Dependent Claim 117 words
A unitary device for protecting a sensitive optical detector from high-power or high-intensity radiation of a particular wavelength or band of wavelengths, wherein the device is of a cooled material subject to two-photon absorption of incident radiation and wherein the material is a body of revolution with a length L along an optical axis between said radiation and said detector, and includes a first end formed as a lens for focusing collimated incident radiation as a spot into said body, and a second end formed as a lens for recollimating radiation which transmits through said body onto said detector, whereby high-power or high-intensity radiation of said particular wavelength or band of wavelengths is self-defocused by said material.
Claim 7
Dependent Claim 117 words
A unitary device for protecting a sensitive optical detector from high-power or high-intensity radiation of a particular wavelength or band of wavelengths, wherein the device is of a cooled material subject to two-photon absorption of incident radiation and wherein the material is a body of revolution with a length L along an optical axis between said radiation and said detector, and includes a first end formed as a lens for focusing collimated incident radiation as a spot into said body, and a second end formed as a lens for recollimating radiation which transmits through said body onto said detector, whereby high-power or high-intensity radiation of said particular wavelength or band of wavelengths is self-defocused by said material.
Claim 8
Dependent Claim 29 words
The device as set forth in claim 5 wherein said lenses have the same focal length and wherein L is equal to twice the focal length of each lens.

References Cited (Backward Citations)

US3395961A Cited
US3790252A Cited
US4410239A Cited
US4776677A Cited

USPTO Annuity & Maintenance Windows

Annuity Stage Window Opens Payment Deadline Surcharge Period Until Estimated Fee Status
3.5 Years (Year 4) 1992-07-10 1993-01-09 1993-07-11 $2000.00 Window Closed / Lapsed
7.5 Years (Year 8) 1996-07-10 1997-01-09 1997-07-11 $3760.00 Window Closed / Lapsed
11.5 Years (Year 12) 2000-07-10 2001-01-09 2001-07-11 $7700.00 Window Closed / Lapsed

Assigned Categories & Tags

No categories assigned to this patent yet.

Assign Category Tag