US5822097A
Expired / Lapsed
US
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Linear extension device for coherent optical wave pulses and extension and compression device used to obtain high power pulses
Assignee: Thales SA
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Filing: 1994-11-07
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Granted: 1998-10-13
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Expires: 2014-11-07
Abstract
Abstract A device for linearly extending the duration of laser light pulses by subjecting the pulses to double diffraction based on a series of variable step gratings placed at right angles to each other. Increased power density is obtained by placing a compression grating at an angle such that each wavelength of light emerging from the compression grating travels an optical path of approximately the same distance, and focusing the emerging light with a lens. Increased amplification is obtained by placing a segmented laser amplifier, one segment aligned with each wavelength of light separated by the double diffraction of the series of variable step gratings and interposed between the series of variable step gratings and the compression grating.
Inventors
- 👤 Pierre Tournois
Bibliographic Details
Application Number
—
Jurisdiction
US
Data Source
google_patents
Last Synchronized
2026-11-06 16:11
CPC Classifications
G; G02; G02B; G02B27/00; G02B27/42; G02B27/4272; G02B27/4277; G02B27/4233; H; H01; H01S; H01S3/00; H01S3/005; H01S3/0057
Claims Analysis
Total Claims: 6
Claim 1
Independent Claim
205 words
A linear extension device for coherent optical wave pulses in a given frequency band Δf comprising a first and a second optical grating, each grating having steps (a i ) defined at different points of each grating, each point of each optical grating being located a distance (d i ) from the other grating, materials transparent to said optical wave pulses having a surface to locate said optical gratings, wherein said gratings are perpendicular to one another and each respective step is inversely proportional to the distance from the point where the respective step is defined to said other grating satisfying a relationship such that: a.sub.1 d.sub.1 =a.sub.2 d.sub.2 =Kc.sup.2 where K is a constant and where c is the speed of light between the gratings, said gratings involving a combined diffraction which linearly frequency disperses in time, a pulse incident at right angles to said first optical grating and emergent from said second grating at right angles to it as a beam, and wherein said emergent beam has frequencies which are delayed with a delay time which varies linearly with each respective frequency to produce a long pulse duration T which satisfies a relationship such that: t.sub.r =K/p f.sub.i where p is an integer.
Claim 2
Dependent Claim
205 words
A linear extension device for coherent optical wave pulses in a given frequency band Δf comprising a first and a second optical grating, each grating having steps (a i ) defined at different points of each grating, each point of each optical grating being located a distance (d i ) from the other grating, materials transparent to said optical wave pulses having a surface to locate said optical gratings, wherein said gratings are perpendicular to one another and each respective step is inversely proportional to the distance from the point where the respective step is defined to said other grating satisfying a relationship such that: a.sub.1 d.sub.1 =a.sub.2 d.sub.2 =Kc.sup.2 where K is a constant and where c is the speed of light between the gratings, said gratings involving a combined diffraction which linearly frequency disperses in time, a pulse incident at right angles to said first optical grating and emergent from said second grating at right angles to it as a beam, and wherein said emergent beam has frequencies which are delayed with a delay time which varies linearly with each respective frequency to produce a long pulse duration T which satisfies a relationship such that: t.sub.r =K/p f.sub.i where p is an integer.
Claim 3
Dependent Claim
96 words
A device as in claim 1, further comprising: a third compression grating disposed at an output of said second grating to compress in time waves of said emergent beam of diameter D, said third grating being inclined at an angle φ with respect to said surface of said second grating such that: ##EQU8## and having a step a i at every point of incidence of said emergent beam satisfying a relationship such that: a.sub.i dco.sup.2 φ=Kc.sup.2, where d is the distance between a respective point of incidence of said emergent beam and a point of reference.
Claim 4
Dependent Claim
119 words
A device as in claim 1, further comprising: a third optical grating disposed as a continuation of said first optical grating on the same surface, such that said third optical grating and said second optical grating form a perpendicular grating pair delay line similar to said first and second optical gratings of the extension device, said steps of said gratings satisfying a relation such that: a.sub.1 d.sub.1 =2a.sub.2 d.sub.2 =a.sub.3 d.sub.3 =Kc.sup.2 wherein a 1 , a 2 and a 3 are steps respectively defined on said first, second, and third optical gratings at points which are respectively a distance of d 1 , d 2 and d 3 from a point located at an intersection of these gratings.
Claim 5
Dependent Claim
44 words
A device as claimed in claim 2, further comprising: a laser amplifier disposed in a space between the surface of said second grating and that of said third grating; and a lens for focusing a beam emerging at right angles to said third grating.
Claim 6
Dependent Claim
43 words
A device as claimed in claim 4, wherein said laser amplifier is segmented into a series of amplifiers with frequency-selective mirrors disposed according to a spatial dispersion pattern corresponding to that of frequencies f i of said beam emerging from said second grating.
References Cited (Backward Citations)
No citation records indexed.
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