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US5049734A Expired / Lapsed US ⏱️ 0.0 years remaining

Method for determining petal piston in a segmented imaging system

Assignee: Exelis Inc
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Filing: 1990-08-23
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Granted: 1991-09-17
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Expires: 2010-08-23
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Abstract

Abstract A method for determining petal piston in a segmented optical imaging system. The system preferably comprises a center mirror and a set of P petals adjacent to the center mirror. The novel method is suitable for determining petal piston for each of the P petals, with respect to the center mirror, or with respect to each other. To this end, the novel method employs a three-part masking scheme, to simulate zero, positive and negative piston error, in order to develop a referrent as a measure of actual piston error.

Inventors

  • 👤 Philip F. Marino

Bibliographic Details

Application Number —
Jurisdiction US
Data Source google_patents
Last Synchronized 2026-11-09 05:15
CPC Classifications
G; G01; G01J; G01J9/00

Claims Analysis

Total Claims: 8
Claim 1
Independent Claim 453 words
In an imaging system for imaging scene radiation comprising a center mirror and a set of P petals adjacent to the center mirror, a method for determining petal piston for each of the P petals, the method comprising the steps of: 1) separating scene radiation into replicate first, second and third scene radiation beams; 2) processing the first scene radiation beam by (i) dividing the first scene radiation beam into p discrete beams, in correspondence to p areas of the imaging system, such that each area p overlaps a portion of one of the P petals and a portion of the center mirror; (ii) adding or subtracting zero path length difference to that component of each of the p discrete beams that exits the petal relative to that component which exits the center mirror, for creating p discrete zero piston beams; and (iii) outputting the p discrete zero piston beams; 3) processing the second scene radiation beam by (i) dividing the second scene radiation beam into p discrete beams, in correspondence to p areas of the imaging system, such that each area p overlaps a portion of one of the P petals and a portion of the center mirror; (ii) adding path length to that component of each of the p discrete beams that exits the petal relative to that component which exits the center mirror, for creating p discrete positive piston beams; and (iii) outputting the p discrete positive piston beams; 4) processing the third scene radiation beam by (i) dividing the third scene radiation beam into p discrete beams, in correspondence to p areas of the imaging system, such that each area p overlaps a portion of one of the P petals and a portion of the center mirror; (ii) adding path length to that component of each of the p discrete beams that exits the center mirror relative to that component which exits the petal, for creating p discrete negative piston beams; and (iii) outputting the p discrete negative piston beams; 5) photodetecting each of the p discrete zero piston beams, for measuring p discrete variance of intensity magnitude., 6) photodetecting each of the p discrete positive piston beams, for measuring p discrete variance of intensity magnitude; 7) photodetecting each of the p discrete negative piston beams, for measuring p discrete variance of intensity magnitude; and 8) determining petal piston for each of the P petals by (i) generating a petal parabolic function by specifying at least three independent variables derived from steps 5, 6 and 7 respectively, the variables thus comprising the magnitudes of the variance of intensity of the zero, positive, and negative piston beams; and (ii) computing a parabolic function maximum as a measure of petal piston.
Claim 2
Dependent Claim 453 words
In an imaging system for imaging scene radiation comprising a center mirror and a set of P petals adjacent to the center mirror, a method for determining petal piston for each of the P petals, the method comprising the steps of: 1) separating scene radiation into replicate first, second and third scene radiation beams; 2) processing the first scene radiation beam by (i) dividing the first scene radiation beam into p discrete beams, in correspondence to p areas of the imaging system, such that each area p overlaps a portion of one of the P petals and a portion of the center mirror; (ii) adding or subtracting zero path length difference to that component of each of the p discrete beams that exits the petal relative to that component which exits the center mirror, for creating p discrete zero piston beams; and (iii) outputting the p discrete zero piston beams; 3) processing the second scene radiation beam by (i) dividing the second scene radiation beam into p discrete beams, in correspondence to p areas of the imaging system, such that each area p overlaps a portion of one of the P petals and a portion of the center mirror; (ii) adding path length to that component of each of the p discrete beams that exits the petal relative to that component which exits the center mirror, for creating p discrete positive piston beams; and (iii) outputting the p discrete positive piston beams; 4) processing the third scene radiation beam by (i) dividing the third scene radiation beam into p discrete beams, in correspondence to p areas of the imaging system, such that each area p overlaps a portion of one of the P petals and a portion of the center mirror; (ii) adding path length to that component of each of the p discrete beams that exits the center mirror relative to that component which exits the petal, for creating p discrete negative piston beams; and (iii) outputting the p discrete negative piston beams; 5) photodetecting each of the p discrete zero piston beams, for measuring p discrete variance of intensity magnitude., 6) photodetecting each of the p discrete positive piston beams, for measuring p discrete variance of intensity magnitude; 7) photodetecting each of the p discrete negative piston beams, for measuring p discrete variance of intensity magnitude; and 8) determining petal piston for each of the P petals by (i) generating a petal parabolic function by specifying at least three independent variables derived from steps 5, 6 and 7 respectively, the variables thus comprising the magnitudes of the variance of intensity of the zero, positive, and negative piston beams; and (ii) computing a parabolic function maximum as a measure of petal piston.
Claim 3
Dependent Claim 20 words
A method according to claim 1, wherein step 2 comprises processing the first scene radiation beam at an exit pupil.
Claim 4
Dependent Claim 28 words
A method according to claim 2, where step 2 comprises employing a single unit pupil mask comprising dividing, adding and outputting functions for creating discrete zero piston beams.
Claim 5
Dependent Claim 20 words
A method according to claim 1, wherein step 3 comprises processing the second scene radiation beam at an exit pupil.
Claim 6
Dependent Claim 28 words
A method according to claim 4, wherein step 3 comprises employing a single unit pupil mask comprising dividing, adding and outputting functions for creating discrete positive piston beams.
Claim 7
Dependent Claim 20 words
A method according to claim 1, wherein step 4 comprises processing the third scene radiation beam at an exit pupil.
Claim 8
Dependent Claim 28 words
A method according to claim 6, wherein step 4 comprises employing a single unit pupil mask comprising dividing, adding and outputting functions for creating discrete negative piston beams.

References Cited (Backward Citations)

US4518854A Cited
WO1988009488A1 Cited
US4959532A Cited

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