Patent US4126033A successfully refreshed from Google Patents.
US4126033A
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US
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Determination of thermal conductances of bonding layers in infrared photoconductor arrays
Assignee: United States Department of the Navy
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Filing: 1977-06-23
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Granted: 1978-11-21
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Expires: 1997-06-23
Abstract
Abstract A method for determining in situ the thermal conductances of bonding layers of detectors in infrared detector arrays for quality selection of preferred detector arrays. Each detector of the array is heated successively by laser pulses of variable pulse width and the thermally-induced change in detector resistance is measured as a function of time after each laser pulse and converted directly to its corresponding temperature. Using measured values of detector resistance as a function of temperature for each detector, one can obtain the time-dependence of the detector temperature following each laser pulse for each detector of the array.
Inventors
- 👤 Filbert J. Bartoli
- 👤 Leon Esterowitz
- 👤 Roger E. Allen
- 👤 Melvin R. Kruer
Bibliographic Details
Application Number
—
Jurisdiction
US
Data Source
google_patents
Last Synchronized
2026-10-29 19:15
CPC Classifications
G; G01; G01R; G01R27/00; G01R27/02; G01K; G01K7/00; G01K7/16; G01K7/22; G01N; G01N25/00; G01N25/18; G01R31/00
Claims Analysis
Total Claims: 2
Claim 1
Independent Claim
314 words
A method of determining in-site the thermal conductances of bonding layers of IR detectors in a test array of infrared detectors which comprises: simultaneously scanning all detectors of said array with a laser beam having a specific intensity such that said laser beam dwells on each detector of said array for a set time duration; setting the incident laser beam intensity to zero; recording the temperature of each of said detectors and the time at said zero intensity setting; continuously recording the time and temperature change of each of said detectors from said zero setting until the initial preheated temperature is reached to obtain a thermal recovery curve of each of said detectors; comparing the recorded thermal recovery curve for each of said detectors with a calculated family of thermal recovery curves using like laser intensities and beam duration and thermal conductances of different bonding layers employed in fabricating said detectors of said array thereby obtaining from said comparison individual thermal conductances of each of said bonding layers of said array of detectors; repeating said heat-record steps for other laser beam intensities and time durations of incidence to obtain a family of thermal recovery curves for each of said detectors at different laser beam intensities and time durations; comparing the measured and calculated thermal recovery curves for each of said laser beam intensities and laser beam durations to determing the optimum laser intensity and beam duration for determining the thermal conductance of a first bonding layer of each of said detectors; said optimum laser beam intensity and pulse duration being different for each of said detectors; repeating said latter comparison step for determing the thermal conductance of a second bonding layer of each of said detectors; whereby the thermal conductances of said first and second bonding layers are derived from said optimum laser intensities and pulse durations obtained separately for each of said layers.
Claim 2
Independent Claim
314 words
A method of determining in-site the thermal conductances of bonding layers of IR detectors in a test array of infrared detectors which comprises: simultaneously scanning all detectors of said array with a laser beam having a specific intensity such that said laser beam dwells on each detector of said array for a set time duration; setting the incident laser beam intensity to zero; recording the temperature of each of said detectors and the time at said zero intensity setting; continuously recording the time and temperature change of each of said detectors from said zero setting until the initial preheated temperature is reached to obtain a thermal recovery curve of each of said detectors; comparing the recorded thermal recovery curve for each of said detectors with a calculated family of thermal recovery curves using like laser intensities and beam duration and thermal conductances of different bonding layers employed in fabricating said detectors of said array thereby obtaining from said comparison individual thermal conductances of each of said bonding layers of said array of detectors; repeating said heat-record steps for other laser beam intensities and time durations of incidence to obtain a family of thermal recovery curves for each of said detectors at different laser beam intensities and time durations; comparing the measured and calculated thermal recovery curves for each of said laser beam intensities and laser beam durations to determing the optimum laser intensity and beam duration for determining the thermal conductance of a first bonding layer of each of said detectors; said optimum laser beam intensity and pulse duration being different for each of said detectors; repeating said latter comparison step for determing the thermal conductance of a second bonding layer of each of said detectors; whereby the thermal conductances of said first and second bonding layers are derived from said optimum laser intensities and pulse durations obtained separately for each of said layers.
References Cited (Backward Citations)
USPTO Annuity & Maintenance Windows
| Annuity Stage | Window Opens | Payment Deadline | Surcharge Period Until | Estimated Fee | Status |
|---|---|---|---|---|---|
| 3.5 Years (Year 4) | 1981-11-20 | 1982-05-22 | 1982-11-21 | $2000.00 | Window Closed / Lapsed |
| 7.5 Years (Year 8) | 1985-11-20 | 1986-05-22 | 1986-11-21 | $3760.00 | Window Closed / Lapsed |
| 11.5 Years (Year 12) | 1989-11-20 | 1990-05-22 | 1990-11-21 | $7700.00 | Window Closed / Lapsed |