ํŒ๋…์ถœ๋ ฅํ†ตํ•ฉํšŒ๋กœ (ROIC)

Teledyne FLIR ํŒ๋… ์ง‘์  ํšŒ๋กœ(ROIC) ์ œํ’ˆ์€ ๊ทผ๊ฑฐ๋ฆฌ, ์ค‘๊ฑฐ๋ฆฌ ๋ฐ ์žฅ๊ฑฐ๋ฆฌ ํŒŒ์žฅ ์ ์™ธ์„  ๊ฒ€์ถœ๊ธฐ๋ฅผ ์‚ฌ์šฉํ•˜์—ฌ ๊ฐ€์žฅ ๊นŒ๋‹ค๋กœ์šด ๋น„์ „ ์‹œ์Šคํ…œ ์• ํ”Œ๋ฆฌ์ผ€์ด์…˜์„ ์œ„ํ•œ ๊ธฐ์„ฑ ์†”๋ฃจ์…˜์„ ์ œ๊ณตํ•ฉ๋‹ˆ๋‹ค. ๊ฐ„๋‹จํ•œ ์‚ฌ์šฉ์ž ์ธํ„ฐํŽ˜์ด์Šค๋ฅผ ํ†ตํ•ด ์š”๊ตฌ ์‚ฌํ•ญ์— ๋”ฐ๋ผ ์ €์†Œ์Œ, ๊ฐ€๋ณ€ ์ „ํ•˜ ์ €์žฅ ์šฉ๋Ÿ‰, ์„ ํƒ ๊ฐ€๋Šฅํ•œ ํ†ตํ•ฉ ์‹œ๊ฐ„, ์กฐ์ • ๊ฐ€๋Šฅํ•œ ์ด๋“ ๋ฐ ์ „๋ ฅ ์„ค์ •์ด ํ•„์š”ํ•œ ๊ฒฝ์šฐ, ๋‹น์‚ฌ์˜ ํ˜ผํ•ฉ ์‹ ํ˜ธ ROIC๋Š” ์„ฑ๋Šฅ์ด๋‚˜ ์œ ์—ฐ์„ฑ์„ ํ›ผ์†ํ•˜์ง€ ์•Š์œผ๋ฉด์„œ ์™„์ „ ๋งž์ถคํ˜• ์„ค๊ณ„์— ๋Œ€ํ•œ ์ž…์ฆ๋œ ๋น„์šฉ ํšจ์œจ์ ์ธ ๋Œ€์•ˆ์„ ์ œ์‹œํ•ฉ๋‹ˆ๋‹ค.

๊ฐ„ํŽธํ•œ ํ†ตํ•ฉ

๊ฐ„ํŽธํ•œ ํ†ตํ•ฉ

์ œํ’ˆ ํ•„ํ„ฐ

๋ชจ๋“  ์ œํ’ˆ (5) ๊ทธ๋ฆฌ๋“œ๋ทฐ ๊ทธ๋ฆฌ๋“œ๋ทฐ ๋ฆฌ์ŠคํŠธ๋ทฐ ๋ฆฌ์ŠคํŠธ๋ทฐ

FLIR ISC0403

์•ˆํ‹ฐ๋ชฌํ™” ์ธ๋“ (InSb), 640 x 512์‹, 15 ๋ฏธํฌ๋ก  ํ”ผ์น˜

ISC0403์€ 15-๋ฏธํฌ๋ก  ํ”ฝ์…€ ํ”ผ์น˜๋ฅผ ๊ฐ–์ถ˜ ๋Œ€ํ˜• ROIC์ž…๋‹ˆ๋‹ค. P-์˜จ-N ์•ˆํ‹ฐ๋ชฌํ™” ์ธ๋“ (InSb) ๋””ํ…ํ„ฐ์™€ ํ•จ๊ป˜ ์‚ฌ์šฉ๋˜๋Š” ์ด 640x512 ๋ฐฐ์—ด์€ ์œˆ๋„์ž‰, ์ด๋ฏธ์ง€ ์ „์œ„, ์กฐ์ •์‹ ๊ฒŒ์ธ (Adjustable gain), ์Šค๋ƒ… ์ƒท ํ†ตํ•ฉ ์„ค์น˜ ํ›„ ํŒ๋… ๋ฐ ํ†ตํ•ฉ ์„ค์น˜ ์ค‘ ํŒ๋… ๋“ฑ ํ‘œ์ค€ํ˜• ์ œํ’ˆ๊ณผ ๋™์ผํ•œ ๊ณ ๊ธ‰ ๊ธฐ๋Šฅ์„ ์ œ๊ณตํ•ฉ๋‹ˆ๋‹ค. ์•„์šธ๋Ÿฌ, ์ „๋ ฅ ์กฐ์ •, ๋‹ค์ค‘ ์ถœ๋ ฅ ์ฑ„๋„์„ ์ œ๊ณตํ•˜์—ฌ ํ’€ ํ”„๋ ˆ์ž„์œผ๋กœ ์ž‘๋™ ํ•  ๋•Œ์—๋Š” ์ตœ๋Œ€ ์ดˆ๋‹น 120 ํ”„๋ ˆ์ž„, ๋ณด๋‹ค ์ž‘์€ ์œˆ๋„์šฐ ํฌ๊ธฐ๋กœ ์ž‘๋™ ํ•  ๋•Œ์—๋Š” ์ดˆ๋‹น 2054 ํ”„๋ ˆ์ž„์˜ ๋ฐ์ดํ„ฐ ์ฒ˜๋ฆฌ ์†๋„๋ฅผ ์ง€์›ํ•ฉ๋‹ˆ๋‹ค. ์ „ํ•˜ ์šฉ๋Ÿ‰์€ >6.5 e6 ์ „์ž์ด๋ฉฐ, ํŽธํ–ฅ ๋ณด์ •์€ 600mV์ž…๋‹ˆ๋‹ค.

FLIR ISC1202

์ธ๋“๊ฐˆ๋ฅจ๋น„์†Œ (InGaAs), 640 x 512์‹, 15 ๋ฏธํฌ๋ก  ํ”ผ์น˜

ISC1202๋Š” 640 × 512 ํฌ๋งท, 15๋ฏธํฌ๋ก  ํ”ผ์น˜ ROIC๋กœ, ๋‚ฎ์€ ๋ฐฑ๊ทธ๋ผ์šด๋“œ ์• ํ”Œ๋ฆฌ์ผ€์ด์…˜์— ์ตœ์ ํ™”๋˜์—ˆ์Šต๋‹ˆ๋‹ค. CTIA ํ”„๋ก ํŠธ ์—”๋“œ ํšŒ๋กœ๋ฅผ ์‚ฌ์šฉํ•˜๋ฉฐ ํ•˜์ด ๊ฒŒ์ธ ๋ชจ๋“œ์˜ ํŒ๋… ๋…ธ์ด์ฆˆ๋Š” 35 ์ผ๋ ‰ํŠธ๋ก  ๋ฏธ๋งŒ์ž…๋‹ˆ๋‹ค. InGaAs, SLS ๋ฐ MCT์™€ ๊ฐ™์€ P-on-N ๊ฐ์ง€๊ธฐ์™€ ํ˜ธํ™˜๋˜๋Š” ์ด ๋Œ€ํ˜• ROIC๋Š” ๋‹ค๋ฅธ ํ‘œ์ค€ ROIC์™€ ๋™์ผํ•œ ๊ณ ๊ธ‰ ๊ธฐ๋Šฅ, ์Šค๋ƒ…์ƒท ๋ชจ๋“œ, ์กฐ์ • ๊ฐ€๋Šฅํ•œ ํ†ตํ•ฉ ์‹œ๊ฐ„ ๋ฐ ์ด๋“, ์ „์› ๋ฐ ์ „๋ฅ˜ ์กฐ์ •, 3๊ฐœ์˜ ์„ ํƒ ๊ฐ€๋Šฅํ•œ ํ†ตํ•ฉ ์บํŒจ์‹œํ„ฐ(41K, 118K ๋˜๋Š” 1.38M ์ „์ž)๋ฅผ ์ถ”๊ฐ€๋กœ ์ง€์›ํ•ฉ๋‹ˆ๋‹ค.

FLIR ISC1308

์ด์›์  ๊ทน์„ฑ 2-์ปฌ๋Ÿฌ์‹, HD 1280 x 1024, 12 ๋ฏธํฌ๋ก  ํ”ผ์น˜

ISC 1308์€ ์ด์›์  ๊ทน์„ฑ, 2-์ปฌ๋Ÿฌ์‹, HD์‹, 1280 x 1024, 12 ๋ฏธํฌ๋ก  ํ”ผ์น˜ ํŒ๋…์ถœ๋ ฅํ†ตํ•ฉํšŒ๋กœ (ROIC) ์ œํ’ˆ์ž…๋‹ˆ๋‹ค.

FLIR ISC1901

Mega-pixel 2K × 1.5K readout integrated circuit (ROIC) optimized for Indium Antimonide (InSb), Type-II strained-layer superlattice (T2SLS) and Quantum Well (QWIP) infrared detectors

The ISC1901 is a 2048 × 1536 format, 10-micron pitch device designed for P-on-N detectors with a direct injection input circuit. The ISC1901 supports single sample or sub-frame averaging for effective well fill of 3 to 19M electrons, respectively. The selectable settings allow user control of modes such as 2 × 2 binning, 8 or 16 output channels and additional reverse bias for QWIP detectors. Teledyne FLIR’s familiar user interface makes system integration straightforward.

FLIR ISC1902

Mega-pixel 2K × 2K readout integrated circuit (ROIC) optimized for Indium Antimonide (InSb), Type-II strained-layer superlattice (T2SLS) and Quantum Well (QWIP) infrared detectors

The ISC1902 is a 2048 × 2048 format, 10-micron pitch device designed for P-on-N detectors with a direct injection input circuit. The ISC1902 is the big brother to the ISC1901 and supports all the same features with higher resolution. This includes single sample or sub-frame averaging for effective well fill of 3 to 19M electrons, respectively. The selectable settings allow user control of modes such as 2 × 2 binning, 8 or 16 output channels and additional reverse bias for QWIP detectors. Teledyne FLIR’s familiar user interface makes system integration straightforward.

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