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ํŒ๋…์ถœ๋ ฅํ†ตํ•ฉํšŒ๋กœ (ROIC) - 2์ฐจ์› ํŒ๋…์ถœ๋ ฅํ†ตํ•ฉํšŒ๋กœ (ROIC)

๋ชจ๋“  ์ œํ’ˆ (18) ๊ทธ๋ฆฌ๋“œ๋ทฐ ๊ทธ๋ฆฌ๋“œ๋ทฐ ๋ฆฌ์ŠคํŠธ๋ทฐ ๋ฆฌ์ŠคํŠธ๋ทฐ

FLIR ISC9705

InSb(Indium Antimonide), Type-II strained-layer superlattice(T2SLS) ๋ฐ Quantum Well(QWIP) ์ ์™ธ์„  ๊ฐ์ง€๊ธฐ์— ์ตœ์ ํ™”๋œ ๋ฏธ๋“œ ํฌ๋งท ํŒ๋… ์ง‘์  ํšŒ๋กœ(ROIC)์ž…๋‹ˆ๋‹ค.

ISC9705๋Š” ์‹œ์žฅ์— ์ถœ์‹œ๋œ ์ตœ์ดˆ์˜ ๊ธฐ์„ฑํ’ˆ ํ‘œ์ค€ ๋ฉ€ํ‹ฐํ”Œ๋ ‰์„œ์˜€์Šต๋‹ˆ๋‹ค. 1997๋…„ 10์›” ๋„์ž…๋œ ์ด๋ž˜ ์ „์„ธ๊ณ„์˜ ํƒ์ง€๊ธฐ ์ œ์กฐ์—…์ฒด๋“ค์€ ์ ์™ธ์„  ์ดˆ์ ๋ฉด ์–ด๋ ˆ์ด ์ œ์ž‘์šฉ์œผ๋กœ ISC9705๋ฅผ ๊ตฌ์ž…ํ•ด ์™”์Šต๋‹ˆ๋‹ค. ์ด ๊ณ ์„ฑ๋Šฅ์˜ 320 × 256ํ”ฝ์…€, 30๋ฏธํฌ๋ก  ํ”ผ์น˜ ํŒ๋… ํ†ตํ•ฉ ํšŒ๋กœ๋Š” 6์ธ์น˜ ์›จ์ดํผ ํ˜•ํƒœ๋กœ ์ œ๊ณต๋˜๋Š” ์„œ๋ธŒ๋ฏธํฌ๋ก  CMOS(complementary metal-oxide-silicon) ๊ณต์ •์„ ์‚ฌ์šฉํ•˜์—ฌ ์ œ์ž‘๋˜์—ˆ์Šต๋‹ˆ๋‹ค. ์žฅ์น˜๋Š” ํ…Œ์ŠคํŠธ๋ฅผ ๊ฑฐ์ณ ๊ด‘๋ฒ”์œ„ํ•œ ์‚ฌ์šฉ์ž ์„ค๋ช…์„œ์™€ ํ•จ๊ป˜ ์›จ์ดํผ ํ˜•ํƒœ๋กœ ๊ณ ๊ฐ์—๊ฒŒ ์ „๋‹ฌ๋ฉ๋‹ˆ๋‹ค.

์ œํ’ˆ ์ˆ˜๋ช… ์ข…๋ฃŒ ํ†ต์ง€

ํ•ด๋‹น ์ œํ’ˆ์„ ์ฃผ๋ฌธํ•  ์ˆ˜ ์žˆ๋Š” ํŒ๋งค ์ข…๋ฃŒ์ผ์€ 2024๋…„ 3์›” 18์ผ์ž…๋‹ˆ๋‹ค. ๊ณ ๊ฐ์€ 2025๋…„ 6์›” 30์ผ๊นŒ์ง€ Teledyne FLIR์˜ ์ง€์›์„ ๊ณ„์† ๋ฐ›์„ ์ˆ˜ ์žˆ์Šต๋‹ˆ๋‹ค. ์ž์„ธํ•œ ๋‚ด์šฉ์€ ์•„๋ž˜์˜ ์•Œ๋ฆผ์„ ์ฐธ์กฐํ•˜์‹ญ์‹œ์˜ค.

FLIR ISC9809

Indium Gallium Arsenide(InGaAs) ์ ์™ธ์„  ํƒ์ง€๊ธฐ์— ์ตœ์ ํ™”๋œ ๋ฏธ๋“œ ํฌ๋งท ํ†ตํ•ฉ ํšŒ๋กœ(ROIC)

ISC9809๋Š” 320 × 256 ํฌ๋งท, 30๋ฏธํฌ๋ก  ํ”ผ์น˜ ROIC๋กœ, ์ € ๋ฐฑ๊ทธ๋ผ์šด๋“œ ์• ํ”Œ๋ฆฌ์ผ€์ด์…˜์„ ์œ„ํ•ด ํŠน๋ณ„ํžˆ ์„ค๊ณ„๋˜์—ˆ์Šต๋‹ˆ๋‹ค. CTIA ํ”„๋ก ํŠธ ์—”๋“œ ํšŒ๋กœ๋ฅผ ์‚ฌ์šฉํ•˜๋ฉฐ ํ•˜์ด ๊ฒŒ์ธ ๋ชจ๋“œ์˜ ํŒ๋… ๋…ธ์ด์ฆˆ๋Š” 70 ์ผ๋ ‰ํŠธ๋ก  ๋ฏธ๋งŒ์ž…๋‹ˆ๋‹ค. ์ด ๋ฏธ๋“œ ํฌ๋งท ROIC๋Š” ๋‹ค๋ฅธ ํ‘œ์ค€ ROIC์™€ ๋™์ผํ•œ ๊ณ ๊ธ‰ ๊ธฐ๋Šฅ, ์Šค๋ƒ…์ƒท ๋ชจ๋“œ, ์กฐ์ • ๊ฐ€๋Šฅํ•œ ํ†ตํ•ฉ ์‹œ๊ฐ„ ๋ฐ ์ด๋“, ์Šคํ‚ค๋ฐ, ์ „์› ๋ฐ ์ „๋ฅ˜ ์กฐ์ •, ์„ ํƒ ๊ฐ€๋Šฅํ•œ ํ†ตํ•ฉ ์บํŒจ์‹œํ„ฐ(0.17M ๋˜๋Š” 3.5M ์ „์ž)๋ฅผ ์ถ”๊ฐ€๋กœ ์ง€์›ํ•ฉ๋‹ˆ๋‹ค.

์ œํ’ˆ ์ˆ˜๋ช… ์ข…๋ฃŒ ํ†ต์ง€

ํ•ด๋‹น ์ œํ’ˆ์„ ์ฃผ๋ฌธํ•  ์ˆ˜ ์žˆ๋Š” ํŒ๋งค ์ข…๋ฃŒ์ผ์€ 2024๋…„ 3์›” 18์ผ์ž…๋‹ˆ๋‹ค. ๊ณ ๊ฐ์€ 2025๋…„ 6์›” 30์ผ๊นŒ์ง€ Teledyne FLIR์˜ ์ง€์›์„ ๊ณ„์† ๋ฐ›์„ ์ˆ˜ ์žˆ์Šต๋‹ˆ๋‹ค. ์ž์„ธํ•œ ๋‚ด์šฉ์€ ์•„๋ž˜์˜ ์•Œ๋ฆผ์„ ์ฐธ์กฐํ•˜์‹ญ์‹œ์˜ค.

FLIR ISC0903

Mid-format, two-color, dual polarity readout integrated circuit (ROIC) optimized for Indium Antimonide (InSb), Type-II strained-layer superlattice (T2SLS) and Quantum Well (QWIP) infrared detectors.

The ISC0903 is a 320 × 256 format, 30-micron pitch, two-color, dual polarity ROIC. It is designed for use with p-on-n or n-on-p detectors such as strained-layer superlattice devices. It is based on the ISC9705 so the pixel pitch is identical and interface is similar. The ROIC has been specifically designed to allow for both polarities of detectors to be placed back-to-back and to connect to the ROIC through the one input pad to obtain a two-color image.

FLIR ISC0208

์œ ๋Ÿฝ์‹ ์•ˆํ‹ฐ๋ชฌํ™” ์ธ๋“ (InSb) & ์–‘์ž ์šฐ๋ฌผ ์ ์™ธ์„  ๊ด‘ ๊ฒ€์ถœ๊ธฐ (QWIP), 384 x 288 ํ˜•์‹, 25 ๋ฏธํฌ๋ก  ํ”ผ์น˜

ISC0208์€ ๊ณ ์„ฑ๋Šฅ, ์œ ๋Ÿฝํ˜•, 384 × 288 ํ˜•์‹, 25๋ฏธํฌ๋ก  ํ”ผ์น˜ ํŒ๋… ์ง‘์  ํšŒ๋กœ์ž…๋‹ˆ๋‹ค. QWIP ๊ฒ€์ถœ๊ธฐ์™€ ํ•จ๊ป˜ ์‚ฌ์šฉํ•˜๋„๋ก ์„ค๊ณ„๋œ 18M ์ „์ž ์›ฐ ์šฉ๋Ÿ‰์„ ๊ฐ€์ง„ -1๊ณผ InSb ๊ฒ€์ถœ๊ธฐ๋ฅผ ์œ„ํ•œ 13M ์ „์ž ์›ฐ ์šฉ๋Ÿ‰์„ ๊ฐ€์ง„ -2์˜ ๋‘ ๊ฐ€์ง€ ๋ฒ„์ „์ด ์ œ๊ณต๋ฉ๋‹ˆ๋‹ค. ISC0208์€ ์„œ๋ธŒ๋งˆ์ดํฌ๋ก  ์ƒ๋ณด์  ๊ธˆ์† ์‚ฐํ™”๋ฌผ ์‹ค๋ฆฌ์ฝ˜ ๊ณต์ •์„ ์‚ฌ์šฉํ•˜์—ฌ ์ œ์ž‘๋ฉ๋‹ˆ๋‹ค. ์žฅ์น˜๋Š” ์ผ๋ฐ˜์ ์œผ๋กœ 6์ธ์น˜ ์›จ์ดํผ ํ˜•ํƒœ๋กœ ์ œ๊ณต๋˜๋ฉฐ, ๊ฐ ์ œ๊ณตํ’ˆ์— ํฌํ•จ๋œ ๊ด‘๋ฒ”์œ„ํ•œ ์‚ฌ์šฉ์ž ์„ค๋ช…์„œ ๋ฐ ํ…Œ์ŠคํŠธ ๋ฐ์ดํ„ฐ๊ฐ€ ํฌํ•จ๋˜์–ด ์žˆ์Šต๋‹ˆ๋‹ค.

์ œํ’ˆ ์ˆ˜๋ช… ์ข…๋ฃŒ ํ†ต์ง€

ํ•ด๋‹น ์ œํ’ˆ์„ ์ฃผ๋ฌธํ•  ์ˆ˜ ์žˆ๋Š” ํŒ๋งค ์ข…๋ฃŒ์ผ์€ 2024๋…„ 3์›” 18์ผ์ž…๋‹ˆ๋‹ค. ๊ณ ๊ฐ์€ 2025๋…„ 6์›” 30์ผ๊นŒ์ง€ Teledyne FLIR์˜ ์ง€์›์„ ๊ณ„์† ๋ฐ›์„ ์ˆ˜ ์žˆ์Šต๋‹ˆ๋‹ค. ์ž์„ธํ•œ ๋‚ด์šฉ์€ ์•„๋ž˜์˜ ์•Œ๋ฆผ์„ ์ฐธ์กฐํ•˜์‹ญ์‹œ์˜ค.

FLIR ISC0402

Large format readout integrated circuit (ROIC) optimized for Indium Antimonide (InSb) and Quantum well infrared detectors

The ISC0402 is 640 × 512 format, 20-micron pixel ROIC. Itโ€™s compatible with P-on-N detectors such as InSb, QWIP, InGaAs, and MCT. It offers the same advanced features as our other standard designs including windowing, adjustable gain, interlaced/non-interlaced readout, power adjustment, and multiple output channels. Two versions of the design are available with different size integration capacitors 3.5M electrons for the smaller well and >6M electrons for the large well version.

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 ISC0905

Large format, dual band, dual polarity readout integrated circuit (ROIC) optimized for Indium Antimonide (InSb) and Type-II strained-layer superlattice (T2SLS) infrared detectors

The ISC0905 is a 640 ร— 512 format, 30-micron pitch, two-color, dual polarity device. It is designed for use with p-on-n or n-on-p detectors such as strained-layer superlattice devices. This large format device is based on the mid-format ISC0903 with the same pixel pitch and similar interface. The ROIC has been specifically designed to allow for both polarities of detectors to be placed back-to-back and to connect to the ROIC through the one input pad to obtain a two-color image.

FLIR ISC9901

์•ˆํ‹ฐ๋ชฌํ™” ์ธ๋“ (InSb), 640 x 512์‹, 20 ๋ฏธํฌ๋ก  ํ”ผ์น˜

ISC9901์€ ์•ˆํ‹ฐ๋ชฌํ™” ์ธ๋“ (InSb), ์–‘์ž ์šฐ๋ฌผ ์ ์™ธ์„  ๊ด‘ ๊ฒ€์ถœ๊ธฐ (QWIP), ์ธ๋“๊ฐˆ๋ฅจ๋น„์†Œ (InGaAs), ํ…”๋ฃจ๋ฅดํ™”์ˆ˜์€์นด๋“œ๋ฎด (MCT) ๋“ฑ๊ณผ ๊ฐ™์€ P-on-N ๋””ํ…ํ„ฐ์™€ ํ˜ธํ™˜์ด ๊ฐ€๋Šฅํ•œ ๋Œ€ํ˜• ํŒ๋…์ถœ๋ ฅํ†ตํ•ฉํšŒ๋กœ (ROIC) ์ž…๋‹ˆ๋‹ค. 640 x 512 ๋ฐฐ์—ด์€ ๊ฐ–์ถ˜ ISC9901์€ ISC9803 ๊ธฐ๊ธฐ์˜ ๋™์ƒ ๊ฒฉ์ธ ์ œํ’ˆ์ด๋ฉฐ, ํ”ฝ์…€ ํ”ผ์น˜๊ฐ€ 20 ๋ฏธํฌ๋ก ์œผ๋กœ ์ƒ๋Œ€์ ์œผ๋กœ ๋” ์ž‘์Šต๋‹ˆ๋‹ค. ๋˜ํ•œ, ์œˆ๋„์ž‰, ์ด๋ฏธ์ง€ ์ „์œ„, ์กฐ์ •์‹ ๊ฒŒ์ธ (Adjustable gain), ๋‹ค์ค‘ ์ถœ๋ ฅ ์ฑ„๋„๊ณผ ๊ฐ™์€ ๊ณ ๊ธ‰ํ˜• ๊ธฐ๋Šฅ์„ ์ œ๊ณตํ•˜์—ฌ ํ’€-ํ”„๋ ˆ์ž„ ์ž‘๋™ ์‹œ์—๋Š” ์ตœ๋Œ€ 97 ํ”„๋ ˆ์ž„/์ดˆ, ์ž‘์€ ์ฐฝ ํฌ๊ธฐ๋กœ ์ž‘๋™ ์‹œ์—๋Š” 930 ํ”„๋ ˆ์ž„/์ดˆ์˜ ๋ฐ์ดํ„ฐ ์†๋„๋ฅผ ์„ ์‚ฌํ•ฉ๋‹ˆ๋‹ค.

FLIR ISC0002

640 ร— 512 ์ € ๋ฐฑ๊ทธ๋ผ์šด๋“œ ํŒ๋…์ถœ๋ ฅํ†ตํ•ฉํšŒ๋กœ (ROIC)

ISC0002๋Š” 640 × 512 ํฌ๋งท, 25๋ฏธํฌ๋ก  ํ”ผ์น˜ ๊ธฐ๊ธฐ๋กœ, ๋ฐฑ๊ทธ๋ผ์šด๋“œ๊ฐ€ ์ ์€ ์• ํ”Œ๋ฆฌ์ผ€์ด์…˜์„ ์œ„ํ•ด ์„ค๊ณ„๋˜์—ˆ์Šต๋‹ˆ๋‹ค. CTIA ํ”„๋ก ํŠธ ์—”๋“œ ํšŒ๋กœ๋ฅผ ์‚ฌ์šฉํ•˜๋ฉฐ ํ•˜์ด ๊ฒŒ์ธ ๋ชจ๋“œ์˜ ํŒ๋… ๋…ธ์ด์ฆˆ๋Š” 70 ์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“, ์Šคํ‚ค๋ฐ, ์ „์› ๋ฐ ์ „๋ฅ˜ ์กฐ์ •, ์„ ํƒ ๊ฐ€๋Šฅํ•œ ํ†ตํ•ฉ ์บํŒจ์‹œํ„ฐ(39K ๋˜๋Š” 1.9M ์ „์ž)๋ฅผ ์ถ”๊ฐ€๋กœ ์ง€์›ํ•ฉ๋‹ˆ๋‹ค.

์ œํ’ˆ ์ˆ˜๋ช… ์ข…๋ฃŒ ํ†ต์ง€

ํ•ด๋‹น ์ œํ’ˆ์„ ์ฃผ๋ฌธํ•  ์ˆ˜ ์žˆ๋Š” ํŒ๋งค ์ข…๋ฃŒ์ผ์€ 2024๋…„ 3์›” 18์ผ์ž…๋‹ˆ๋‹ค. ๊ณ ๊ฐ์€ 2025๋…„ 6์›” 30์ผ๊นŒ์ง€ Teledyne FLIR์˜ ์ง€์›์„ ๊ณ„์† ๋ฐ›์„ ์ˆ˜ ์žˆ์Šต๋‹ˆ๋‹ค. ์ž์„ธํ•œ ๋‚ด์šฉ์€ ์•„๋ž˜์˜ ์•Œ๋ฆผ์„ ์ฐธ์กฐํ•˜์‹ญ์‹œ์˜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 ISC0404

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

ISC0404์€ 18๋ฏธํฌ๋ก  ํ”ฝ์…€ ํ”ผ์น˜์˜ 1024 × 1024 ํ˜•์‹ ROIC์ž…๋‹ˆ๋‹ค. InSb, InGaAs ๋ฐ T2SLS ๊ฒ€์ถœ๊ธฐ์™€ ๊ฐ™์€ P-on-N ๊ฒ€์ถœ๊ธฐ์™€ ํ•จ๊ป˜ ์‚ฌ์šฉํ•˜๋„๋ก ์„ค๊ณ„๋œ ์ด ์–ด๋ ˆ์ด๋Š” ์ „์ฒด ํ”„๋ ˆ์ž„ ์ž‘๋™ ์‹œ ์ตœ๋Œ€ 120 ํ”„๋ ˆ์ž„/์ดˆ, ์ž‘์€ ์ฐฝ ํฌ๊ธฐ์—์„œ๋Š” 2054 ํ”„๋ ˆ์ž„/์ดˆ์˜ ๋ฐ์ดํ„ฐ ์†๋„๋ฅผ ์ง€์›ํ•˜๋Š” ๋‹ค์ค‘ ์ถœ๋ ฅ ์ฑ„๋„์„ ํฌํ•จํ•˜์—ฌ ๋ชจ๋“  ํ‘œ์ค€ ์„ค๊ณ„์™€ ๋™์ผํ•œ ๊ณ ๊ธ‰ ๊ธฐ๋Šฅ ์„ธํŠธ๋ฅผ ์ œ๊ณตํ•ฉ๋‹ˆ๋‹ค. ์ถฉ์ „ ์šฉ๋Ÿ‰์€ >10M ์ผ๋ ‰ํŠธ๋ก ์ด๊ณ  ๋ฐ”์ด์–ด์Šค ์กฐ์ •์€ 600mV์ž…๋‹ˆ๋‹ค.

์ œํ’ˆ ์ˆ˜๋ช… ์ข…๋ฃŒ ํ†ต์ง€

ํ•ด๋‹น ์ œํ’ˆ์„ ์ฃผ๋ฌธํ•  ์ˆ˜ ์žˆ๋Š” ํŒ๋งค ์ข…๋ฃŒ์ผ์€ 2024๋…„ 3์›” 18์ผ์ž…๋‹ˆ๋‹ค. ๊ณ ๊ฐ์€ 2025๋…„ 6์›” 30์ผ๊นŒ์ง€ Teledyne FLIR์˜ ์ง€์›์„ ๊ณ„์† ๋ฐ›์„ ์ˆ˜ ์žˆ์Šต๋‹ˆ๋‹ค. ์ž์„ธํ•œ ๋‚ด์šฉ์€ ์•„๋ž˜์˜ ์•Œ๋ฆผ์„ ์ฐธ์กฐํ•˜์‹ญ์‹œ์˜ค.

FLIR ISC0904

Mega-pixel format readout integrated circuit (ROIC) optimized for Type-II strained-layer superlattice (T2SLS) and MCT infrared detectors

The ISC0904 is 1K × 1K format, 18-micron pixel pitch device. It is derived from the ISC0404 but designed for N-on-P detectors such as strained-layer superlattice devices or MCT. The 18-micron pixel pitch is identical and the user interface is similar. The ISC0904 has a well capacity of 11M electrons and can be operated in 4, 8 or 16 output mode. A frame of 120 Hz can be achieved for 1024 × 1024 pixels using the 16-output mode.

FLIR ISC0802

HD format readout integrated circuit (ROIC) optimized for Indium Antimonide (InSb) infrared detectors

ISC0802๋Š” InSb ๋˜๋Š” MCT์™€ ๊ฐ™์€ ๋‚ฎ์€ ์—ญ๋ฐฉํ–ฅ ๋ฐ”์ด์–ด์Šค ๊ฒ€์ถœ๊ธฐ์™€ ํ•จ๊ป˜ ์‚ฌ์šฉํ•˜๋„๋ก ์„ค๊ณ„๋œ 1344 × 784 ํ˜•์‹์˜ 14๋ฏธํฌ๋ก  ํ”ฝ์…€ ์žฅ์น˜์ž…๋‹ˆ๋‹ค. ์ด HD ํ˜•์‹์˜ ROIC๋Š” 4, 8 ๋˜๋Š” 16 ์ถœ๋ ฅ ๋ชจ๋“œ์—์„œ ์ž‘๋™ํ•˜์—ฌ 16 ์ถœ๋ ฅ ๋ชจ๋“œ์—์„œ 120Hz ํ”„๋ ˆ์ž„ ์†๋„๋ฅผ ๋‹ฌ์„ฑํ•  ์ˆ˜ ์žˆ์Šต๋‹ˆ๋‹ค. ISC0802๋Š” ์œˆ๋„์šฐ ์„ค์ •, ์กฐ์ • ๊ฐ€๋Šฅํ•œ ํ†ตํ•ฉ ์‹œ๊ฐ„, ์ฝ๊ธฐ ์ค‘ ํ†ตํ•ฉ ๋˜๋Š” ์ฝ๊ธฐ ํ›„ ํ†ตํ•ฉ ๋ชจ๋“œ, ์กฐ์ • ๊ฐ€๋Šฅํ•œ ๋ฐ”์ด์–ด์Šค ๋ฐ ์ „์› ์„ค์ •์„ ์ง€์›ํ•ฉ๋‹ˆ๋‹ค.

์ œํ’ˆ ์ˆ˜๋ช… ์ข…๋ฃŒ ํ†ต์ง€

ํ•ด๋‹น ์ œํ’ˆ์„ ์ฃผ๋ฌธํ•  ์ˆ˜ ์žˆ๋Š” ํŒ๋งค ์ข…๋ฃŒ์ผ์€ 2024๋…„ 3์›” 18์ผ์ž…๋‹ˆ๋‹ค. ๊ณ ๊ฐ์€ 2025๋…„ 6์›” 30์ผ๊นŒ์ง€ Teledyne FLIR์˜ ์ง€์›์„ ๊ณ„์† ๋ฐ›์„ ์ˆ˜ ์žˆ์Šต๋‹ˆ๋‹ค. ์ž์„ธํ•œ ๋‚ด์šฉ์€ ์•„๋ž˜์˜ ์•Œ๋ฆผ์„ ์ฐธ์กฐํ•˜์‹ญ์‹œ์˜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 ISC1504

Mega-pixel format readout integrated circuit (ROIC) optimized for Indium Gallium Arsenide (InGaAs) infrared detectors

The ISC1504 is our largest format ROIC, optimized for InGaAs/VisGaAs detectors. This 1920 × 1080 format, 10-micron pitch device uses a CTIA input circuit for P-on-N detectors. The ISC1504 supports anti-blooming, input skimming, multiple integration modes and selectable output modes. A simple user interface with analog outputs allows for easy integration into high resolution systems.

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.

ISC1404

์•ˆํ‹ฐ๋ชฌํ™” ์ธ๋“ (InSb) ๋ฐ SLS, 2K x 2K ํ˜•์‹์— ์ตœ์ ํ™” ๋˜์–ด ์žˆ๋Š” ๋Œ€ํ˜• 10 ๋ฏธํฌ๋ก  ํ”ผ์น˜

ISC 1404๋Š” ์•ˆํ‹ฐ๋ชฌํ™” ์ธ๋“ (InSb) ๋ฐ SLS, 2K x 2K ํ˜•์‹์— ์ตœ์ ํ™” ๋˜์–ด ์žˆ๋Š” ๋Œ€ํ˜• 10 ๋ฏธํฌ๋ก  ํ”ผ์น˜ ํŒ๋…์ถœ๋ ฅํ†ตํ•ฉํšŒ๋กœ (ROIC) ์ œํ’ˆ์ž…๋‹ˆ๋‹ค.