NIR, SWIR, MWIR, LWIR은 각기 다른 설계 공간입니다
IR filters should be matched to detector material, substrate transmission, and working temperature. Do not treat all IR bands as interchangeable.
NIR, SWIR, MWIR 및 LWIR용 적외선 광학 필터
근적외선, 단파장 적외선, 중파장 적외선, 장파장 적외선 시스템용 적외선 필터를 확인하세요. 중적외선 대역통과, 원적외선 필터, 실리콘 적외선 필터, 사파이어 적외선 필터, 게르마늄 AR 코팅 윈도우, 금속증착 적외선 윈도우를 센싱 및 이미징 기기용으로 비교하세요.
선택 모델
- 권장 모델은 문의해 주세요.
선택 방법
먼저 적외선 영역에서 선택하고, 검출기 감도, 기판 투과율, 코팅 대역, 환경 노출, 장착 요구사항을 확인하세요. 적외선 필터는 가시광 필터와 다른 소재 선택이 필요한 경우가 많습니다.
17
적외선 필터
OPTOStokes 적외선 필터는 근적외선(750-1100nm), 단파장 적외선(SWIR 1.1-2.5µm), 중파장 적외선(MWIR 3-5µm) 및 장파장 적외선(LWIR 8-14µm) 응용을 커버합니다. 카탈로그에는 중/원적외선 협대역 대역통과, 광대역 대역통과, 적외선 장파통과 필터, AR 코팅 및 금속증착 적외선 윈도우도 포함되어 열화상, 가스 센싱, 분광, 검출기 패키징에 대응합니다.
IR 밴드패스 필터
| 모델 | 중심 파장 (nm) | 투과율 | 반치폭 (nm) | 광학 밀도 |
|---|---|---|---|---|
| STO-BP680 | 680 ± 2 | T≥90% | 10-20 | OD≥3@300-1100 |
| STO-BP1120 | 1120 ± 2 | T≥90% | 10-20 | OD≥3@300-1200 |
| STO-BP1150 | 1150 ± 2 | T≥90% | 10-20 | OD≥3@300-1200 |
| STO-BP1173 | 1173 ± 2 | T≥90% | 10-20 | OD≥3@300-1200 |
| STO-BP1250 | 1250 ± 2 | T≥70% | 10-20 | OD≥3@700-1800 |
| STO-BP1285 | 1285 ± 2 | T≥70% | 10-20 | OD≥3@1000-1700 |
| STO-BP1455 | 1455 ± 2 | T≥50% | 10-20 | OD≥3@1200-1800 |
| STO-BP1535 | 1535 ± 2 | T≥90% | 10-20 | OD≥3@600-2000 |
| STO-BP1545 | 1545 ± 2 | T≥90% | 10-20 | OD≥3@600-2000 |
| STO-BP1550 | 1550 ± 2 | T≥90% | 10-20 | OD≥3@600-2000 |
| STO-BP1555 | 1555 ± 2 | T≥90% | 10-20 | OD≥3@600-2000 |
| STO-BP1570 | 1570 ± 2 | T≥90% | 10-20 | OD≥3@1250-1700 |
| STO-BP1615 | 1615 ± 2 | T≥90% | 10-20 | OD≥3@1450-1900 |
| STO-BP1620 | 1620 ± 2 | T≥70% | 10-20 | OD≥3@1450-1900 |
| STO-BP1625 | 1625 ± 2 | T≥70% | 10-20 | OD≥3@1450-1900 |
| STO-BP1655 | 1655 ± 5 | T≥70% | 10-20 | OD≥3@1350-2200 |
| STO-BP1660 | 1660 ± 5 | T≥70% | 10-20 | OD≥3@1350-2200 |
| STO-BP1680 | 1680 ± 10 | T≥90% | 10-20 | OD≥3@800-3000 |
| STO-BP1685 | 1685 ± 2 | T≥80% | 10-20 | OD≥3@1550-2000 |
| STO-BP1695 | 1695 ± 2 | T≥80% | 10-20 | OD≥3@1550-2000 |
| STO-BP1935 | 1935 ± 2 | T≥60% | 10-20 | OD≥3@800-2000 |
| STO-BP1940 | 1940 ± 2 | T≥60% | 10-20 | OD≥3@800-2000 |
| STO-BP2050 | 2050 ± 2 | T≥80% | 10-20 | OD≥3@800-2000 |
| STO-BP2180 | 2180 ± 2 | T≥80% | 10-20 | OD≥3@800-2000 |
| STO-BP2230 | 2230 ± 2 | T≥80% | 10-20 | OD≥3@800-2000 |
| STO-BP2270 | 2270 ± 2 | T≥80% | 10-20 | OD≥3@800-2000 |
| STO-BP2340 | 2340 ± 2 | T≥80% | 10-20 | OD≥3@800-2000 |
| STO-BP1100 | 1100 ± 5 | T≥90% | 20-60 | OD≥3@350-1700 |
| STO-BP1120 | 1120 ± 5 | T≥90% | 20-60 | OD≥3@350-1700 |
| STO-BP1125 | 1125 ± 5 | T≥90% | 20-60 | OD≥3@350-1700 |
| STO-BP1150 | 1150 ± 5 | T≥90% | 20-60 | OD≥3@350-1700 |
| STO-BP1173 | 1173 ± 5 | T≥90% | 20-60 | OD≥3@350-1700 |
| STO-BP1200 | 1200 ± 5 | T≥90% | 20-60 | OD≥3@350-1700 |
| STO-BP1235 | 1235 ± 5 | T≥90% | 20-60 | OD≥3@350-1700 |
| STO-BP1245 | 1245 ± 5 | T≥90% | 20-60 | OD≥3@350-1700 |
| STO-BP1250 | 1250 ± 5 | T≥90% | 20-60 | OD≥3@350-1700 |
| STO-BP1290 | 1290 ± 5 | T≥90% | 20-60 | OD≥3@350-1700 |
| STO-BP1300 | 1300 ± 5 | T≥90% | 20-60 | OD≥3@350-1700 |
| STO-BP1320 | 1320 ± 5 | T≥90% | 20-60 | OD≥3@350-1700 |
| STO-BP1340 | 1340 ± 5 | T≥90% | 20-60 | OD≥3@350-1700 |
| STO-BP1380 | 1380 ± 5 | T≥90% | 20-60 | OD≥3@350-1700 |
| STO-BP1430 | 1430 ± 5 | T≥90% | 20-60 | OD≥3@350-1700 |
| STO-BP1445 | 1445 ± 5 | T≥90% | 20-60 | OD≥3@350-1700 |
| STO-BP1450 | 1450 ± 5 | T≥90% | 20-60 | OD≥3@350-1700 |
| STO-BP1530 | 1530 ± 5 | T≥90% | 20-60 | OD≥3@350-1700 |
| STO-BP1535 | 1535 ± 5 | T≥90% | 20-60 | OD≥3@350-1700 |
| STO-BP1540 | 1540 ± 5 | T≥90% | 20-60 | OD≥3@350-1700 |
| STO-BP1550 | 1550 ± 5 | T≥90% | 20-60 | OD≥3@350-1700 |
| STO-BP1570 | 1570 ± 5 | T≥90% | 20-60 | OD≥3@350-1700 |
| STO-BP1575 | 1575 ± 5 | T≥90% | 20-60 | OD≥3@350-1700 |
| STO-BP1600 | 1600 ± 5 | T≥90% | 90-100 | OD≥3@350-1700 |
| STO-BP1610 | 1610 ± 5 | T≥90% | 90-100 | OD≥3@350-1700 |
| STO-BP1630 | 1630 ± 5 | T≥90% | 90-100 | OD≥3@350-1700 |
| STO-BP1650 | 1650 ± 5 | T≥90% | 20-60 | OD≥3@350-1700 |
| STO-BP1654 | 1654 ± 5 | T≥90% | 20-60 | OD≥3@350-1700 |
| STO-BP1660 | 1660 ± 5 | T≥90% | 20-60 | OD≥3@800-3000 |
| STO-BP1680 | 1680 ± 5 | T≥90% | 20-60 | OD≥3@800-3000 |
| STO-BP1700 | 1700 ± 5 | T≥90% | 90-100 | OD≥3@800-2000 |
| STO-BP1714 | 1714 ± 5 | T≥90% | 90-100 | OD≥3@800-2000 |
| STO-BP1716 | 1716 ± 5 | T≥90% | 90-100 | OD≥3@800-2000 |
| STO-BP1780 | 1780 ± 5 | T≥90% | 40-70 | OD≥3@200-3000 |
| STO-BP1800 | 1800 ± 5 | T≥90% | 40-70 | OD≥3@200-3000 |
| STO-BP1810 | 1810 ± 5 | T≥90% | 40-70 | OD≥3@200-3000 |
| STO-BP1818 | 1818 ± 5 | T≥90% | 40-70 | OD≥3@200-3000 |
| STO-BP1830 | 1830 ± 5 | T≥90% | 40-70 | OD≥3@200-3000 |
| STO-BP1920 | 1920 ± 5 | T≥90% | 40-70 | OD≥3@200-3000 |
| STO-BP1930 | 1930 ± 5 | T≥90% | 40-70 | OD≥3@200-3000 |
| STO-BP1935 | 1935 ± 5 | T≥90% | 40-70 | OD≥3@200-3000 |
| STO-BP1940 | 1940 ± 5 | T≥90% | 40-70 | OD≥3@200-3000 |
| STO-BP1945 | 1945 ± 5 | T≥90% | 40-70 | OD≥3@200-3000 |
| STO-BP1950 | 1950 ± 5 | T≥90% | 40-70 | OD≥3@200-3000 |
IR 롱패스 필터
| 모델 | 차단 시작 (nm) | 투과율 | 투과 범위 (nm) | 광학 밀도 |
|---|---|---|---|---|
| STO-LP900 | 900 ± 5 | T≥90% | 910-1100 | OD≥3@350-880 |
| STO-LP910 | 910 ± 5 | T≥90% | 920-1100 | OD≥3@350-890 |
| STO-LP920 | 920 ± 5 | T≥90% | 930-1100 | OD≥3@350-900 |
| STO-LP920 | 920 ± 10 | T≥90% | 940-1700 | OD≥3@350-890 |
| STO-LP930 | 930 ± 5 | T≥90% | 940-1100 | OD≥3@350-910 |
| STO-LP940 | 940 ± 5 | T≥90% | 950-1100 | OD≥3@350-920 |
| STO-LP950 | 950 ± 5 | T≥90% | 970-1100 | OD≥3@350-930 |
| STO-LP970 | 970 ± 5 | T≥90% | 980-1100 | OD≥3@350-940 |
| STO-LP1000 | 1000 ± 10 | T≥90% | 1020-2000 | OD≥3@350-970 |
| STO-LP1010 | 1010 ± 10 | T≥90% | 1030-1200 | OD≥3@350-990 |
| STO-LP1060 | 1060 ± 10 | T≥88% | 1085-1100 | OD≥3@350-1035 |
| STO-LP1150 | 1150 ± 10 | T≥90% | 1180-1700 | OD≥3@700-1120 |
| STO-LP1170 | 1170 ± 10 | T≥90% | 1200-1700 | OD≥3@700-1135 |
| STO-LP1200 | 1200 ± 10 | T≥90% | 1230-1800 | OD≥3@350-1175 |
| STO-LP1250 | 1250 ± 10 | T≥90% | 1260-1750 | OD≥3@350-1215 |
| STO-LP1270 | 1270 ± 10 | T≥90% | 1300-1800 | OD≥3@350-1240 |
| STO-LP1380 | 1380 ± 10 | T≥90% | 1400-2150 | OD≥3@700-1360 |
| STO-LP1400 | 1400 ± 10 | T≥90% | 1420-1100 | OD≥3@350-1380 |
| STO-LP1450 | 1450 ± 10 | T≥90% | 1480-1800 | OD≥3@350-1420 |
| STO-LP1470 | 1470 ± 10 | T≥90% | 1500-1800 | OD≥3@350-1400 |
| STO-LP1600 | 1600 ± 10 | T≥90% | 1625-2300 | OD≥3@350-1540 |
카탈로그 중/원적외선 협대역 대역통과 필터
중/원적외선 협대역 대역통과 필터는 MWIR 및 LWIR 기기 대역용으로 실리콘, 사파이어, 게르마늄, 불화칼슘, 셀렌화아연 기판을 사용합니다. 검출기 모듈 및 열화상 센싱 시스템용 커스텀 사이즈도 가능합니다.
| 모델 | IR 영역 | 중심 파장 (nm) | 반치폭 (nm) | 피크 투과율 | 차단 | 기판 | 크기 |
|---|---|---|---|---|---|---|---|
| STO-NBP 2750 500nm | MWIR | 2750 ± 50 | 500 ± 60 | >=80% | 400-7000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 2775 250nm | MWIR | 2775 ± 30 | 250 ± 20 | >=80% | 400-7000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 2850 400nm | MWIR | 2850 ± 40 | 400 ± 30 | >=80% | 400-7000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 3040 140nm | MWIR | 3040 ± 30 | 140 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 3040 140nm | MWIR | 3040 ± 30 | 140 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 25 x 0.6mm |
| STO-NBP 3060 140nm | MWIR | 3060 ± 30 | 140 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 3060 140nm | MWIR | 3060 ± 30 | 140 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 25 x 0.6mm |
| STO-NBP 3080 140nm | MWIR | 3080 ± 30 | 140 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 25 x 0.6mm |
| STO-NBP 3090 140nm | MWIR | 3090 ± 30 | 140 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 3280 160nm | MWIR | 3280 ± 30 | 160 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 3300 160nm | MWIR | 3300 ± 30 | 160 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 3300 160nm | MWIR | 3300 ± 30 | 160 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 25 x 0.6mm |
| STO-NBP 3310 60nm | MWIR | 3310 ± 10 | 60 ± 20 | >=80% | 400-4700nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 3330 60nm | MWIR | 3330 ± 10 | 60 ± 20 | >=80% | 400-4700nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 3330 160nm | MWIR | 3330 ± 30 | 160 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 3375 160nm | MWIR | 3375 ± 30 | 160 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 3375 160nm | MWIR | 3375 ± 30 | 160 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 25 x 0.6mm |
| STO-NBP 3400 120nm | MWIR | 3400 ± 30 | 120 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 3400 180nm | MWIR | 3400 ± 30 | 180 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 3420 180nm | MWIR | 3420 ± 30 | 180 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 3440 120nm | MWIR | 3440 ± 30 | 120 ± 20 | >=80% | 400-25000nm,T≤1% | Sapphire | Dia. 25 x 0.8mm |
| STO-NBP 3440 160nm | MWIR | 3440 ± 30 | 160 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 3460 150nm | MWIR | 3460 ± 30 | 150 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 3800 300nm | MWIR | 3800 ± 40 | 300 ± 30 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 3900 90nm | MWIR | 3900 ± 20 | 90 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 3920 90nm | MWIR | 3920 ± 20 | 90 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 3950 90nm | MWIR | 3950 ± 20 | 90 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 3950 90nm | MWIR | 3950 ± 20 | 90 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | 3.3 x 3.3 x 0.5mm |
| STO-NBP 3970 90nm | MWIR | 3970 ± 20 | 90 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 4000 90nm | MWIR | 4000 ± 20 | 90 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 4050 180nm | MWIR | 4050 ± 30 | 180 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 4100 180nm | MWIR | 4100 ± 30 | 180 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 4200 180nm | MWIR | 4200 ± 30 | 180 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 4230 160nm | MWIR | 4230 ± 30 | 160 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 4260 180nm | MWIR | 4260 ± 30 | 180 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 4260 180nm | MWIR | 4260 ± 30 | 180 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | 2.9 x 2.9 x 0.5mm |
| STO-NBP 4260 180nm | MWIR | 4260 ± 30 | 180 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | 3.3 x 3.3 x 0.5mm |
| STO-NBP 4280 180nm | MWIR | 4280 ± 20 | 180 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 4300 130nm | MWIR | 4300 ± 30 | 130 ± 20 | >=75% | 400-16000nm,T≤1% | Monocrystalline silicon | Dia. 25 x 0.6mm |
| STO-NBP 4300 160nm | MWIR | 4300 ± 30 | 160 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 4300 180nm | MWIR | 4300 ± 30 | 180 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 4320 160nm | MWIR | 4320 ± 30 | 160 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 4330 130nm | MWIR | 4330 ± 30 | 130 ± 20 | >=80% | 400-16000nm,T≤1% | Monocrystalline silicon | Dia. 25 x 0.6mm |
| STO-NBP 4330 180nm | MWIR | 4330 ± 30 | 180 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 4360 180nm | MWIR | 4360 ± 30 | 180 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 4380 180nm | MWIR | 4380 ± 30 | 180 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 4420 60nm | MWIR | 4420 ± 10 | 60 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 25 x 0.6mm |
| STO-NBP 4430 60nm | MWIR | 4430 ± 10 | 60 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 25 x 0.6mm |
| STO-NBP 4450 60nm | MWIR | 4450 ± 10 | 60 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 25 x 0.6mm |
| STO-NBP 4450 200nm | MWIR | 4450 ± 30 | 200 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 25 x 0.6mm |
| STO-NBP 4480 60nm | MWIR | 4480 ± 10 | 60 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 25 x 0.6mm |
| STO-NBP 4500 60nm | MWIR | 4500 ± 10 | 60 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 25 x 0.6mm |
| STO-NBP 4500 140nm | MWIR | 4500 ± 30 | 140 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 25 x 0.6mm |
| STO-NBP 4500 200nm | MWIR | 4500 ± 30 | 200 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 4520 140nm | MWIR | 4520 ± 30 | 140 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 25 x 0.6mm |
| STO-NBP 4560 160nm | MWIR | 4560 ± 30 | 160 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 4600 160nm | MWIR | 4600 ± 30 | 160 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 4640 160nm | MWIR | 4640 ± 30 | 160 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 4650 160nm | MWIR | 4650 ± 30 | 160 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 4680 150nm | MWIR | 4680 ± 30 | 150 ± 20 | >=80% | 400-25000nm,T≤1% | Sapphire | Dia. 25 x 0.8mm |
| STO-NBP 4690 160nm | MWIR | 4690 ± 30 | 160 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 4750 180nm | MWIR | 4750 ± 30 | 180 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 4770 150nm | MWIR | 4770 ± 30 | 150 ± 20 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 5300 600nm | MWIR/LWIR transition | 5300 ± 40 | 600 ± 30 | >=80% | 400-11000nm,T≤1% | Monocrystalline silicon | Dia. 25 x 0.5mm |
| STO-NBP 7300 300nm | MWIR/LWIR transition | 7300 ± 40 | 300 ± 30 | >=70% | 400-12000nm,T≤1% | Monocrystalline silicon | Dia. 25 x 0.5mm |
| STO-NBP 7350 200nm | MWIR/LWIR transition | 7350 ± 30 | 200 ± 30 | >=65% | 400-12000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 7410 200nm | MWIR/LWIR transition | 7410 ± 30 | 200 ± 30 | >=65% | 400-12000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 7470 200nm | MWIR/LWIR transition | 7470 ± 30 | 200 ± 30 | >=75% | 400-12000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 7625 200nm | MWIR/LWIR transition | 7625 ± 30 | 200 ± 30 | >=75% | 400-12000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 7650 200nm | MWIR/LWIR transition | 7650 ± 30 | 200 ± 30 | >=60% | 400-12000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 8420 200nm | LWIR | 8420 ± 40 | 200 ± 30 | >=60% | 400-16000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 9020 180nm | LWIR | 9020 ± 30 | 180 ± 30 | >=75% | 400-16000nm,T≤1% | Float-zone silicon | Dia. 100 x 0.5mm |
| STO-NBP 9080 180nm | LWIR | 9080 ± 30 | 180 ± 30 | >=75% | 400-16000nm,T≤1% | Float-zone silicon | Dia. 100 x 0.5mm |
| STO-NBP 9900 370nm | LWIR | 9900 ± 30 | 370 ± 20 | >=70% | 400-16000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 10000 370nm | LWIR | 10000 ± 40 | 370 ± 30 | >=75% | 400-16000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 10050 370nm | LWIR | 10050 ± 40 | 370 ± 30 | >=60% | 400-16000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 10270 600nm | LWIR | 10270 ± 40 | 600 ± 30 | >=75% | 400-13500nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 10460 370nm | LWIR | 10460 ± 40 | 370 ± 30 | >=75% | 400-14000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 10500 600nm | LWIR | 10500 ± 50 | 600 ± 40 | >=75% | 400-13500nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 10560 370nm | LWIR | 10560 ± 40 | 370 ± 30 | >=75% | 400-18000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 10700 370nm | LWIR | 10700 ± 40 | 370 ± 30 | >=75% | 400-14000nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 11500 600nm | LWIR | 11500 ± 50 | 600 ± 40 | >=65% | 400-14500nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 11700 600nm | LWIR | 11700 ± 50 | 600 ± 40 | >=65% | 400-14500nm,T≤1% | Monocrystalline silicon | Dia. 100 x 0.5mm |
| STO-NBP 14500 1000nm | LWIR | 14500 ± 50 | 1000 ± 50 | >=70% | 400-19000nm,T≤1% | Monocrystalline silicon | Dia. 25 x 0.5mm |
카탈로그 적외선 광대역 대역통과 필터
광대역 적외선 대역통과 필터는 MWIR 및 LWIR의 더 넓은 투과 윈도우를 대외 차단과 함께 제공하여 열화상, 가스 분석, 적외선 센싱에 대응합니다.
| 모델 | IR 영역 | 투과 범위 (nm) | 평균 투과율 | 차단 | 크기 | 기판 |
|---|---|---|---|---|---|---|
| STO-WBP 3100-3800nm Filter | MWIR | 3100-3800nm | >=85% | 400-25000nm, <=1% | Custom | Sapphire |
| STO-WBP 3250-3500nm Filter | MWIR | 3250-3500nm | >=88% | 400-6000nm, <=1% | Custom | Germanium |
| STO-WBP 3550-4150nm Filter | MWIR | 3550-4150nm | >=90% | 400-6000nm, <=1% | Custom | Germanium |
| STO-WBP 3670-4970nm Filter | MWIR | 3670-4970nm | >=90% | 400-6000nm, <=1% | Custom | Germanium |
| STO-WBP 4500-5000nm Filter | MWIR | 4500-5000nm | >=90% | 400-6000nm, <=1% | Custom | Germanium |
| STO-WBP 4750-5400nm Filter | MWIR/LWIR transition | 4750-5400nm | >=80% | 400-25000nm, <=1% | Custom | Sapphire |
| STO-WBP 8000-14000nm Filter | LWIR | 8000-14000nm | >75% | 0.4-7.5um, 15-21.5um, <=1% | Custom | Monocrystalline silicon |
| STO-WBP 8000-9450nm Filter | LWIR | 8000-9450nm | >=92% | 400-12000nm, <=1% | Custom | Germanium |
카탈로그 적외선 장파통과 필터
적외선 장파통과 필터는 긴 파장 영역을 투과하고 짧은 파장 에너지를 차단하여 검출기 측 분리와 열화상 경로에 대응합니다.
| 모델 | IR 영역 | 투과 범위 (nm) | 평균 투과율 | 차단 | 크기 | 기판 |
|---|---|---|---|---|---|---|
| STOLWP 3000-5000nm Filter | MWIR | 3000-5000nm | >85% | 400-2900nm, <=1% | Custom | Sapphire |
| STOLWP 5500-14000nm | LWIR | 5500-14000nm | >80% | 400-5000nm, <=1% | Custom | Monocrystalline silicon |
| STOLWP 7000-14000nm Filter | LWIR | 7000-14000nm | >80% | 400-6500nm, <=1% | Custom | Monocrystalline silicon |
| STOLWP 7700-9000nm Filter | LWIR | 7700-9000nm | >80% | 400-7600nm, <=1% | Custom | Monocrystalline silicon |
| STOLWP 8000-12000nm Filter | LWIR | 8000-12000nm | >85% | 400-7500nm, <=1% | Custom | Germanium |
카탈로그 적외선 AR 코팅
적외선 반사방지 코팅은 표면 반사를 줄여 실리콘, 사파이어, 게르마늄 광학 소자의 시스템 처리량을 향상시킵니다.
| 코팅 | IR 영역 | 투과 범위 (nm) | 평균 투과율 | 크기 | 기판 |
|---|---|---|---|---|---|
| 0.8-5µm AR | MWIR | 0.8-5um | >=86% | Custom | Sapphire |
| 2.9-14.5µm AR | LWIR | 2.9-14.5um | >=73% | Custom | Germanium |
| 3-5µm AR | MWIR | 3-5um | >=90% | Custom | Monocrystalline silicon |
| 7-12µm AR | LWIR | 7-12um | >=88% | Custom | Monocrystalline silicon |
| 8-12µm AR+DLC | LWIR | 8-12um | >=75% | Custom | Monocrystalline silicon |
| 8-14µm AR | LWIR | 8-14um | >=83% | Custom | Monocrystalline silicon |
카탈로그 금속증착 적외선 윈도우
금속증착 적외선 윈도우는 검출기 및 이미징 어셈블리에서 납땜 및 기밀 봉합용으로 코팅된 광학 개구와 금속증착 에지를 사용합니다.
| Specification | IR 영역 | 유효 구경 | 금속화 영역 | 스펙트럼 사양 | 기판 | 외형 크기 |
|---|---|---|---|---|---|---|
| 16 x 16 x 0.8mm | MWIR | 13.2 x 13.2 | ≥13.7 x 13.7 | 3-5um, Tavg≥96% | Germanium | 16 x 16 |
| Dia. 12 x 1mm | MWIR | Dia. 10 | ≥Dia. 10.5 | 3-5um, Tavg≥96% | Monocrystalline silicon | Dia. 12 |
| Dia. 18 x 1mm | MWIR | Dia. 14 | ≥Dia. 14.5 | 3-5um, Tavg≥96% | Monocrystalline silicon | Dia. 18 |
| Dia. 30 x 1mm | MWIR | Dia. 26 | ≥Dia. 26.5 | 3-5um, Tavg≥96% | Sapphire | Dia. 30 |
| 10 x 10 x 1mm | LWIR | 8.5 x 8.5 x 0.9 | ≥8.9 x 8.9 | 8-12um, Tavg≥82% | Monocrystalline silicon | 10 x 10 x 1 |
| Dia. 2.5 x 0.28mm | SWIR | Dia. 1.6 | ≥Dia. 1.8 | 1250-1650nm, Tavg>99% | Sapphire | Dia. 2.5 |
관련 기술 자료
기판 및 코팅 제약
Material choice can limit usable wavelength range before coating performance is considered. Confirm substrate first for IR applications.
열화상 및 센싱
For thermal or gas-sensing work, specify the target absorption band, blocking range, and operating environment.
자주 묻는 질문
어떤 적외선 영역을 커버하나요?
The page covers near infrared, short-wave infrared, mid-wave infrared, and long-wave infrared filter needs where data is available.
적외선 필터에서 기판이 중요한 이유는 무엇인가요?
Substrate materials have different transmission ranges, so the material must support the target infrared wavelength band.
적외선 필터를 커스터마이징할 수 있나요?
Yes. Custom wavelength bands, sizes, substrate choices, and coating targets can be discussed for infrared systems.
Quality & Compliance
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For OEM programs, laboratory instruments, and industrial systems, OPTOStokes keeps quality, material compliance, and engineering support visible from the start of supplier evaluation.
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Process control, inspection records, and repeatable coating workflows for production optical components.
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Compliance documentation can be prepared for qualified projects and regulated supply chains.
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Custom coating and dimensions
Wavelength, FWHM, substrate, AOI, size, and mounting requirements can be reviewed with engineering.
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