NIR, SWIR, MWIR ve LWIR farklı tasarım alanlarıdır
IR filtrelerini dedektör malzemesine, altlık geçirgenliğine ve çalışma sıcaklığına göre eşleştirin. Tüm IR bantları birbirinin yerine kullanılamaz.
OPTOStokes, Optofilters.com'un optik filtre markasıdır; UV, VIS, NIR ve IR uygulamaları için stokta bulunan filtreler ve özel kaplamalı filtreler sunar.
Termal görüntüleme, gaz algılama veya IR spektroskopisi için filtre seçmeden önce NIR, SWIR, MWIR ve LWIR filtrelerini spektral bölge, altlık, kaplama bandı ve türe göre inceleyip karşılaştırın.
Önce kızılötesi bölgeye göre seçin; ardından dedektör duyarlılığını, altlık geçirgenliğini, kaplama bandını, çevresel maruziyeti ve montaj gereksinimlerini doğrulayın. IR filtreleri genellikle görünür ışık filtrelerinden farklı malzeme seçenekleri gerektirir.
OPTOStokes IR filtreleri yakın kızılötesi (750-1100 nm), kısa dalga kızılötesi (SWIR 1,1-2,5 µm), orta dalga kızılötesi (MWIR 3-5 µm) ve uzun dalga kızılötesi (LWIR 8-14 µm) uygulamalarını kapsar. Bu bölümdeki IR bant geçiren ve uzun geçiren filtreler termal görüntüleme kameraları, IR spektroskopisi, gaz algılama ve kızılötesi iletişim sistemleri içindir.
Tüm IR bant geçiren filtreleri görüntüle
| Model | Merkez dalga boyu (nm) | Geçirgenlik | FWHM (nm) | Optik yoğunluk |
|---|---|---|---|---|
| STO-BP680 | 680 ± 2 | T≥90% | 10-20 | OD ≥ 3 at 300-1100 nm |
| STO-BP1120 | 1120 ± 2 | T≥90% | 10-20 | OD ≥ 3 at 300-1200 nm |
| STO-BP1150 | 1150 ± 2 | T≥90% | 10-20 | OD ≥ 3 at 300-1200 nm |
| STO-BP1173 | 1173 ± 2 | T≥90% | 10-20 | OD ≥ 3 at 300-1200 nm |
| STO-BP1250 | 1250 ± 2 | T≥70% | 10-20 | OD ≥ 3 at 700-1800 nm |
| STO-BP1285 | 1285 ± 2 | T≥70% | 10-20 | OD ≥ 3 at 1000-1700 nm |
| STO-BP1455 | 1455 ± 2 | T≥50% | 10-20 | OD ≥ 3 at 1200-1800 nm |
| STO-BP1535 | 1535 ± 2 | T≥90% | 10-20 | OD ≥ 3 at 600-2000 nm |
| STO-BP1545 | 1545 ± 2 | T≥90% | 10-20 | OD ≥ 3 at 600-2000 nm |
| STO-BP1550 | 1550 ± 2 | T≥90% | 10-20 | OD ≥ 3 at 600-2000 nm |
| STO-BP1555 | 1555 ± 2 | T≥90% | 10-20 | OD ≥ 3 at 600-2000 nm |
| STO-BP1570 | 1570 ± 2 | T≥90% | 10-20 | OD ≥ 3 at 1250-1700 nm |
| STO-BP1615 | 1615 ± 2 | T≥90% | 10-20 | OD ≥ 3 at 1450-1900 nm |
| STO-BP1620 | 1620 ± 2 | T≥70% | 10-20 | OD ≥ 3 at 1450-1900 nm |
| STO-BP1625 | 1625 ± 2 | T≥70% | 10-20 | OD ≥ 3 at 1450-1900 nm |
| STO-BP1655 | 1655 ± 5 | T≥70% | 10-20 | OD ≥ 3 at 1350-2200 nm |
| STO-BP1660 | 1660 ± 5 | T≥70% | 10-20 | OD ≥ 3 at 1350-2200 nm |
| STO-BP1680 | 1680 ± 10 | T≥90% | 10-20 | OD ≥ 3 at 800-3000 nm |
| STO-BP1685 | 1685 ± 2 | T≥80% | 10-20 | OD ≥ 3 at 1550-2000 nm |
| STO-BP1695 | 1695 ± 2 | T≥80% | 10-20 | OD ≥ 3 at 1550-2000 nm |
| STO-BP1935 | 1935 ± 2 | T≥60% | 10-20 | OD ≥ 3 at 800-2000 nm |
| STO-BP1940 | 1940 ± 2 | T≥60% | 10-20 | OD ≥ 3 at 800-2000 nm |
| STO-BP2050 | 2050 ± 2 | T≥80% | 10-20 | OD ≥ 3 at 800-2000 nm |
| STO-BP2180 | 2180 ± 2 | T≥80% | 10-20 | OD ≥ 3 at 800-2000 nm |
| STO-BP2230 | 2230 ± 2 | T≥80% | 10-20 | OD ≥ 3 at 800-2000 nm |
| STO-BP2270 | 2270 ± 2 | T≥80% | 10-20 | OD ≥ 3 at 800-2000 nm |
| STO-BP2340 | 2340 ± 2 | T≥80% | 10-20 | OD ≥ 3 at 800-2000 nm |
| STO-BP1100 | 1100 ± 5 | T≥90% | 20-60 | OD ≥ 3 at 350-1700 nm |
| STO-BP1120 | 1120 ± 5 | T≥90% | 20-60 | OD ≥ 3 at 350-1700 nm |
| STO-BP1125 | 1125 ± 5 | T≥90% | 20-60 | OD ≥ 3 at 350-1700 nm |
| STO-BP1150 | 1150 ± 5 | T≥90% | 20-60 | OD ≥ 3 at 350-1700 nm |
| STO-BP1173 | 1173 ± 5 | T≥90% | 20-60 | OD ≥ 3 at 350-1700 nm |
| STO-BP1200 | 1200 ± 5 | T≥90% | 20-60 | OD ≥ 3 at 350-1700 nm |
| STO-BP1235 | 1235 ± 5 | T≥90% | 20-60 | OD ≥ 3 at 350-1700 nm |
| STO-BP1245 | 1245 ± 5 | T≥90% | 20-60 | OD ≥ 3 at 350-1700 nm |
| STO-BP1250 | 1250 ± 5 | T≥90% | 20-60 | OD ≥ 3 at 350-1700 nm |
| STO-BP1290 | 1290 ± 5 | T≥90% | 20-60 | OD ≥ 3 at 350-1700 nm |
| STO-BP1300 | 1300 ± 5 | T≥90% | 20-60 | OD ≥ 3 at 350-1700 nm |
| STO-BP1320 | 1320 ± 5 | T≥90% | 20-60 | OD ≥ 3 at 350-1700 nm |
| STO-BP1340 | 1340 ± 5 | T≥90% | 20-60 | OD ≥ 3 at 350-1700 nm |
| STO-BP1380 | 1380 ± 5 | T≥90% | 20-60 | OD ≥ 3 at 350-1700 nm |
| STO-BP1430 | 1430 ± 5 | T≥90% | 20-60 | OD ≥ 3 at 350-1700 nm |
| STO-BP1445 | 1445 ± 5 | T≥90% | 20-60 | OD ≥ 3 at 350-1700 nm |
| STO-BP1450 | 1450 ± 5 | T≥90% | 20-60 | OD ≥ 3 at 350-1700 nm |
| STO-BP1530 | 1530 ± 5 | T≥90% | 20-60 | OD ≥ 3 at 350-1700 nm |
| STO-BP1535 | 1535 ± 5 | T≥90% | 20-60 | OD ≥ 3 at 350-1700 nm |
| STO-BP1540 | 1540 ± 5 | T≥90% | 20-60 | OD ≥ 3 at 350-1700 nm |
| STO-BP1550 | 1550 ± 5 | T≥90% | 20-60 | OD ≥ 3 at 350-1700 nm |
| STO-BP1570 | 1570 ± 5 | T≥90% | 20-60 | OD ≥ 3 at 350-1700 nm |
| STO-BP1575 | 1575 ± 5 | T≥90% | 20-60 | OD ≥ 3 at 350-1700 nm |
| STO-BP1600 | 1600 ± 5 | T≥90% | 90-100 | OD ≥ 3 at 350-1700 nm |
| STO-BP1610 | 1610 ± 5 | T≥90% | 90-100 | OD ≥ 3 at 350-1700 nm |
| STO-BP1630 | 1630 ± 5 | T≥90% | 90-100 | OD ≥ 3 at 350-1700 nm |
| STO-BP1650 | 1650 ± 5 | T≥90% | 20-60 | OD ≥ 3 at 350-1700 nm |
| STO-BP1654 | 1654 ± 5 | T≥90% | 20-60 | OD ≥ 3 at 350-1700 nm |
| STO-BP1660 | 1660 ± 5 | T≥90% | 20-60 | OD ≥ 3 at 800-3000 nm |
| STO-BP1680 | 1680 ± 5 | T≥90% | 20-60 | OD ≥ 3 at 800-3000 nm |
| STO-BP1700 | 1700 ± 5 | T≥90% | 90-100 | OD ≥ 3 at 800-2000 nm |
| STO-BP1714 | 1714 ± 5 | T≥90% | 90-100 | OD ≥ 3 at 800-2000 nm |
| STO-BP1716 | 1716 ± 5 | T≥90% | 90-100 | OD ≥ 3 at 800-2000 nm |
| STO-BP1780 | 1780 ± 5 | T≥90% | 40-70 | OD ≥ 3 at 200-3000 nm |
| STO-BP1800 | 1800 ± 5 | T≥90% | 40-70 | OD ≥ 3 at 200-3000 nm |
| STO-BP1810 | 1810 ± 5 | T≥90% | 40-70 | OD ≥ 3 at 200-3000 nm |
| STO-BP1818 | 1818 ± 5 | T≥90% | 40-70 | OD ≥ 3 at 200-3000 nm |
| STO-BP1830 | 1830 ± 5 | T≥90% | 40-70 | OD ≥ 3 at 200-3000 nm |
| STO-BP1920 | 1920 ± 5 | T≥90% | 40-70 | OD ≥ 3 at 200-3000 nm |
| STO-BP1930 | 1930 ± 5 | T≥90% | 40-70 | OD ≥ 3 at 200-3000 nm |
| STO-BP1935 | 1935 ± 5 | T≥90% | 40-70 | OD ≥ 3 at 200-3000 nm |
| STO-BP1940 | 1940 ± 5 | T≥90% | 40-70 | OD ≥ 3 at 200-3000 nm |
| STO-BP1945 | 1945 ± 5 | T≥90% | 40-70 | OD ≥ 3 at 200-3000 nm |
| STO-BP1950 | 1950 ± 5 | T≥90% | 40-70 | OD ≥ 3 at 200-3000 nm |
| Model | Cut-on (nm) | Geçirgenlik | Geçirgenlik aralığı (nm) | Optik yoğunluk |
|---|---|---|---|---|
| STO-LP900 | 900 ± 5 | T≥90% | 910-1100 | OD ≥ 3 at 350-880 nm |
| STO-LP910 | 910 ± 5 | T≥90% | 920-1100 | OD ≥ 3 at 350-890 nm |
| STO-LP920 | 920 ± 5 | T≥90% | 930-1100 | OD ≥ 3 at 350-900 nm |
| STO-LP920 | 920 ± 10 | T≥90% | 940-1700 | OD ≥ 3 at 350-890 nm |
| STO-LP930 | 930 ± 5 | T≥90% | 940-1100 | OD ≥ 3 at 350-910 nm |
| STO-LP940 | 940 ± 5 | T≥90% | 950-1100 | OD ≥ 3 at 350-920 nm |
| STO-LP950 | 950 ± 5 | T≥90% | 970-1100 | OD ≥ 3 at 350-930 nm |
| STO-LP970 | 970 ± 5 | T≥90% | 980-1100 | OD ≥ 3 at 350-940 nm |
| STO-LP1000 | 1000 ± 10 | T≥90% | 1020-2000 | OD ≥ 3 at 350-970 nm |
| STO-LP1010 | 1010 ± 10 | T≥90% | 1030-1200 | OD ≥ 3 at 350-990 nm |
| STO-LP1060 | 1060 ± 10 | T≥88% | 1085-1100 | OD ≥ 3 at 350-1035 nm |
| STO-LP1150 | 1150 ± 10 | T≥90% | 1180-1700 | OD ≥ 3 at 700-1120 nm |
| STO-LP1170 | 1170 ± 10 | T≥90% | 1200-1700 | OD ≥ 3 at 700-1135 nm |
| STO-LP1200 | 1200 ± 10 | T≥90% | 1230-1800 | OD ≥ 3 at 350-1175 nm |
| STO-LP1250 | 1250 ± 10 | T≥90% | 1260-1750 | OD ≥ 3 at 350-1215 nm |
| STO-LP1270 | 1270 ± 10 | T≥90% | 1300-1800 | OD ≥ 3 at 350-1240 nm |
| STO-LP1380 | 1380 ± 10 | T≥90% | 1400-2150 | OD ≥ 3 at 700-1360 nm |
| STO-LP1400 | 1400 ± 10 | T≥90% | 1420-1100 | OD ≥ 3 at 350-1380 nm |
| STO-LP1450 | 1450 ± 10 | T≥90% | 1480-1800 | OD ≥ 3 at 350-1420 nm |
| STO-LP1470 | 1470 ± 10 | T≥90% | 1500-1800 | OD ≥ 3 at 350-1400 nm |
| STO-LP1600 | 1600 ± 10 | T≥90% | 1625-2300 | OD ≥ 3 at 350-1540 nm |
Orta ve uzak kızılötesi dar bant geçiren filtreler, MWIR ve LWIR cihaz bantları için silikon, safir, germanyum, kalsiyum florür ve çinko selenür altlıklar kullanır. Dedektör modülleri ve termal algılama sistemleri için özel boyutlar mevcuttur.
| Model | IR bölgesi | Merkez dalga boyu (nm) | FWHM (nm) | Tepe geçirgenliği | Engelleme | Altlık | Boyut |
|---|---|---|---|---|---|---|---|
| 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 |
Geniş bant kızılötesi filtreler, termal görüntüleme, gaz analizi ve kızılötesi algılama için bant dışı engelleme sunarken MWIR ve LWIR aralıklarında daha geniş geçirgenlik pencerelerini kapsar.
| Model | IR bölgesi | Geçirgenlik aralığı (nm) | Ortalama geçirgenlik | Engelleme | Boyut | Altlık |
|---|---|---|---|---|---|---|
| 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 |
Kızılötesi uzun geçiren filtreler, dedektör tarafında yalıtım ve termal görüntüleme optik yolları için uzun dalga boylarını iletirken daha kısa dalga boyu enerjisini engeller.
| Model | IR bölgesi | Geçirgenlik aralığı (nm) | Ortalama geçirgenlik | Engelleme | Boyut | Altlık |
|---|---|---|---|---|---|---|
| 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 |
Kızılötesi yansıma önleyici kaplamalar, silikon, safir ve germanyum optiklerde yüzey yansımasını azaltarak sistem geçirgenliğini artırır.
| Kaplama | IR bölgesi | Geçirgenlik aralığı (nm) | Ortalama geçirgenlik | Boyut | Altlık |
|---|---|---|---|---|---|
| 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 |
Metalize kızılötesi pencereler, dedektör ve görüntüleme düzeneklerinde lehimleme veya hermetik paketleme için kaplamalı optik açıklık ve metalize kenarlar kullanır.
| Teknik özellik | IR bölgesi | Net açıklık | Metalize alan | Spektral teknik özellik | Altlık | Dış boyutlar |
|---|---|---|---|---|---|---|
| 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 |
FWHM değeri 10 nm'ye kadar olan ek IR bant geçiren filtre modelleri. Özette optik alanlar görünür tutulur; fiziksel boyutlar teklif incelemesine bırakılır.
| Model | Spektral aralık | Bant genişliği sınıfı | CWL (nm) | FWHM (nm) | Geçirgenlik | Engelleme | Altlık | Altlık kalınlığı (mm) |
|---|---|---|---|---|---|---|---|---|
| STO-BP2475±5 | SWIR | ultra-narrow | 2475 ± 5 | 10 ± 5 | T>=60% | 600-3000 nm; T < 1% | Borosilicate glass | 2 |
| STO-BP2490±5 | SWIR | ultra-narrow | 2490 ± 5 | 10 ± 5 | T>=60% | 600-3000 nm; T < 1% | Borosilicate glass | 2 |
FWHM değeri 10 nm'den büyük ve 20 nm'ye kadar olan, dalga boyu ve bant genişliğinin hızlı seçimi için gruplandırılmış ek IR bant geçiren filtre modelleri.
| Model | Spektral aralık | Bant genişliği sınıfı | CWL (nm) | FWHM (nm) | Geçirgenlik | Engelleme | Altlık | Altlık kalınlığı (mm) |
|---|---|---|---|---|---|---|---|---|
| STO-BP1440±20 | SWIR | narrow | 1440 ± 5 | 20 ± 10 | T>=70% | 400-2200 nm; T < 1% | White glass | 3 |
| STO-BP1645±5 | SWIR | narrow | 1645 ± 5 | 20 ± 5 | T>=90% | 800-2000 nm; T < 1% | Borosilicate glass | 0.5 |
| STO-BP1663±5 | SWIR | narrow | 1663 ± 5 | 20 ± 5 | T>=80% | 800-2000 nm; T < 1% | Borosilicate glass | 0.5 |
| STO-BP1697 | SWIR | narrow | 1697 ± 2 | 15 ± 2 | T>=85% | 800-2000 nm; T < 1% | Borosilicate glass | 0.5 |
| STO-BP1745±15 | SWIR | narrow | 1740 ± 5 | 20 ± 5 | T=55-65% | 400-2200 nm; T < 1.5% | White glass | 3 |
Daha geniş spektral seçim için FWHM değeri 20 nm'den büyük ek IR bant geçiren filtre modelleri.
| Model | Spektral aralık | Bant genişliği sınıfı | CWL (nm) | FWHM (nm) | Geçirgenlik | Engelleme | Altlık | Altlık kalınlığı (mm) |
|---|---|---|---|---|---|---|---|---|
| STO-BP900±30 | NIR | standard | 900 ± 30 | 70 ± 30 | T>=90% | 650-1250 nm; T < 1% | Sapphire | 3.5 |
| STO-BP1380±30 | SWIR | standard | 1380 ± 30 | 70 ± 30 | T>=85% | 500-2000 nm; T < 1% | Sapphire | 3.5 |
| STO-BP1600±16 | SWIR | standard | 1600 ± 16 | 150 ± 20 | T>=80% | 400-3000 nm; T < 1% | Corning 7980 | 2 |
| STO-BP1900±20 | SWIR | standard | 1900 ± 20 | 50 ± 15 | T>=80% | 400-3000 nm; T < 1% | White glass | 1 |
| STO-BP1940±18 | SWIR | standard | 1940 ± 18 | 45 ± 10 | T>=80% | 400-3000 nm; T < 1% | White glass | 1, 2 |
| STO-BP2010±20 | SWIR | standard | 2010 ± 20 | 180 ± 30 | T>=80% | 500-3000 nm; T < 1% | Sapphire | 3.5 |
| STO-BP2017±10 | SWIR | standard | 2017 ± 10 | 35 ± 10 | T>=55% | 400-15000 nm; T < 1% | Sapphire | 1 |
| STO-BP2050±20 | SWIR | standard | 2050 ± 20 | 200 ± 30 | T>=80% | 500-3000 nm; T < 1% | Sapphire | 3.5 |
| STO-BP2120±20 | SWIR | standard | 2120 ± 20 | 50 ± 10 | T>=80% | 400-3000 nm; T < 1% | White glass | 1 |
| STO-BP2220±20 | SWIR | standard | 2220 ± 20 | 45 ± 10 | T>=75% | 400-15000 nm; T < 1% | Sapphire | 1 |
| STO-BP2240±20 | SWIR | standard | 2240 ± 20 | 30 ± 10 | T>=80% | 400-3000 nm; T < 1% | White glass | 1 |
| STO-BP2250±10 | SWIR | standard | 2250 ± 10 | 30 ± 10 | T>=85% | 400-3000 nm; T < 1% | White glass | 1 |
| STO-BP2300±20 | SWIR | standard | 2300 ± 20 | 90 ± 10 | T>=90% | 400-3000 nm; T < 1% | White glass | 1 |
| STO-BP2310±20 | SWIR | standard | 2310 ± 20 | 90 ± 10 | T>=90% | 400-3000 nm; T < 1% | White glass | 1 |
| STO-BP2400±24 | SWIR | standard | 2400 ± 24 | 70 ± 30 | T>=75% | 500-3000 nm; T < 1% | Sapphire | 3.5 |
| STO-BP2435±10 | SWIR | standard | 2435 ± 10 | 60 ± 15 | T>=70% | 400-20000 nm; T < 1% | Sapphire | 1 |
| STO-BP2435±20 | SWIR | standard | 2435 ± 20 | 60 ± 15 | T>=70% | 400-20000 nm; T < 1% | Sapphire | 1 |
| STO-BP2460±20 | SWIR | standard | 2460 ± 20 | 50 ± 10 | T>=80% | 1500-15000 nm; T < 1% | Sapphire | 1 |
| STO-BP2470±30 | SWIR | standard | 2470 ± 30 | 50 ± 20 | T>=75% | 400-6000 nm; T < 1% | Silicon | 0.5 |
| STO-BP2500±25 | MWIR | standard | 2500 ± 25 | 70 ± 30 | T>=80% | 500-3000 nm; T < 1% | Sapphire | 1, 3.5 |
| STO-BP2520±10 | MWIR | standard | 2520 ± 10 | 50 ± 20 | T>=80% | 400-6000 nm; T < 1% | Silicon | 0.5 |
| STO-BP2530±30 | MWIR | standard | 2530 ± 30 | 50 ± 20 | T>=75% | 400-6000 nm; T < 1% | Silicon | 0.5 |
| STO-BP2550±50 | MWIR | standard | 2550 ± 50 | 70 ± 30 | T>=75% | 500-3000 nm; T < 1% | Sapphire | 1, 3.5 |
| STO-BP2560±30 | MWIR | standard | 2560 ± 30 | 50 ± 20 | T>=75% | 400-6000 nm; T < 1% | Silicon | 0.5 |
| STO-BP2570±30 | MWIR | standard | 2570 ± 30 | 50 ± 20 | T>=75% | 400-6000 nm; T < 1% | Silicon | 0.5 |
| STO-BP2580±30 | MWIR | standard | 2580 ± 30 | 50 ± 20 | T>=75% | 400-6000 nm; T < 1% | Silicon | 0.5 |
| STO-BP2600±10 | MWIR | standard | 2600 ± 10 | 50 ± 20 | T>=80% | 400-6000 nm; T < 1% | Silicon | 0.5 |
| STO-BP2600±30 | MWIR | standard | 2600 ± 30 | 50 ± 20 | T>=80% | 400-6000 nm; T < 1% | Silicon | 0.5 |
| STO-BP2610±30 | MWIR | standard | 2610 ± 30 | 50 ± 20 | T>=80% | 400-6000 nm; T < 1% | Silicon | 0.5 |
| STO-BP2720 | MWIR | standard | 2720 ± 50 | 140 ± 20 | T>=80% | 100-30000 nm; T < 1% | Fused silica | 1 |
| STO-BP2730±30 | MWIR | standard | 2730 ± 30 | 210 ± 20 | T>=80% | 400-6000 nm; T < 1% | Silicon | 1 |
| STO-BP2750±50 | MWIR | standard | 2750 ± 50 | 140 ± 20 | T>=80% | 200-30000 nm; T < 1% | Fused silica | 1 |
| STO-BP2850±28 | MWIR | standard | 2850 ± 28 | 86 ± 20 | T>=80% | 1500-5500 nm; T < 1% | Silicon | 0.5, 6.35 |
| STO-BP2900±20 | MWIR | standard | 2900 ± 20 | 50 ± 10 | T>=70% | 1500-15000 nm; T < 1% | Sapphire | 1 |
| STO-BP3030±40 | MWIR | standard | 3030 ± 40 | 145 ± 30 | T>=85% | 400-11000 nm | Silicon | 0.5 |
| STO-BP3050±50 | MWIR | standard | 3050 ± 50 | 100 ± 20 | T>=80% | 300-20000 nm; T < 1% | Sapphire | 1 |
| STO-BP3085±30 | MWIR | standard | 3085 ± 30 | 100 ± 20 | T>=80% | 300-30000 nm; T < 1% | Sapphire | 0.5, 1 |
| STO-BP3130±40 | MWIR | standard | 3130 ± 40 | 145 ± 30 | T>=85% | 400-11000 nm | Silicon | 0.5 |
| STO-BP3150±20 | MWIR | standard | 3150 ± 20 | 60 ± 10 | T>=80% | 1500-5500 nm; T < 1% | Fused silica | 0.5 |
| STO-BP3250±25 | MWIR | standard | 3250 ± 25 | 210 ± 10 | T>=80% | 400-3800 nm; T < 1% | Silicon | 0.25 |
| STO-BP3250±50 | MWIR | standard | 3250 ± 50 | 180 ± 20 | T>=80% | 400-10000 nm; T < 1% | Silicon | 0.5 |
| STO-BP3275±20 | MWIR | standard | 3275 ± 10 | 30 ± 10 | T>=70% | 400-11000 nm; T < 1% | Silicon | 1 |
| STO-BP3280±30 | MWIR | standard | 3280 ± 30 | 210 ± 15 | T>=75% | 400-3800 nm; T < 1% | Silicon | 0.25 |
| STO-BP3315±10 | MWIR | standard | 3315 ± 10 | 210 ± 10 | T>=80% | 400-3800 nm; T < 1% | Silicon | 0.25 |
| STO-BP3320±50单 | MWIR | standard | 3320 ± 50 | 190 ± 20 | T>=60% | 800-6000 nm; T < 1% | Silicon | 0.5 |
| STO-BP3330±15 | MWIR | standard | 3330 ± 15 | 160 ± 20 | T>=85% | 400-11000 nm; T < 1% | Silicon | 0.5 |
| STO-BP3360±20 | MWIR | standard | 3360 ± 20 | 70 ± 10 | T>=80% | 1500-6500 nm; T < 1% | Fused silica | 0.5 |
| STO-BP3370±35 | MWIR | standard | 3370 ± 35 | 660 ± 70 | T>=80% | 400-3800 nm; T < 1% | Silicon | 0.25, 0.38 |
| STO-BP3370±50 | MWIR | standard | 3370 ± 50 | 400 ± 30 | T>=80% | 1000-6000 nm; T < 1% | Silicon | 0.5 |
| STO-BP3375±20 | MWIR | standard | 3375 ± 20 | 180 ± 20 | T>=80% | 400-11000 nm; T < 1% | Silicon | 0.5, 1 |
| STO-BP3375±40 | MWIR | standard | 3375 ± 40 | 660 ± 70 | T>=85% | 400-7000 nm; T < 1% | Silicon | 0.25 |
| STO-BP3390±35 | MWIR | standard | 3390 ± 35 | 210 ± 10 | T>=80% | 400-7000 nm; T < 1% | Silicon | 0.25 |
| STO-BP3416±20 | MWIR | standard | 3416 ± 20 | 120 ± 20 | T>=80% | 400-11000 nm; T < 1% | Silicon | 0.5 |
| STO-BP3430±40 | MWIR | standard | 3430 ± 40 | 120 ± 20 | T>=75% | 400-11000 nm; T < 1% | Silicon | 0.5 |
| STO-BP3440±30 | MWIR | standard | 3440 ± 30 | 120 ± 10 | T>=80% | 400-10000 nm; T < 1% | Silicon | 0.5 |
| STO-BP3580±40 | MWIR | standard | 3580 ± 40 | 160 ± 20 | T>=80% | 400-20000 nm; T < 1% | Sapphire | 0.5 |
| STO-BP3615±20 | MWIR | standard | 3615 ± 20 | 160 ± 20 | T>=80% | 400-20000 nm; T < 1% | Sapphire | 0.5, 1 |
| STO-BP3630±50 | MWIR | standard | 3630 ± 50 | 145 ± 20 | T>=80% | 400-15000 nm; T < 1% | Sapphire | 0.5, 1 |
| STO-BP3660±20 | MWIR | standard | 3660 ± 20 | 40 ± 10 | T>=80% | 800-6000 nm; T < 1% | Silicon | 0.5, 0.916 |
| STO-BP3680±40 | MWIR | standard | 3680 ± 40 | 162 ± 24 | T>=85% | 400-11000 nm | Silicon | 0.5 |
| STO-BP3770±20 | MWIR | standard | 3770 ± 20 | 50 ± 10 | T>=80% | 400-13600 nm; T < 1% | Sapphire | 0.5 |
| STO-BP3940±60 | MWIR | standard | 3940 ± 60 | 90 ± 20 | T>=80% | 1000-9000 nm; T < 1% | Silicon | 0.5 |
| STO-BP3950±39 | MWIR | standard | 3950 ± 39 | 200 ± 20 | T>=85% | 400-8000 nm; T < 1% | Silicon | 0.5 |
| STO-BP3990±50 | MWIR | standard | 3990 ± 50 | 180 ± 20 | T>=80% | 400-11000 nm; T < 1% | Silicon | 0.5 |
| STO-BP4020±40 | MWIR | standard | 4020 ± 40 | 180 ± 20 | T>=80% | 400-11000 nm; T < 1% | Silicon | 0.5 |
| STO-BP4050±50 | MWIR | standard | 4050 ± 50 | 100 ± 20 | T>=80% | 400-11000 nm; T < 1% | Silicon | 0.5 |
| STO-BP4060±50 | MWIR | standard | 4060 ± 50 | 100 ± 20 | T>=80% | 400-6000 nm; T < 1% | Silicon | 0.5 |
| STO-BP4073±40 | MWIR | standard | 4073 ± 40 | 125 ± 50 | T>=85% | 400-11000 nm | Silicon | 0.5 |
| STO-BP4260±50 | MWIR | standard | 4260 ± 50 | 180 ± 20 | T>=80% | 400-11000 nm; T < 1% | Silicon | 0.5 |
| STO-BP4320±50 | MWIR | standard | 4320 ± 50 | 600 ± 40 | T>=80% | 400-11000 nm; T < 1% | Silicon | 0.5 |
| STO-BP4380±50 | MWIR | standard | 4380 ± 50 | 150 ± 20 | T>=80% | 1000-9000 nm; T < 1% | Silicon | 0.5 |
| STO-BP4490±70 | MWIR | standard | 4490 ± 70 | 180 ± 20 | T>=70% | 400-11000 nm; T < 1% | Silicon | 0.5 |
| STO-BP4515±20 | MWIR | standard | 4515 ± 20 | 90 ± 20 | T>=75% | 200-30000 nm; T < 1% | Sapphire | 1 |
| STO-BP4530±45 | MWIR | standard | 4530 ± 45 | 350 ± 20 | T>=80% | 400-20000 nm; T < 1% | Sapphire | 0.3, 0.5 |
| STO-BP4560±40 | MWIR | standard | 4560 ± 40 | 310 ± 20 | T>=80% | 400-11000 nm; T < 1% | Silicon | 0.5 |
| STO-BP4580±60 | MWIR | standard | 4580 ± 60 | 140 ± 20 | T>=70% | 400-10000 nm; T < 1% | Silicon | 1 |
| STO-BP4680±50 | MWIR | standard | 4680 ± 50 | 180 ± 20 | T>=75% | 400-11000 nm; T < 1% | Silicon | 1 |
| STO-BP4680±55 | MWIR | standard | 4680 ± 55 | 180 ± 20 | T>=70% | 400-11000 nm; T < 1% | Silicon | 1 |
| STO-BP4680±60 | MWIR | standard | 4680 ± 60 | 180 ± 20 | T>=75% | 400-11000 nm; T < 1% | Silicon | 1 |
| STO-BP4710±20 | MWIR | standard | 4710 ± 20 | 140 ± 20 | T>=75% | 400-11000 nm; T < 1% | Silicon | 1 |
| STO-BP4710±40 | MWIR | standard | 4710 ± 40 | 180 ± 20 | T>=75% | 400-20000 nm; T < 1% | Sapphire | 1 |
| STO-BP4760±50 | MWIR | standard | 4760 ± 50 | 285 ± 70 | T>=80% | 400-11000 nm | Silicon | 0.5 |
| STO-BP4830±40 | MWIR | standard | 4830 ± 40 | 220 ± 20 | T>=75% | 400-11000 nm; T < 1% | Germanium | 1 |
| STO-BP5000±50 | MWIR/LWIR transition | standard | 5000 ± 50 | 150 ± 20 | T>=85% | 1000-10000 nm; T < 1% | Silicon | 1.5 |
| STO-BP5010±50 | MWIR/LWIR transition | standard | 5010 ± 50 | 220 ± 20 | T>=80% | 400-11000 nm; T < 1% | Silicon | 0.5 |
| STO-BP5070±40 | MWIR/LWIR transition | standard | 5070 ± 50 | 100 ± 20 | T>=75% | 400-20000 nm; T < 1% | Sapphire | 0.5, 1 |
| STO-BP5120±50 | MWIR/LWIR transition | standard | 5120 ± 50 | 320 ± 20 | T>=70% | 400-5500 nm; T < 1% | Silicon | 1 |
| STO-BP5200±50 | MWIR/LWIR transition | standard | 5200 ± 50 | 610 ± 40 | T>=80% | 400-11000 nm; T < 1% | Silicon | 1 |
| STO-BP5250±50 | MWIR/LWIR transition | standard | 5250 ± 50 | 90 ± 20 | T>=80% | 400-11000 nm; T < 1% | Silicon | 0.5, 1 |
| STO-BP5380±30 | MWIR/LWIR transition | standard | 5380 ± 30 | 100 ± 20 | T>=65% | 400-15000 nm; T < 1% | Sapphire | 1 |
| STO-BP5450±30 | MWIR/LWIR transition | standard | 5450 ± 30 | 100 ± 20 | T>=65% | 400-15000 nm; T < 1% | Sapphire | 1 |
| STO-BP5480±30 | MWIR/LWIR transition | standard | 5480 ± 30 | 100 ± 20 | T>=65% | 400-15000 nm; T < 1% | Sapphire | 1 |
| STO-BP5600±60 | MWIR/LWIR transition | standard | 5600 ± 60 | 120 ± 20 | T>=80% | 1000-10000 nm | Silicon | 1.5 |
| STO-BP5850±50 | MWIR/LWIR transition | standard | 5850 ± 50 | 200 ± 20 | T>=70% | 400-11000 nm; T < 1% | Silicon | 1 |
| STO-BP5850±60 | MWIR/LWIR transition | standard | 5850 ± 60 | 160 ± 20 | T>=75% | 1000-10000 nm; T < 1% | Silicon | 1.5 |
| STO-BP5950±50 | MWIR/LWIR transition | standard | 5950 ± 50 | 200 ± 20 | T>=70% | 1000-10000 nm; T < 1% | Silicon | 0.5 |
| STO-BP6050±50 | MWIR/LWIR transition | standard | 6050 ± 50 | 200 ± 20 | T>=75% | 1000-10000 nm; T < 1% | Silicon | 1.5 |
| STO-BP6150±60 | MWIR/LWIR transition | standard | 6150 ± 60 | 200 ± 20 | T>=70% | 1000-10000 nm; T < 1% | Silicon | 1.5 |
| STO-BP6220±30 | MWIR/LWIR transition | standard | 6220 ± 62 | 140 ± 20 | T>=80% | 400-11000 nm; T < 1% | Silicon | 0.5 |
| STO-BP6235±30 | MWIR/LWIR transition | standard | 6235 ± 30 | 110 ± 20 | T>=60% | 400-11000 nm; T < 1% | Germanium | 0.9, 1 |
| STO-BP6240±40 | MWIR/LWIR transition | standard | 6240 ± 40 | 90 ± 20 | T>=70% | 400-11000 nm; T < 1% | Germanium | 1 |
| STO-BP6250±30 | MWIR/LWIR transition | standard | 6250 ± 30 | 120 ± 20 | T>=70% | 400-15000 nm; T < 1% | Silicon | 1 |
| STO-BP6820±68 | MWIR/LWIR transition | standard | 6820 ± 68 | 100 ± 20 | T>=75% | 400-10600 nm; T < 1% | Silicon | 1 |
| STO-BP6910±20 | MWIR/LWIR transition | standard | 6910 ± 30 | 90 ± 20 | T>=65% | 400-11000 nm; T < 1% | Silicon | 0.5 |
| STO-BP7400±50 | MWIR/LWIR transition | standard | 7400 ± 50 | 360 ± 20 | T>=80% | 400-10600 nm; T < 1% | Silicon | 0.5 |
| STO-BP7500±50 | MWIR/LWIR transition | standard | 7500 ± 50 | 2500 ± 100 | T>=90% | 400-17100 nm; T < 1% | Germanium | 0.6 |
| STO-BP7530±30 | MWIR/LWIR transition | standard | 7530 ± 30 | 180 ± 30 | T>=80% | 400-10600 nm; T < 1% | Silicon | 0.5, 1 |
| STO-BP7690±50 | MWIR/LWIR transition | standard | 7690 ± 50 | 340 ± 30 | T>=70% | 200-16000 nm; T < 1% | Silicon | 1 |
| STO-BP7700±50 | MWIR/LWIR transition | standard | 7700 ± 50 | 450 ± 30 | T>=80% | 200-16000 nm; T < 1% | Silicon | 1 |
| STO-BP7720±50 | MWIR/LWIR transition | standard | 7720 ± 50 | 180 ± 30 | T>=80% | 400-10600 nm; T < 1% | Silicon | 0.5, 1 |
| STO-BP7760±50 | MWIR/LWIR transition | standard | 7760 ± 50 | 500 ± 30 | T>=80% | 200-13500 nm; T < 1% | Silicon | 0.5 |
| STO-BP7780±20 | MWIR/LWIR transition | standard | 7780 ± 20 | 180 ± 30 | T>=80% | 400-10600 nm; T < 1% | Silicon | 0.5, 1 |
| STO-BP7800±50 | MWIR/LWIR transition | standard | 7800 ± 50 | 450 ± 30 | T>=80% | 200-16000 nm; T < 1% | Silicon | 1 |
| STO-BP7890±80 | MWIR/LWIR transition | standard | 7890 ± 80 | 500 ± 30 | T>=80% | 200-13500 nm; T < 1% | Silicon | 0.5 |
| STO-BP7950±50 | MWIR/LWIR transition | standard | 7950 ± 50 | 450 ± 30 | T>=75% | 200-16000 nm; T < 1% | Silicon | 1 |
| STO-BP7950±80 | MWIR/LWIR transition | standard | 7950 ± 80 | 250 ± 20 | T>75% | 400-11000 nm; T < 1% | Silicon | 0.5 |
| STO-BP8010±20 | LWIR | standard | 8010 ± 20 | 200 ± 20 | T>90% | 400-11000 nm; T < 1% | Silicon | 0.5 |
| STO-BP8060±60 | LWIR | standard | 8060 ± 60 | 250 ± 20 | T>80% | 400-11000 nm; T < 1% | Silicon | 0.5 |
| STO-BP8120±30 | LWIR | standard | 8120 ± 30 | 250 ± 20 | T>90% | 400-11000 nm; T < 1% | Silicon | 0.5 |
| STO-BP8340±30 | LWIR | standard | 8340 ± 30 | 250 ± 20 | T>75% | 400-11000 nm; T < 1% | Silicon | 0.5 |
| STO-BP8350±100 | LWIR | standard | 8350 ± 100 | 45 ± 10 | T>70% | 400-13600 nm; T < 1% | Silicon | 0.5 |
| STO-BP8400±100 | LWIR | standard | 8400 ± 100 | 50 ± 20 | T>70% | 400-13600 nm; T < 1% | Silicon | 0.5 |
| STO-BP8500±100 | LWIR | standard | 8500 ± 100 | 50 ± 10 | T>70% | 400-13600 nm; T < 1% | Silicon | 0.5 |
| STO-BP8550±100 | LWIR | standard | 8550 ± 100 | 45 ± 10 | T>70% | 400-13600 nm; T < 1% | Silicon | 0.5 |
| STO-BP8700±100 | LWIR | standard | 8700 ± 100 | 210 ± 30 | T>=75% | 400-13600 nm; T < 1% | Silicon | 0.5 |
| STO-BP8800±100 | LWIR | standard | 8800 ± 100 | 210 ± 30 | T>=75% | 400-13600 nm; T < 1% | Silicon | 0.5 |
| STO-BP10100±100 | LWIR | standard | 10100 ± 100 | 660 ± 40 | T>=85% | 400-14000 nm; T < 1% | Germanium | 1 |
| STO-BP10220±100 | LWIR | standard | 10220 ± 100 | 660 ± 40 | T>=85% | 400-14000 nm; T < 1% | Germanium | 1 |
| STO-BP10580±50 | LWIR | standard | 10580 ± 50 | 250 ± 20 | T>=70% | 400-18000 nm; T < 1% | Silicon | 0.5 |
| STO-BP10860±150 | LWIR | standard | 10860 ± 150 | 640 ± 50 | T>=70% | 400-14000 nm; T < 1% | Silicon | 0.5 |
| STO-BP11100±150 | LWIR | standard | 11100 ± 150 | 640 ± 50 | T>=70% | 400-14000 nm; T < 1% | Silicon | 0.5 |
| STO-BP11200±150 | LWIR | standard | 11200 ± 150 | 640 ± 50 | T>=70% | 400-14000 nm; T < 1% | Silicon | 0.5 |
| STO-BP11500±50 | LWIR | standard | 11500 ± 50 | 550 ± 50 | T>=65% | 400-18000 nm; T < 1% | Silicon | 0.5 |
| STO-BP11580±60 | LWIR | standard | 11580 ± 60 | 550 ± 50 | T>=70% | 400-18000 nm; T < 1% | Silicon | 0.5 |
| STO-BP12600±100 | LWIR | standard | 12600 ± 100 | 800 ± 40 | T>=85% | 400-15000 nm; T < 1% | Germanium | 1 |
| STO-BP12750±100 | LWIR | standard | 12750 ± 100 | 800 ± 40 | T>=85% | 400-15000 nm; T < 1% | Germanium | 1 |
| STO-BP13000±100 | LWIR | standard | 13000 ± 100 | 4000 ± 100 | T>=85% | 1200-20000 nm; T < 1% | Germanium | 0.75, 0.9 |
| STO-BP13250±100 | LWIR | standard | 13250 ± 100 | 850 ± 50 | T>=85% | 400-15000 nm; T < 1% | Germanium | 1 |
| STO-BP13650±100 | LWIR | standard | 13650 ± 100 | 850 ± 50 | T>=80% | 400-15000 nm; T < 1% | Germanium | 0.5 |
| STO-BP15000±200 | LWIR | standard | 15000 ± 200 | 2200 ± 50 | T>=65% | 2000-25000 nm; T < 1% | Germanium | 2.2 |
| STO-BP16000±200 | LWIR | standard | 16000 ± 200 | 2400 ± 50 | T>=70% | 2000-25000 nm; T < 1% | Germanium | 1 |
| STO-BP16200±200 | LWIR | standard | 16200 ± 200 | 2400 ± 50 | T>=70% | 2000-25000 nm; T < 1% | Germanium | 1 |
MWIR ve LWIR dedektör yollarında algılama ve görüntüleme için ek geniş bant modeller.
| Model | Spektral aralık | Geçiş bandı (nm) | Geçirgenlik aralığı (nm) | Geçirgenlik | Engelleme | Altlık | Altlık kalınlığı (mm) |
|---|---|---|---|---|---|---|---|
| STO-WBP1000~3000 | SWIR | 970 ± 100 – 2470 ± 100 | 1100-2300 | T>=90% | 200-3560 nm; T < 1% | Glass ceramic | 1 |
| STO-WBP1520~1850 | SWIR | 1520 ± 50 – 1850 ± 50 | 1600-1750 | T>=80% | 400-3300 nm; T < 1% | Silicon | 0.5, 1 |
| STO-WBP1550~1750 | SWIR | 1550 ± 50 – 1750 ± 50 | 1600-1700 | T>=80% | 1500-2800 nm; T < 1% | Silicon | 1.2 |
| STO-WBP1550~5050 | MWIR | 1550 ± 50 – 5050 ± 50 | 1600-5000 | T>=80% | 1500-5580 nm; T < 1% | Silicon | 1.2 |
| STO-WBP1650~2350 | SWIR | 1650 ± 50 – 2350 ± 50 | 1700-2250 | T>=80% | 400-4000 nm; T < 10% | Silicon | 0.5 |
| STO-WBP2050~2350 | SWIR | 2050 ± 50 – 2350 ± 50 | 2150-2250 | T>=80% | 1500-2800 nm; T < 1% | Silicon | 0.5, 1, 1.2 |
| STO-WBP2050~2500 | SWIR | 2050 ± 50 – 2500 ± 50 | 2150-2450 | T>=80% | 1500-5000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP2080~2350 | SWIR | 2080 ± 50 – 2350 ± 50 | 2135-2330 | T>=80% | 1500-2800 nm; T < 1% | Silicon | 1.2 |
| STO-WBP2080~2430 | SWIR | 2080 ± 50 – 2430 ± 50 | 2180-2330 | T>=80% | 1500-2800 nm; T < 1% | Silicon | 0.5, 1 |
| STO-WBP2170~3670 | MWIR | 2170 ± 50 – 3670 ± 50 | 2300-3600 | T>=85% | 1500-5000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP2300~3600 | MWIR | 2200 ± 50 – 3750 ± 50 | 2300-3600 | T>=85% | 1500-5000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP2300~3700 | MWIR | 2250 ± 30 – 3770 ± 30 | 2300-3700 | T>=90% | 1500-5000 nm; T < 1% | Silicon | 1 |
| STO-WBP2400~3150 | MWIR | 2400 ± 50 – 3150 ± 50 | 2500-3000 | T>=90% | 400-10500 nm; T < 1% | Sapphire | 1, 5 |
| STO-WBP2450~3200 | MWIR | 2450 ± 20 – 3200 ± 20 | 2500-3140 | T>=90% | 1500-7000 nm; T < 1% | Germanium | 2.5 |
| STO-WBP2450~4600 | MWIR | 2450 ± 50 – 4600 ± 50 | 2550-4500 | T>=90% | 400-7000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP2450~5150 | MWIR | 2450 ± 50 – 5150 ± 50 | 2640-5040 | T>=90% | 400-7040 nm; T < 1% | Silicon | 1 |
| STO-WBP2490~5240 | MWIR | 2490 ± 50 – 5240 ± 50 | 2640-5040 | T>=90% | 400-7040 nm; T < 1% | Silicon | 1 |
| STO-WBP2600~5000 | MWIR | 2490 ± 50 – 5240 ± 50 | 2640-5040 | T>=90% | 400-7040 nm; T < 1% | Germanium | 0.5, 0.9, 1 |
| STO-WBP2500-5000 | MWIR | 2500 ± 50 – 5000 ± 50 | 2700-4900 | T>=90% | 200-10000 nm; T < 1% | Germanium | 0.9, 1.8 |
| STO-WBP2500~5100 | MWIR | 2500 ± 50 – 5100 ± 50 | 2650-4950 | T>=90% | 1500-10500 nm; T < 1% | Germanium | 0.3, 0.7 |
| STO-WBP2550~3150 | MWIR | 2550 ± 50 – 3150 ± 50 | 2700-3100 | T>=85% | 1500-5000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP2550~3250 | MWIR | 2550 ± 50 – 3250 ± 50 | 2700-3100 | T>=90% | 430-10030 nm; T < 1% | Silicon | 0.5, 2.5 |
| STO-WBP2600~3300 | MWIR | 2600 ± 50 – 3300 ± 50 | 2850-3000 | T>=85% | 400-10000 nm; T < 1% | Germanium | 0.7 |
| STO-WBP2650~5050 | MWIR | 2600 ± 100 – 5050 ± 50 | 2750-4950 | T>=90% | 1500-8000 nm; T < 1% | Silicon | 0.5, 1 |
| STO-WBP2650~3000 | MWIR | 2650 ± 40 – 3000 ± 40 | 2700-2950 | T>=85% | 1000-6000 nm; T < 1% | Germanium | 1.8 |
| STO-WBP2700-3550 | MWIR | 2700 ± 50 – 3550 ± 50 | 2800-3450 | T>=90% | 300-20000 nm; T < 1% | Sapphire | 1 |
| STO-WBP2700-3600 | MWIR | 2700 ± 50 – 3600 ± 50 | 2800-3500 | T>=90% | 300-20000 nm; T < 1% | Sapphire | 0.5, 1 |
| STO-WBP2700~3150 | MWIR | 2700 ± 50 – 3150 ± 50 | 2800-3050 | T>=80% | 1500-5000 nm; T < 1% | Germanium | 1 |
| STO-WBP2720~2980 | MWIR | 2720 ± 20 – 2980 ± 20 | 2780-2920 | T>=80% | 1500-5000 nm; T < 1% | Germanium | 1 |
| STO-WBP2730~3010 | MWIR | 2730 ± 20 – 3010 ± 20 | 2800-2900 | T>=85% | 1500-5000 nm; T < 1% | Germanium | 1 |
| STO-WBP2750~4850 | MWIR | 2750 ± 50 – 4850 ± 50 | 3000-4600 | T>=85% | 1000-5100 nm; T < 1% | Germanium | 0.3, 0.4, 1 |
| STO-WBP2750~5100 | MWIR | 2750 ± 50 – 5100 ± 50 | 2900-5000 | T>=90% | 1500-10500 nm; T < 1% | Germanium | 0.3, 0.7 |
| STO-WBP2790~3070 | MWIR | 2790 ± 20 – 3070 ± 20 | 2900-3000 | T>=80% | 1500-5000 nm; T < 1% | Germanium | 0.9, 1 |
| STO-WBP2800~3050 | MWIR | 2800 ± 50 – 3050 ± 50 | 2900-3000 | T>=90% | 1500-6500 nm; T < 1% | Silicon | 0.5 |
| STO-WBP2800~5150 | MWIR | 2800 ± 50 – 5150 ± 50 | 2950-5000 | T>=90% | 1500-10500 nm; T < 1% | Germanium | 0.3, 0.9 |
| STO-WBP2800~5200单 | MWIR | 2800 ± 100 – 5200 ± 100 | 2900-5100 | T>=55% | 2580-8000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP2800~5250 | MWIR | 2800 ± 50 – 5250 ± 50 | 2950-5100 | T>=90% | 1500-10500 nm; T < 1% | Germanium | 0.3 |
| STO-WBP2900~4140 | MWIR | 2900 ± 50 – 4140 ± 50 | 3100-4040 | T>=90% | 700-8040 nm; T < 1% | Germanium | 0.3 |
| STO-WBP2900~4450 | MWIR | 2900 ± 50 – 4450 ± 50 | 3050-4350 | T>=85% | 1500-10000 nm; T < 1% | Germanium | 0.9 |
| STO-WBP2900~4550 | MWIR | 2900 ± 50 – 4550 ± 50 | 3050-4450 | T>=85% | 1500-10000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP2900~4850 | MWIR | 2900 ± 50 – 4850 ± 50 | 3050-4750 | T>=90% | 400-11000 nm; T < 1% | Silicon | 0.5, 1 |
| STO-WBP2900~5100 | MWIR | 2900 ± 50 – 5100 ± 50 | 3000-5000 | T>=90% | 1000-10500 nm; T < 1% | Germanium | 0.3, 0.4, 0.7 |
| STO-WBP2950~3250 | MWIR | 2950 ± 50 – 3250 ± 50 | 3000-3200 | T>=85% | 200-20000 nm; T < 1% | Sapphire | 1 |
| STO-WBP2950~3600 | MWIR | 2950 ± 50 – 3600 ± 50 | 3150-3400 | T>=85% | 1000-10500 nm; T < 1% | Germanium | 0.6, 0.9 |
| STO-WBP2950~3650 | MWIR | 2950 ± 50 – 3650 ± 50 | 3150-3450 | T>=85% | 1000-10500 nm; T < 1% | Germanium | 0.6, 0.9 |
| STO-WBP2950~4950 | MWIR | 2950 ± 50 – 4950 ± 50 | 3100-4800 | T>=90% | 400-11000 nm; T < 1% | Silicon | 0.5, 1 |
| STO-WBP3000~3300 | MWIR | 3000 ± 20 – 3300 ± 20 | 3050-3250 | T>=85% | 200-20000 nm; T < 1% | Sapphire | 0.5, 1 |
| STO-WBP3000~3700 | MWIR | 3000 ± 50 – 3700 ± 50 | 3100-3600 | T>=90% | 200-10000 nm; T < 1% | Germanium | 1.8 |
| STO-WBP3000~3800 | MWIR | 3000 ± 100 – 3800 ± 100 | 3100-3700 | T>=80% | 400-14000 nm; T < 1% | Sapphire | 0.5 |
| STO-WBP3000~3875 | MWIR | 3000 ± 100 – 3875 ± 75 | 3250-3650 | T>=80% | 500-5500 nm; T < 1% | Sapphire | 0.3, 0.5 |
| STO-WBP3000~4260 | MWIR | 3000 ± 50 – 4260 ± 50 | 3250-3900 | T>=80% | 400-11000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3000~4300 | MWIR | 3000 ± 50 – 4300 ± 50 | 3250-3900 | T>=80% | 400-11000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3000~5300 | MWIR | 3000 ± 50 – 5300 ± 50 | 3150-5150 | T>=85% | 1500-15500 nm; T < 1% | Sapphire | 0.3, 0.75, 1 |
| STO-WBP3000~5400 | MWIR | 3000 ± 50 – 5400 ± 50 | 3100-5300 | T>=90% | 1500-2800 nm; T < 1% | Germanium | 0.7, 1 |
| STO-WBP3020~3320 | MWIR | 3020 ± 20 – 3320 ± 20 | 3050-3250 | T>=85% | 200-20000 nm; T < 1% | Sapphire | 1 |
| STO-WBP3040~4320 | MWIR | 3040 ± 50 – 4320 ± 50 | 3250-4050 | T>=85% | 400-11000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3050~4200 | MWIR | 3050 ± 50 – 4200 ± 50 | 3250-3900 | T>=85% | 400-11000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3050~5000 | MWIR | 3050 ± 50 – 5000 ± 50 | 3200-4850 | T>=85% | 1500-10000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3050~5450 | MWIR | 3050 ± 50 – 5450 ± 50 | 3200-5300 | T>=85% | 1500-15500 nm; T < 1% | Sapphire | 0.3, 0.75, 1 |
| STO-WBP3100~3700 | MWIR | 3100 ± 150 – 3700 ± 150 | 3200-3600 | T>=90% | 400-20000 nm; T < 1% | Sapphire | 1 |
| STO-WBP3100~4100 | MWIR | 3100 ± 50 – 4100 ± 50 | 3300-3900 | T>=90% | 900-8000 nm; T < 1% | Germanium | 0.3, 0.9 |
| STO-WBP3100~4150 | MWIR | 3100 ± 50 – 4150 ± 50 | 3250-4050 | T>=90% | 1500-10600 nm; T < 1% | Germanium | 0.4 |
| STO-WBP3100~4200 | MWIR | 3100 ± 50 – 4200 ± 50 | 3250-4050 | T>=85% | 1500-11000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3100~4250 | MWIR | 3100 ± 50 – 4250 ± 50 | 3250-3900 | T>=80% | 400-11000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3130~3400 | MWIR | 3130 ± 50 – 3400 ± 50 | 3250-3350 | T>=75% | 500-3700 nm; T < 1% | Germanium | 0.9 |
| STO-WBP3150~3560 | MWIR | 3150 ± 50 – 3560 ± 50 | 3300-3500 | T>=85% | 400-10000 nm; T < 1% | Sapphire | 0.3 |
| STO-WBP3150~3600 | MWIR | 3150 ± 50 – 3600 ± 50 | 3250-3520 | T>=90% | 1500-6000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP3150~3650 | MWIR | 3150 ± 50 – 3650 ± 50 | 3250-3500 | T>=90% | 1500-6000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP3150~4100 | MWIR | 3150 ± 50 – 4100 ± 50 | 3250-4000 | T>=80% | 1500-10000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3150~4200 | MWIR | 3150 ± 50 – 4200 ± 50 | 3300-4100 | T>=90% | 1500-10600 nm; T < 1% | Germanium | 0.3 |
| STO-WBP3150~5150 | MWIR | 3150 ± 50 – 5150 ± 50 | 3300-5000 | T>=85% | 1500-10000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3180-3420 | MWIR | 3180 ± 50 – 3420 ± 50 | 3200-3380 | T>=85% | 450-5600 nm; T < 1% | Zinc selenide | 1.5, 2 |
| STO-WBP3180~3420 | MWIR | 3180 ± 50 – 3420 ± 50 | 3200-3400 | T>=80% | 400-7000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3200~3500 | MWIR | 3200 ± 50 – 3500 ± 50 | 3250-3450 | T>=85% | 500-3700 nm; T < 1% | Germanium | 0.3 |
| STO-WBP3200~3550 | MWIR | 3200 ± 50 – 3550 ± 50 | 3280-3480 | T>=90% | 500-7000 nm; T < 1% | Germanium | 0.7, 0.9 |
| STO-WBP3200~4000 | MWIR | 3200 ± 50 – 4000 ± 50 | 3350-3850 | T>=90% | 500-10000 nm; T < 1% | Silicon | 4 |
| STO-WBP3200~4100 | MWIR | 3200 ± 50 – 4100 ± 50 | 3300-4000 | T>=85% | 400-11000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3200~5200 | MWIR | 3200 ± 100 – 5200 ± 100 | 3300-5050 | T>=80% | 1500-7000 nm; T < 1% | Silicon | 0.3 |
| STO-WBP3170~3430 | MWIR | 3220 ± 20 – 3480 ± 20 | 3300-3430 | T>=85% | 450-6050 nm; T < 1% | Germanium | 0.3, 0.9, 1 |
| STO-WBP3230~3500 | MWIR | 3230 ± 50 – 3500 ± 50 | 3250-3480 | T>=80% | 400-7000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3230~3520 | MWIR | 3230 ± 30 – 3520 ± 30 | 3300-3430 | T>=85% | 450-6050 nm; T < 1% | Germanium | 0.3 |
| STO-WBP3250~4200 | MWIR | 3250 ± 50 – 4200 ± 50 | 3400-4100 | T>=85% | 1500-10600 nm; T < 1% | Germanium | 0.3, 0.4, 1 |
| STO-WBP3270~3470 | MWIR | 3270 ± 50 – 3470 ± 50 | 3320-3420 | T>=80% | 200-7000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP3300~4250 | MWIR | 3300 ± 50 – 4250 ± 50 | 3450-4150 | T>=85% | 1500-10600 nm; T < 1% | Germanium | 0.4 |
| STO-WBP3300~4900 | MWIR | 3300 ± 50 – 4900 ± 50 | 3400-4800 | T>=90% | 500-8000 nm; T < 1% | Germanium | 0.3, 0.9 |
| STO-WBP3400~3600 | MWIR | 3325 ± 25 – 3675 ± 25 | 3450-3550 | T>=90% | 900-6000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP3350~4250 | MWIR | 3350 ± 50 – 4250 ± 50 | 3550-4150 | T>=90% | 430-10030 nm; T < 1% | Silicon | 2.5 |
| STO-WBP3350~4500 | MWIR | 3350 ± 50 – 4500 ± 50 | 3500-4350 | T>=90% | 1500-7000 nm; T < 1% | Germanium | 0.7 |
| STO-WBP3350~4750 | MWIR | 3350 ± 50 – 4750 ± 50 | 3450-4650 | T>=90% | 1500-8000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3400~4000 | MWIR | 3400 ± 50 – 4000 ± 50 | 3500-3850 | T>=90% | 200-10000 nm; T < 1% | Germanium | 1.8 |
| STO-WBP3400~4100 | MWIR | 3400 ± 100 – 4100 ± 100 | 3550-4000 | T>=90% | 1500-10600 nm; T < 1% | Germanium | 0.4 |
| STO-WBP3400~4200 | MWIR | 3400 ± 100 – 4200 ± 100 | 3550-4100 | T>=90% | 1500-10600 nm; T < 1% | Germanium | 0.5, 1 |
| STO-WBP3400~4300 | MWIR | 3400 ± 50 – 4300 ± 50 | 3500-4200 | T>=80% | 1500-7000 nm; T < 1% | Sapphire | 2.5 |
| STO-WBP3400~4800 | MWIR | 3400 ± 50 – 4800 ± 50 | 3500-4700 | T>=90% | 1500-8000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3400~4850 | MWIR | 3400 ± 50 – 4850 ± 50 | 3400-4500 | T>=90% | 1500-10000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3400~4950 | MWIR | 3400 ± 50 – 4950 ± 50 | 3700-4700 | T>=90% | 1500-10000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3400~5000 | MWIR | 3400 ± 50 – 5000 ± 50 | 3500-4900 | T>=90% | 1500-10600 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3400~5100 | MWIR | 3400 ± 50 – 5100 ± 50 | 3600-5000 | T>=90% | 1500-10600 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3420~3910 | MWIR | 3420 ± 50 – 3910 ± 50 | 3500-3830 | T>=80% | 400-6000 nm; T < 1% | Silicon | 0.5, 1 |
| STO-WBP3425~4850 | MWIR | 3425 ± 75 – 4850 ± 50 | 3650-4750 | T>=85% | 1500-7000 nm; T < 1% | Germanium | 0.3, 0.9 |
| STO-WBP3440~4890 | MWIR | 3440 ± 50 – 4890 ± 50 | 3500-4830 | T>=90% | 540-10040 nm; T < 1% | Germanium | 0.3, 0.9 |
| STO-WBP3450~4000 | MWIR | 3450 ± 50 – 4000 ± 50 | 3500-3900 | T>=85% | 1500-6000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3450~4050 | MWIR | 3450 ± 50 – 4050 ± 50 | 3600-3900 | T>=90% | 200-10000 nm; T < 1% | Germanium | 1.8 |
| STO-WBP3470~4950 | MWIR | 3470 ± 50 – 4950 ± 50 | 3570-4850 | T>=90% | 500-10070 nm; T < 1% | Germanium | 0.3, 0.9 |
| STO-WBP3480~4880 | MWIR | 3480 ± 50 – 4880 ± 50 | 3700-4800 | T>=80% | 400-10000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3490~3850 | MWIR | 3490 ± 50 – 3850 ± 50 | 3550-3750 | T>=80% | 400-6000 nm; T < 1% | Silicon | 0.5, 1 |
| STO-WBP3490~3950 | MWIR | 3490 ± 50 – 3950 ± 50 | 3650-3800 | T>=80% | 400-10000 nm; T < 1% | Silicon | 0.5, 1 |
| STO-WBP3490~4050 | MWIR | 3490 ± 50 – 4050 ± 50 | 3650-3950 | T>=80% | 400-10000 nm; T < 1% | Silicon | 1 |
| STO-WBP3500~4150 | MWIR | 3500 ± 50 – 4150 ± 50 | 3600-4050 | T>=90% | 1500-10000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP3500~4900 | MWIR | 3500 ± 50 – 4900 ± 50 | 3600-4800 | T>=70% | 400-10000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3500~4950 | MWIR | 3500 ± 50 – 4950 ± 50 | 3560-4900 | T>=90% | 540-10040 nm; T < 1% | Germanium | 0.3 |
| STO-WBP3500~5300 | MWIR | 3500 ± 50 – 5300 ± 50 | 3600-5100 | T>=85% | 1500-10000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP3500~5600 | MWIR | 3500 ± 50 – 5600 ± 50 | 3600-5500 | T>=85% | 1500-10000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP3525~4925 | MWIR | 3525 ± 100 – 4950 ± 100 | 3700-4800 | T>=90% | 1500-9000 nm; T < 1% | Germanium | 0.5 |
| STO-WBP3530~3950 | MWIR | 3530 ± 50 – 3950 ± 50 | 3610-3870 | T>=75% | 400-5580 nm; T < 1% | Silicon | 0.5, 1.2 |
| STO-WBP3500~3970 | MWIR | 3545 ± 20 – 4015 ± 20 | 3610-3955 | T>=80% | 450-5600 nm; T < 1% | Zinc selenide | 2 |
| STO-WBP3550~4100 | MWIR | 3550 ± 50 – 4100 ± 50 | 3650-4000 | T>=93% | 1500-6000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3550~4250 | MWIR | 3550 ± 50 – 4250 ± 50 | 3600-4200 | T>=90% | 500-6500 nm; T < 1% | Germanium | 0.3, 0.9 |
| STO-WBP3550~4750 | MWIR | 3550 ± 50 – 4750 ± 50 | 3650-4650 | T>=90% | 1500-7000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3550~4950 | MWIR | 3550 ± 50 – 4950 ± 50 | 3700-4800 | T>=90% | 1500-10000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3550~4990 | MWIR | 3550 ± 50 – 4990 ± 50 | 3600-4800 | T>=85% | 400-10000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3550~5000 | MWIR | 3550 ± 50 – 5000 ± -100 | 3700-4600 | T>=90% | 1500-10500 nm; T < 1% | Sapphire | 0.3, 0.5 |
| STO-WBP3600-4000 | MWIR | 3600 ± 50 – 4000 ± 50 | 3620-3890 | T>=75% | 450-5600 nm; T < 1% | Zinc selenide | 1.5, 2 |
| STO-WBP3600~4000 | MWIR | 3600 ± 50 – 4000 ± 50 | 3680-3900 | T>=75% | 400-5580 nm; T < 1% | Silicon | 1.2 |
| STO-WBP3600~4300 | MWIR | 3600 ± 50 – 4300 ± 50 | 3700-4200 | T>=85% | 1500-6000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3600~4850 | MWIR | 3600 ± 50 – 4850 ± 50 | 3700-4700 | T>=90% | 1500-7000 nm; T < 1% | Germanium | 0.3, 1 |
| STO-WBP3600~5000 | MWIR | 3600 ± 50 – 5000 ± 50 | 3700-4700 | T>=90% | 400-9000 nm; T < 1% | Germanium | 0.8 |
| STO-WBP3600~5100 | MWIR | 3600 ± 100 – 5100 ± 100 | 3800-5000 | T>=90% | 200-10500 nm; T < 1% | Sapphire | 0.5 |
| STO-WBP3600~5300 | MWIR | 3600 ± 50 – 5300 ± 50 | 3700-5200 | T>=90% | 930-10050 nm; T < 1% | Germanium | 0.5 |
| STO-WBP3600~5450 | MWIR | 3600 ± 50 – 5450 ± 50 | 3800-5250 | T>=80% | 400-6000 nm; T < 1% | Germanium | 0.9 |
| STO-WBP3600~5550 | MWIR | 3600 ± 50 – 5550 ± 50 | 3700-5400 | T>=90% | 1500-7000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP3605~5275 | MWIR | 3605 ± 25 – 5275 ± 25 | 3730-5150 | T>=90% | 930-10050 nm; T < 1% | Germanium | 0.5 |
| STO-WBP3650~4265 | MWIR | 3650 ± 50 – 4265 ± 50 | 3750-4150 | T>=90% | 500-7000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP3650~5050 | MWIR | 3650 ± 50 – 5050 ± 50 | 3800-4900 | T>=90% | 1500-7000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP3650~5100 | MWIR | 3650 ± 50 – 5100 ± 50 | 3740-5000 | T>=93% | 1500-7000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP3650~5150 | MWIR | 3650 ± 70 – 5150 ± 70 | 3800-5000 | T>=90% | 200-10500 nm; T < 1% | Sapphire | 0.5 |
| STO-WBP3650~5350 | MWIR | 3650 ± 50 – 5350 ± 50 | 3800-5200 | T>=90% | 400-11000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP3650~5550 | MWIR | 3650 ± 50 – 5550 ± 50 | 3750-5300 | T>=85% | 1500-7000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3650~5600 | MWIR | 3650 ± 50 – 5600 ± 50 | 3750-5400 | T>=90% | 1500-7000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP3650~5750 | MWIR | 3650 ± 50 – 5750 ± 50 | 3750-5450 | T>=90% | 1500-7000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP3700~4500 | MWIR | 3650 ± 50 – 4600 ± 50 | 3700-4500 | T>=90% | 1500-7000 nm; T < 1% | Silicon | 0.5, 1 |
| STO-WBP3660~4250 | MWIR | 3660 ± 50 – 4250 ± 50 | 3750-4150 | T>=90% | 500-7000 nm; T < 1% | Germanium | 0.9, 1 |
| STO-WBP3800~4850 | MWIR | 3675 ± 25 – 4975 ± 25 | 3800-4850 | T>=90% | 500-6500 nm; T < 1% | Germanium | 0.3 |
| STO-WBP3680~5160 | MWIR | 3700 ± 100 – 5200 ± 100 | 3800-4700 | T>=90% | 400-14000 nm; T < 1% | Sapphire | 0.5 |
| STO-WBP3700~4550 | MWIR | 3700 ± 50 – 4550 ± 50 | 3800-4450 | T>=90% | 1500-7000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3700~4700 | MWIR | 3700 ± 50 – 4700 ± 50 | 3800-4600 | T>=85% | 500-8000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP3700~4990 | MWIR | 3700 ± 50 – 4990 ± 40 | 3800-4750 | T>=85% | 1000-6500 nm; T < 1% | Germanium | 0.3, 0.38, 0.7 |
| STO-WBP3700~5020 | MWIR | 3700 ± 50 – 5020 ± 50 | 3800-4920 | T>=90% | 500-7000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP3700~5150 | MWIR | 3700 ± 50 – 5150 ± 50 | 3750-4900 | T>=92% | 1500-7000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP3700~5200 | MWIR | 3700 ± 60 – 5200 ± 60 | 3850-5050 | T>=90% | 200-10500 nm; T < 1% | Sapphire | 0.5 |
| STO-WBP3700~5600 | MWIR | 3700 ± 50 – 5600 ± 50 | 3850-5450 | T>=85% | 1500-10000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP3700~5750 | MWIR | 3700 ± 50 – 5750 ± 50 | 3850-5500 | T>=90% | 1500-7000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP3700~5800 | MWIR | 3700 ± 50 – 5800 ± 50 | 3850-5600 | T>=90% | 1500-7000 nm; T < 1% | Germanium | 1 |
| STO-WBP3710~5030 | MWIR | 3710 ± 30 – 5030 ± 30 | 3800-4900 | T>=90% | 1800-7000 nm; T < 1% | Silicon | 1 |
| STO-WBP3730~4850 | MWIR | 3730 ± 50 – 4850 ± 50 | 3900-4700 | T>=90% | 1500-7000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP3730~4900 | MWIR | 3730 ± 50 – 4900 ± 50 | 3850-4750 | T>=90% | 1000-6500 nm; T < 1% | Germanium | 0.3, 0.4 |
| STO-WBP3730~4960 | MWIR | 3730 ± 50 – 4960 ± 50 | 3850-4600 | T>=85% | 1000-6500 nm; T < 1% | Germanium | 0.9 |
| STO-WBP3740~4840 | MWIR | 3740 ± 50 – 4840 ± 50 | 3740-4840 | T>=90% | 540-8040 nm | Germanium | 0.3 |
| STO-WBP3740~4860 | MWIR | 3740 ± 40 – 4860 ± 40 | 3850-4700 | T>=85% | 1000-10000 nm; T < 1% | Germanium | 0.3, 0.38, 0.4 |
| STO-WBP3740~4950 | MWIR | 3740 ± 50 – 4950 ± 50 | 3900-4800 | T>=90% | 540-8040 nm | Germanium | 0.3 |
| STO-WBP3750~4500 | MWIR | 3750 ± 50 – 4500 ± 50 | 3850-4400 | T>=85% | 1500-7000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3750~4850 | MWIR | 3750 ± 50 – 4850 ± 50 | 3900-4700 | T>=90% | 1500-7000 nm; T < 1% | Germanium | 0.3, 0.9 |
| STO-WBP3750~4900 | MWIR | 3750 ± 50 – 4900 ± 50 | 3900-4700 | T>=90% | 1500-7000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP3750~5020 | MWIR | 3750 ± 50 – 5020 ± 50 | 3850-4920 | T>=90% | 500-7000 nm; T < 1% | Germanium | 0.3, 1 |
| STO-WBP3750~5050 | MWIR | 3750 ± 50 – 5050 ± 50 | 3900-4900 | T>=85% | 1000-6500 nm; T < 1% | Germanium | 0.8 |
| STO-WBP3750~5650 | MWIR | 3750 ± 50 – 5650 ± 50 | 4000-5300 | T>=90% | 1500-7000 nm; T < 1% | Germanium | 0.7 |
| STO-WBP3750~5700 | MWIR | 3750 ± 50 – 5700 ± 50 | 4000-5500 | T>=85% | 1500-7000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3750~5800 | MWIR | 3750 ± 50 – 5800 ± 50 | 3800-5600 | T>=80% | 1500-7000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP3800~4100 | MWIR | 3800 ± 50 – 4100 ± 50 | 3850-4050 | T>=90% | 500-8000 nm; T < 1% | Germanium | 0.6 |
| STO-WBP3800~4700 | MWIR | 3800 ± 50 – 4700 ± 50 | 3800-4900 | T>=90% | 1500-7000 nm; T < 1% | Germanium | 0.3, 0.9 |
| STO-WBP3800~5500 | MWIR | 3800 ± 100 – 5500 ± 100 | 3900-5400 | T>=80% | 400-14000 nm; T < 1% | Sapphire | 0.5 |
| STO-WBP3900~5150 | MWIR | 3900 ± 100 – 5150 ± 50 | 4400-4800 | T>=85% | 500-6500 nm; T < 1% | Sapphire | 0.5 |
| STO-WBP3900~5600 | MWIR | 3900 ± 100 – 5600 ± 100 | 4000-5500 | T>=80% | 400-14000 nm; T < 1% | Sapphire | 0.5 |
| STO-WBP3900~5650 | MWIR | 3900 ± 100 – 5650 ± 100 | 4100-5400 | T>=80% | 400-14000 nm; T < 1% | Sapphire | 0.5 |
| STO-WBP4000~4650 | MWIR | 4000 ± 50 – 4650 ± 50 | 4120-4480 | T>=85% | 1500-11000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP4000~5000 | MWIR | 4000 ± 200 – 5000 ± 200 | 4200-4900 | T>=85% | 400-20000 nm; T < 1% | Sapphire | 0.5, 1 |
| STO-WBP4000~5200 | MWIR | 4000 ± 50 – 5200 ± 50 | 4100-5000 | T>=90% | 200-10000 nm; T < 1% | Germanium | 0.9, 1.8 |
| STO-WBP4100~4650 | MWIR | 4100 ± 50 – 4650 ± 50 | 4200-4550 | T>=80% | 1500-7000 nm; T < 1% | Germanium | 0.9 |
| STO-WBP4120~4360 | MWIR | 4120 ± 60 – 4360 ± 60 | 4220-4320 | T>=85% | 300-6500 nm; T < 1% | Silicon | 1 |
| STO-WBP4140~4370 | MWIR | 4140 ± 30 – 4370 ± 30 | 4200-4300 | T>=75% | 1500-7000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP4140~4440 | MWIR | 4140 ± 30 – 4440 ± 30 | 4200-4400 | T>=80% | 1500-7000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP4150~4650 | MWIR | 4150 ± 50 – 4650 ± 50 | 4250-4550 | T>=90% | 1500-6000 nm; T < 1% | Germanium | 0.3, 0.9 |
| STO-WBP4200~4450 | MWIR | 4200 ± 20 – 4450 ± 20 | 4250-4400 | T>=85% | 1500-7000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP4200~4750 | MWIR | 4200 ± 50 – 4750 ± 50 | 4250-4650 | T>=80% | 1500-7000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP4200~5000 | MWIR | 4200 ± 50 – 5000 ± 50 | 4350-4800 | T>=85% | 500-10000 nm; T < 1% | Silicon | 4 |
| STO-WBP4212~4457 | MWIR | 4212 ± 40 – 4457 ± 40 | 4260-4400 | T>=80% | 300-6500 nm; T < 1% | Silicon | 0.95 |
| STO-WBP4230~4520 | MWIR | 4230 ± 20 – 4520 ± 20 | 4350-4450 | T>=80% | 1500-5000 nm; T < 1% | Germanium | 1 |
| STO-WBP4250~4800 | MWIR | 4250 ± 50 – 4800 ± 50 | 4350-4700 | T>=80% | 1500-7000 nm; T < 1% | Germanium | 0.3, 0.9 |
| STO-WBP4250~5300 | MWIR | 4250 ± 50 – 5300 ± 50 | 4400-5000 | T>=85% | 1500-10000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP4290~4580 | MWIR | 4290 ± 20 – 4580 ± 20 | 4400-4500 | T>=80% | 1500-5000 nm; T < 1% | Germanium | 0.9, 1 |
| STO-WBP4300~4500 | MWIR | 4300 ± 30 – 4500 ± 30 | 4350-4450 | T>=90% | 1500-7000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP4400~4700 | MWIR | 4400 ± 50 – 4700 ± 50 | 4570-4600 | T>=80% | 1500-11000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP4420~4720 | MWIR | 4420 ± 50 – 4720 ± 50 | 4470-4670 | T>=80% | 520-8020 nm; T < 1% | Germanium | 0.3 |
| STO-WBP4450~4750 | MWIR | 4450 ± 70 – 4750 ± 70 | 4570-4620 | T>=70% | 1500-11000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP4450~4950 | MWIR | 4450 ± 50 – 4950 ± 50 | 4550-4900 | T>=90% | 1500-6000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP4450~5150 | MWIR | 4450 ± 50 – 5150 ± 50 | 4550-5050 | T>=85% | 1000-9400 nm; T < 1% | Germanium | 0.8, 1 |
| STO-WBP4500~4800 | MWIR | 4500 ± 50 – 4800 ± 50 | 4640-4740 | T>=85% | 400-10000 nm; T < 1% | Germanium | 0.3, 0.7 |
| STO-WBP4500~4900 | MWIR | 4500 ± 50 – 4900 ± 50 | 4600-4800 | T>=85% | 1500-11000 nm; T < 1% | Silicon | 0.8 |
| STO-WBP4520~4720 | MWIR | 4520 ± 50 – 4720 ± 50 | 4570-4670 | T>=80% | 520-8020 nm; T < 1% | Germanium | 0.3, 0.8 |
| STO-WBP4520~4820 | MWIR | 4520 ± 50 – 4820 ± 50 | 4570-4770 | T>=80% | 520-8020 nm; T < 1% | Germanium | 0.3 |
| STO-WBP4550~5200 | MWIR | 4550 ± 50 – 5300 ± 50 | 4600-5150 | T>=85% | 1000-9400 nm; T < 1% | Germanium | 0.8, 1 |
| STO-WBP4600~4900 | MWIR | 4600 ± 50 – 4900 ± 50 | 4700-4800 | T>=80% | 400-10000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP4650~4950 | MWIR | 4650 ± 50 – 4950 ± 50 | 4700-4800 | T>=80% | 400-10000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP4650~4980 | MWIR | 4650 ± 50 – 4980 ± 50 | 4700-4800 | T>=80% | 400-10000 nm; T < 1% | Germanium | 1 |
| STO-WBP4650~5300 | MWIR | 4650 ± 50 – 5300 ± 50 | 4800-5200 | T>=80% | 1500-10000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP4750~5150 | MWIR | 4750 ± 50 – 5150 ± 50 | 4800-5000 | T>=80% | 1000-8000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP4800~5000 | MWIR | 4800 ± 50 – 5000 ± 50 | 4850-4950 | T>=80% | 400-5500 nm; T < 1% | Silicon | 1.2 |
| STO-WBP4800~5100 | MWIR | 4800 ± 50 – 5100 ± 50 | 4850-5050 | T>=80% | 400-5500 nm; T < 1% | Silicon | 1 |
| STO-WBP4800~5200 | MWIR/LWIR transition | 4800 ± 50 – 5200 ± 50 | 4860-5140 | T>=90% | 1000-8000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP4900~5100 | MWIR/LWIR transition | 4900 ± 50 – 5100 ± 50 | 4950-5050 | T>=80% | 400-5500 nm; T < 1% | Silicon | 1 |
| STO-WBP4920~5800 | MWIR/LWIR transition | 4920 ± 50 – 5800 ± 50 | 5100-5600 | T>=85% | 400-10000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP4950~9250 | MWIR/LWIR transition | 4950 ± 50 – 9250 ± 50 | 5100-9100 | T>=90% | 1500-15000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP5000~5800 | MWIR/LWIR transition | 5000 ± 50 – 5800 ± 50 | 5100-5600 | T>=80% | 400-10000 nm; T < 1% | Germanium | 1 |
| STO-WBP5010~5880 | MWIR/LWIR transition | 5010 ± 50 – 5880 ± 50 | 5110-5780 | T>=80% | 400-10000 nm; T < 1% | Germanium | 1 |
| STO-WBP5030~9280 | MWIR/LWIR transition | 5030 ± 50 – 9280 ± 50 | 5180-9130 | T>=90% | 1500-15000 nm; T < 1% | Germanium | 0.3, 0.8 |
| STO-WBP5050~9160 | MWIR/LWIR transition | 5050 ± 50 – 9160 ± 50 | 5300-8750 | T>=85% | 620-10120 nm; T < 1% | Germanium | 2 |
| STO-WBP5090~9450 | MWIR/LWIR transition | 5090 ± 90 – 9450 ± 90 | 5240-9300 | T>=90% | 1500-15000 nm; T < 1% | Germanium | 0.3, 0.8 |
| STO-WBP5100~5850 | MWIR/LWIR transition | 5100 ± 50 – 5850 ± 50 | 5300-5700 | T>=75% | 400-10000 nm; T < 1% | Germanium | 0.9, 1 |
| STO-WBP5100~9350 | MWIR/LWIR transition | 5100 ± 50 – 9350 ± 50 | 6100-9200 | T>=85% | 620-10120 nm; T < 1% | Germanium | 2 |
| STO-WBP5150~6000 | MWIR/LWIR transition | 5150 ± 50 – 6000 ± 50 | 5050-5900 | T>=80% | 500-10120 nm; T < 1% | Germanium | 2 |
| STO-WBP5150~9450 | MWIR/LWIR transition | 5150 ± 50 – 9450 ± 50 | 5400-9100 | T>=85% | 620-10120 nm; T < 1% | Germanium | 2 |
| STO-WBP5240~9440 | MWIR/LWIR transition | 5240 ± 70 – 9440 ± 70 | 6000-9000 | T>=80% | 580-10080 nm; T < 1% | Germanium | 2 |
| STO-WBP5400~7400 | MWIR/LWIR transition | 5400 ± 50 – 7400 ± 50 | 5500-7300 | T>=90% | 1500-10000 nm; T < 1% | Germanium | 1.5 |
| STO-WBP5450~7600 | MWIR/LWIR transition | 5450 ± 50 – 7600 ± 50 | 5600-7400 | T>=90% | 1500-10000 nm; T < 1% | Germanium | 1.5 |
| STO-WBP5510~6700 | MWIR/LWIR transition | 5510 ± 60 – 6700 ± 60 | 5700-6500 | T>=75% | 1500-11000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP5550~7550 | MWIR/LWIR transition | 5550 ± 50 – 7550 ± 50 | 5750-7250 | T>=90% | 1500-10600 nm; T < 1% | Germanium | 0.5 |
| STO-WBP5550~7600 | MWIR/LWIR transition | 5550 ± 50 – 7600 ± 50 | 5750-7300 | T>=90% | 1500-10600 nm; T < 1% | Germanium | 0.5 |
| STO-WBP5550~7650 | MWIR/LWIR transition | 5550 ± 50 – 7650 ± 50 | 5700-7450 | T>=90% | 1500-10000 nm; T < 1% | Germanium | 1.5 |
| STO-WBP5550~7700 | MWIR/LWIR transition | 5550 ± 50 – 7700 ± 50 | 5700-7500 | T>=85% | 1500-10000 nm; T < 1% | Germanium | 1.5 |
| STO-WBP5600~6800 | MWIR/LWIR transition | 5600 ± 30 – 6800 ± 30 | 5700-6680 | T>=75% | 1500-11000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP6000~12100 | LWIR | 6000 ± 200 – 12100 ± 200 | 6200-11800 | T>=90% | 1000-15000 nm; T < 1% | Germanium | 0.5 |
| STO-WBP6200~10200 | LWIR | 6200 ± 100 – 10200 ± 100 | 7000-9400 | T>=90% | 1500-15000 nm; T < 1% | Germanium | 0.3, 0.8 |
| STO-WBP6220~7530 | MWIR/LWIR transition | 6220 ± 50 – 7530 ± 50 | 6450-7450 | T>=90% | 2000-15000 nm; T < 3% | Germanium | 3 |
| STO-WBP6300~7600 | MWIR/LWIR transition | 6300 ± 50 – 7600 ± 50 | 6450-7450 | T>=90% | 2000-15000 nm; T < 3% | Germanium | 3 |
| STO-WBP6300~9900 | LWIR | 6300 ± 100 – 9900 ± 100 | 7000-9400 | T>=90% | 1500-15000 nm; T < 1% | Germanium | 0.3, 0.8 |
| STO-WBP6400~10100 | LWIR | 6400 ± 100 – 10100 ± 100 | 7000-9400 | T>=90% | 1500-15000 nm; T < 1% | Germanium | 0.8 |
| STO-WBP6420~10100 | LWIR | 6420 ± 50 – 10100 ± 50 | 7000-9400 | T>=90% | 1500-15000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP6450~10750 | LWIR | 6450 ± 100 – 10750 ± 100 | 6600-10600 | T>=90% | 1500-14000 nm; T < 1% | Germanium | 1 |
| STO-WBP6450~7750 | MWIR/LWIR transition | 6450 ± 50 – 7750 ± 50 | 6650-7550 | T>=90% | 2000-15000 nm; T < 3% | Germanium | 3 |
| STO-WBP6550~8250 | MWIR/LWIR transition | 6550 ± 100 – 8250 ± 100 | 6700-8100 | T>=85% | 400-11000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP6600~8300 | MWIR/LWIR transition | 6600 ± 100 – 8300 ± 100 | 6750-8150 | T>=85% | 400-11000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP6650~8750 | MWIR/LWIR transition | 6650 ± 50 – 8750 ± 50 | 6800-8500 | T>=75% | 1500-11000 nm; T < 3% | Germanium | 0.3 |
| STO-WBP6650~9760 | LWIR | 6650 ± 50 – 9760 ± 50 | 7000-9400 | T>=90% | 1500-15000 nm; T < 1% | Germanium | 0.3, 0.8 |
| STO-WBP6800~8100 | MWIR/LWIR transition | 6800 ± 80 – 8100 ± 80 | 7100-7800 | T>=90% | 200-12000 nm; T < 1% | Silicon | 1 |
| STO-WBP6800~8300 | MWIR/LWIR transition | 6800 ± 100 – 8300 ± 100 | 6950-8150 | T>=85% | 400-11000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP7100~8400 | MWIR/LWIR transition | 7100 ± 80 – 8400 ± 80 | 7400-8100 | T>=90% | 200-12000 nm; T < 1% | Silicon | 1 |
| STO-WBP7200~8500 | MWIR/LWIR transition | 7200 ± 80 – 8500 ± 80 | 7500-8200 | T>=90% | 200-12000 nm; T < 1% | Silicon | 0.5, 1 |
| STO-WBP7200~9400 | LWIR | 7200 ± 50 – 9400 ± 50 | 7300-9100 | T>=90% | 6400-13000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7250~7850 | MWIR/LWIR transition | 7250 ± 100 – 7850 ± 100 | 7350-7750 | T>=80% | 3300-20000 nm; T < 1% | Germanium | 1, 2 |
| STO-WBP7350~8080 | MWIR/LWIR transition | 7350 ± 50 – 8080 ± 50 | 7510-7980 | T>=90% | 400-12000 nm; T < 3% | Germanium | 0.3 |
| STO-WBP7400~8400 | MWIR/LWIR transition | 7400 ± 50 – 8400 ± 50 | 7600-8200 | T>=80% | 200-16000 nm; T < 1% | Silicon | 1 |
| STO-WBP7400~8430 | MWIR/LWIR transition | 7400 ± 70 – 8430 ± 70 | 7600-8100 | T>=85% | 200-16000 nm; T < 1% | Silicon | 1 |
| STO-WBP7400~8500 | MWIR/LWIR transition | 7400 ± 50 – 8500 ± 50 | 7600-8200 | T>=80% | 200-16000 nm; T < 1% | Silicon | 1 |
| STO-WBP7400~9500 | LWIR | 7400 ± 50 – 9500 ± 50 | 7500-9400 | T>=90% | 1500-13000 nm; T < 1% | Germanium | 0.6 |
| STO-WBP7450~10200 | LWIR | 7450 ± 50 – 10200 ± 50 | 7600-10000 | T>=85% | 1000-12000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7450~13600 | LWIR | 7450 ± 50 – 13600 ± 100 | 7700-13300 | T>=75% | 2000-19000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP7450~8500 | MWIR/LWIR transition | 7450 ± 50 – 8500 ± 50 | 7600-8100 | T>=75% | 200-16000 nm; T < 1% | Silicon | 1 |
| STO-WBP7450~9650 | LWIR | 7450 ± 50 – 9650 ± 50 | 7700-9400 | T>=85% | 1500-12000 nm; T < 1% | Germanium | 0.3, 0.6 |
| STO-WBP7400~9900 | LWIR | 7460 ± 50 – 9960 ± 50 | 7660-9760 | T>=90% | 460-16060 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7460~9630 | LWIR | 7460 ± 50 – 9630 ± 50 | 7550-9600 | T>=90% | 1500-13000 nm; T < 1% | Germanium | 1 |
| STO-WBP7480~9380 | LWIR | 7480 ± 70 – 9380 ± 70 | 7700-9100 | T>=80% | 500-10080 nm; T < 1% | Germanium | 2 |
| STO-WBP7500~7900 | MWIR/LWIR transition | 7500 ± 70 – 7900 ± 70 | 7600-7800 | T>=85% | 400-12075 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7500~8400 | MWIR/LWIR transition | 7500 ± 50 – 8400 ± 50 | 7700-8100 | T>=85% | 200-16000 nm; T < 1% | Silicon | 1 |
| STO-WBP7500~8500 | LWIR | 7500 ± 50 – 8500 ± 50 | 7700-8200 | T>=85% | 200-16000 nm; T < 1% | Silicon | 0.5, 1 |
| STO-WBP7500~8550 | LWIR | 7500 ± 50 – 8550 ± 50 | 7700-8200 | T>=80% | 200-16000 nm; T < 1% | Silicon | 1 |
| STO-WBP7500~8600 | LWIR | 7500 ± 50 – 8600 ± 50 | 7700-8300 | T>=80% | 200-16000 nm; T < 1% | Silicon | 1 |
| STO-WBP7500~9300 | LWIR | 7500 ± 50 – 9300 ± 50 | 7700-9000 | T>=85% | 1000-13900 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7500~9400 | LWIR | 7500 ± 50 – 9400 ± 50 | 8000-9000 | T>=85% | 1500-12000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7550~13700 | LWIR | 7550 ± 50 – 13700 ± 100 | 7750-13400 | T>=85% | 2000-19000 nm; T < 1% | Germanium | 0.7, 1 |
| STO-WBP7550~13950 | LWIR | 7550 ± 100 – 13950 ± 100 | 7750-13400 | T>=80% | 2000-19000 nm; T < 1% | Germanium | 1 |
| STO-WBP7550~8600 | LWIR | 7550 ± 70 – 8600 ± 70 | 7800-8300 | T>=85% | 200-16000 nm; T < 1% | Silicon | 1 |
| STO-WBP7550~9800 | LWIR | 7550 ± 50 – 9800 ± 50 | 7700-9550 | T>=90% | 1500-12000 nm; T < 1% | Germanium | 0.3, 0.7 |
| STO-WBP7575~7975 | MWIR/LWIR transition | 7575 ± 50 – 7975 ± 50 | 7675-7875 | T>=85% | 400-12075 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7600~10100 | LWIR | 7600 ± 70 – 10100 ± 100 | 7770-9900 | T>=90% | 400-16000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7600~10160 | LWIR | 7600 ± 100 – 10160 ± 100 | 7800-9800 | T>=90% | 400-16000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7600~8100 | MWIR/LWIR transition | 7600 ± 100 – 8100 ± 100 | 7700-8000 | T>=85% | 1500-13000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7600~8600 | LWIR | 7600 ± 50 – 8600 ± 50 | 7800-8300 | T>=80% | 200-16000 nm; T < 1% | Silicon | 1 |
| STO-WBP7600~9300 | LWIR | 7600 ± 50 – 9300 ± 50 | 7700-9000 | T>=85% | 1000-13900 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7600~9500 | LWIR | 7600 ± 50 – 9500 ± 50 | 8000-9200 | T>=90% | 1500-12000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7600~9600 | LWIR | 7600 ± 50 – 9600 ± 50 | 7800-9300 | T>=85% | 1500-12000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7600~9700 | LWIR | 7600 ± 50 – 9700 ± 50 | 8000-9500 | T>=90% | 1500-12000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7600~9730 | LWIR | 7600 ± 50 – 9730 ± 50 | 7800-9500 | T>=85% | 1500-12000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7600~9950 | LWIR | 7600 ± 50 – 9950 ± 50 | 7900-9600 | T>=85% | 6400-13000 nm; T < 1% | Germanium | 0.6 |
| STO-WBP7630~8070 | MWIR/LWIR transition | 7630 ± 70 – 8070 ± 70 | 7730-7970 | T>=85% | 400-12075 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7650~10400 | LWIR | 7650 ± 50 – 10400 ± 50 | 7800-10250 | T>=85% | 1000-12000 nm; T < 1% | Germanium | 0.38 |
| STO-WBP7650~13900 | LWIR | 7650 ± 50 – 13900 ± 100 | 7800-13400 | T>=85% | 2000-19000 nm; T < 1% | Germanium | 0.7, 1 |
| STO-WBP7650~14100 | LWIR | 7650 ± 50 – 14100 ± 100 | 7750-13400 | T>=85% | 2000-19000 nm; T < 1% | Germanium | 0.4, 0.7, 1 |
| STO-WBP7650~8690 | LWIR | 7650 ± 70 – 8690 ± 70 | 7900-8400 | T>=80% | 200-16000 nm; T < 1% | Silicon | 1 |
| STO-WBP7650~9870 | LWIR | 7650 ± 50 – 9870 ± 50 | 8000-9600 | T>=90% | 1500-12000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7700~13500 | LWIR | 7700 ± 200 – 13500 ± 500 | 7900-13000 | T>=85% | 2000-19000 nm; T < 1% | Germanium | 1 |
| STO-WBP7700~14250 | LWIR | 7700 ± 100 – 14250 ± 100 | 7750-13400 | T>=85% | 2000-19000 nm | Germanium | 0.4, 1 |
| STO-WBP7700~8200 | MWIR/LWIR transition | 7700 ± 100 – 8200 ± 100 | 7810-8110 | T>=80% | 1500-13000 nm; T < 1% | Germanium | 0.3, 0.7 |
| STO-WBP7700~9400 | LWIR | 7700 ± 50 – 9400 ± 50 | 7850-9200 | T>=90% | 1500-12000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7700~9600 | LWIR | 7700 ± 100 – 9600 ± 100 | 7950-9450 | T>=90% | 400-14000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7700~9650 | LWIR | 7700 ± 50 – 9650 ± 50 | 8000-9400 | T>=85% | 1500-12000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7700~9850 | LWIR | 7700 ± 100 – 9850 ± 100 | 7870-9570 | T>=85% | 1500-14070 nm; T < 1% | Germanium | 0 |
| STO-WBP7700~9900 | LWIR | 7700 ± 50 – 9900 ± 50 | 8000-9600 | T>=90% | 1500-12000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7700~9980 | LWIR | 7700 ± 50 – 9980 ± 50 | 8000-9700 | T>=90% | 1500-12000 nm; T < 1% | Germanium | 0.9 |
| STO-WBP7730~10250 | LWIR | 7730 ± 70 – 10250 ± 100 | 7900-10050 | T>=90% | 400-16000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7730~9950 | LWIR | 7730 ± 50 – 9950 ± 50 | 8100-9600 | T>=90% | 1500-12000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7750~10000 | LWIR | 7750 ± 50 – 10000 ± 50 | 8100-9600 | T>=90% | 1500-12000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7750~10050 | LWIR | 7750 ± 50 – 10050 ± 50 | 7700-10000 | T>=90% | 1500-12000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7750~10100 | LWIR | 7750 ± 50 – 10100 ± 100 | 7700-10000 | T>=85% | 1500-13000 nm; T < 1% | Germanium | 0.3, 0.6 |
| STO-WBP7750~10250 | LWIR | 7750 ± 50 – 10250 ± 50 | 7800-9800 | T>=90% | 400-16000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7750~10300 | LWIR | 7750 ± 50 – 10300 ± 50 | 7900-10150 | T>=90% | 400-16000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7750~10500 | LWIR | 7750 ± 100 – 10500 ± 100 | 7950-10300 | T>=90% | 500-14000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7750~9700 | LWIR | 7750 ± 50 – 9700 ± 50 | 8100-9500 | T>=90% | 1500-12000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7750~9980 | LWIR | 7750 ± 50 – 9980 ± 50 | 8000-9700 | T>=80% | 1500-12000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP7770~10580 | LWIR | 7770 ± 50 – 10580 ± 50 | 7950-10400 | T>=90% | 500-14000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7780~9280 | LWIR | 7780 ± 100 – 9280 ± 100 | 8100-9000 | T>=90% | 3030-14140 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7780~9480 | LWIR | 7780 ± 100 – 9480 ± 100 | 8100-9000 | T>=90% | 3030-14140 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7800~10050 | LWIR | 7800 ± 50 – 10050 ± 50 | 8100-9700 | T>=90% | 1500-12000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7800~10100 | LWIR | 7800 ± 50 – 10100 ± 50 | 7900-10000 | T>=90% | 1500-12000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7800~10350 | LWIR | 7800 ± 70 – 10350 ± 100 | 7970-10150 | T>=90% | 400-16000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7800~10600 | LWIR | 7800 ± 100 – 10600 ± 100 | 8000-10400 | T>=85% | 1000-12000 nm; T < 1% | Germanium | 0.9 |
| STO-WBP7800~12100 | LWIR | 7800 ± 100 – 12100 ± 100 | 8100-11900 | T>=85% | 1000-15000 nm; T < 1% | Germanium | 0.5 |
| STO-WBP7800~12200 | LWIR | 7800 ± 75 – 12200 ± 75 | 8100-11950 | T>=85% | 1000-15000 nm; T < 1% | Germanium | 0.5, 0.9 |
| STO-WBP7800~14200 | LWIR | 7800 ± 100 – 14200 ± 100 | 8300-13500 | T>=85% | 1500-19000 nm; T < 1% | Germanium | 0.7 |
| STO-WBP7800~9650 | LWIR | 7800 ± 50 – 9650 ± 50 | 8200-9300 | T>=90% | 1500-12000 nm; T < 1% | Germanium | 0.3, 0.7 |
| STO-WBP7800~9700 | LWIR | 7800 ± 50 – 9700 ± 50 | 8100-9500 | T>=90% | 1500-12000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7850-13650 | LWIR | 7850 ± 50 – 13650 ± 50 | 8100-13300 | T>=70% | 1500-20000 nm; T < 1.5% | Silicon | 1 |
| STO-WBP7850~10450 | LWIR | 7850 ± 50 – 10450 ± 50 | 8000-10100 | T>=90% | 400-16000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7850~10600 | LWIR | 7850 ± 50 – 10600 ± 50 | 8000-10350 | T>=85% | 1000-12000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7850~10650 | LWIR | 7850 ± 100 – 10650 ± 100 | 8050-10450 | T>=90% | 500-14000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7850~13750 | LWIR | 7850 ± 50 – 13750 ± 50 | 8100-13300 | T>=70% | 1500-20000 nm; T < 1.5% | Silicon | 0.5 |
| STO-WBP7850~13900 | LWIR | 7850 ± 100 – 13900 ± 400 | 8200-13400 | T>=80% | 2000-19000 nm; T < 1% | Germanium | 1 |
| STO-WBP7850~9650 | LWIR | 7850 ± 50 – 9650 ± 50 | 7900-9400 | T>=90% | 400-14000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7850~9700 | LWIR | 7850 ± 50 – 9700 ± 50 | 8300-9600 | T>=90% | 1500-12000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7850~9750 | LWIR | 7850 ± 50 – 9750 ± 50 | 7950-9450 | T>=90% | 400-14000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7850~9850 | LWIR | 7850 ± 50 – 9850 ± 50 | 7900-9400 | T>=90% | 400-14000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7800~10200 | LWIR | 7880 ± 100 – 10300 ± 100 | 8080-10100 | T>=90% | 406-14140 nm; T < 1% | Germanium | 0.5 |
| STO-WBP7880~10400 | LWIR | 7880 ± 100 – 10400 ± 100 | 8100-10100 | T>=90% | 406-14140 nm; T < 1% | Germanium | 0.5 |
| STO-WBP7900~12000 | LWIR | 7900 ± 100 – 12000 ± 100 | 8100-11800 | T>=90% | 400-20000 nm; T < 1% | Germanium | 1 |
| STO-WBP7900~12200 | LWIR | 7900 ± 100 – 12200 ± 100 | 8150-11900 | T>=85% | 1000-15000 nm; T < 1% | Germanium | 0.5 |
| STO-WBP7900~9800 | LWIR | 7900 ± 50 – 9800 ± 50 | 8300-9300 | T>=90% | 1500-12000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7920~10350 | LWIR | 7920 ± 70 – 10350 ± 100 | 8090-10150 | T>=90% | 400-16000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7920~10500 | LWIR | 7920 ± 70 – 10500 ± 100 | 8090-10300 | T>=90% | 400-16000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7950~10050 | LWIR | 7950 ± 50 – 10050 ± 50 | 8300-9700 | T>=92% | 1500-12000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7950~10400 | LWIR | 7950 ± 50 – 10400 ± 50 | 8500-10100 | T>=90% | 1500-12000 nm; T < 1% | Germanium | 0.9 |
| STO-WBP7950~13850 | LWIR | 7950 ± 50 – 13850 ± 50 | 8300-13300 | T>=75% | 1500-20000 nm; T < 1.5% | Silicon | 0.4 |
| STO-WBP7950~9850 | LWIR | 7950 ± 50 – 9850 ± 50 | 8200-9600 | T>=90% | 1500-12000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP7980~9680 | LWIR | 7980 ± 100 – 9680 ± 100 | 8030-9530 | T>=90% | 3030-14140 nm; T < 1% | Germanium | 0.3 |
| STO-WBP8000~10100 | LWIR | 8000 ± 100 – 10100 ± 100 | 8200-9900 | T>=90% | 1500-15000 nm; T < 1% | Germanium | 0.5 |
| STO-WBP8000~10700 | LWIR | 8000 ± 200 – 10700 ± 200 | 8600-10000 | T>=90% | 1590-16090 nm; T < 1% | Germanium | 0.8 |
| STO-WBP8000~11300 | LWIR | 8000 ± 50 – 11300 ± 50 | 8300-11200 | T>=90% | 400-12200 nm; T < 1% | Germanium | 0.5 |
| STO-WBP8000~11400 | LWIR | 8000 ± 50 – 11400 ± 50 | 8300-11000 | T>=90% | 400-12200 nm; T < 1% | Germanium | 0.5 |
| STO-WBP8000~12000 | LWIR | 8000 ± 100 – 12000 ± 100 | 8200-11800 | T>=90% | 400-20000 nm; T < 1% | Germanium | 1 |
| STO-WBP8000~12200 | LWIR | 8000 ± 100 – 12200 ± 100 | 8300-11800 | T>=90% | 1000-15000 nm; T < 1% | Germanium | 0.5, 0.9 |
| STO-WBP8000~12400 | LWIR | 8000 ± 100 – 12400 ± 100 | 8300-12000 | T>=90% | 1000-15000 nm; T < 1% | Germanium | 0.5 |
| STO-WBP8000~13900 | LWIR | 8000 ± 50 – 13900 ± 50 | 8300-13600 | T>=75% | 1500-20000 nm; T < 1.5% | Silicon | 1 |
| STO-WBP8050~13850 | LWIR | 8050 ± 50 – 13850 ± 50 | 8500-13300 | T>=70% | 1500-20000 nm; T < 1.5% | Silicon | 1 |
| STO-WBP8080~9880 | LWIR | 8080 ± 100 – 9880 ± 100 | 8500-9500 | T>=90% | 3030-14140 nm; T < 1% | Germanium | 0.3 |
| STO-WBP8100~11700 | LWIR | 8100 ± 100 – 11700 ± 100 | 8400-11400 | T>=90% | 400-12200 nm; T < 1% | Germanium | 0.5 |
| STO-WBP8100~12800 | LWIR | 8100 ± 100 – 12800 ± 100 | 8300-12600 | T>=85% | 1000-15000 nm; T < 1% | Germanium | 0.5 |
| STO-WBP8100~9000 | LWIR | 8100 ± 100 – 9000 ± 100 | 8250-8850 | T>=85% | 490-10090 nm; T < 1% | Germanium | 0.9, 1 |
| STO-WBP8200-10100 | LWIR | 8200 ± 400 – 10100 ± 420 | 8800-9500 | T>=88% | 2000-12000 nm; T < 1% | Germanium | 0.5, 0.6 |
| STO-WBP8200-12000 | LWIR | 8200 ± 100 – 12000 ± 100 | 8400-11800 | T>=90% | 400-20000 nm; T < 1% | Germanium | 1 |
| STO-WBP8200~10900 | LWIR | 8200 ± 200 – 10900 ± 200 | 8600-10000 | T>=90% | 1590-16090 nm; T < 1% | Germanium | 0.8 |
| STO-WBP8230~12400 | LWIR | 8230 ± 150 – 12400 ± 200 | 8800-11000 | T>=75% | 7000-15000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP8200~9000 | LWIR | 8240 ± 50 – 9140 ± 50 | 8340-9040 | T>=90% | 490-10090 nm; T < 1% | Germanium | 1 |
| STO-WBP8300-8900 | LWIR | 8300 ± 100 – 8900 ± 100 | 8400-8700 | T>=85% | 1570-14070 nm; T < 1% | Germanium | 0 |
| STO-WBP8300~13000 | LWIR | 8300 ± 160 – 13000 ± 160 | 8800-12500 | T>=75% | 7000-15000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP8300~9200 | LWIR | 8300 ± 100 – 9200 ± 100 | 8430-9090 | T>=85% | 490-10090 nm; T < 1% | Germanium | 1 |
| STO-WBP8300~9300 | LWIR | 8300 ± 100 – 9300 ± 100 | 8500-9100 | T>=85% | 490-10090 nm; T < 1% | Germanium | 1 |
| STO-WBP8400~13000 | LWIR | 8400 ± 150 – 13000 ± 150 | 8900-12500 | T>=75% | 7000-15000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP8400~14700 | LWIR | 8400 ± 200 – 14700 ± 300 | 9000-13000 | T>=75% | 400-20000 nm; T < 1% | Silicon | 0.5 |
| STO-WBP8500-12250 | LWIR | 8500 ± 100 – 12250 ± 100 | 8700-12100 | T>=85% | 1500-15500 nm; T < 1% | Germanium | 0.3 |
| STO-WBP8500-9050 | LWIR | 8500 ± 100 – 9050 ± 100 | 8650-8900 | T>=85% | 1570-14070 nm; T < 1% | Germanium | 0 |
| STO-WBP8550-12350 | LWIR | 8550 ± 50 – 12350 ± 50 | 8700-12200 | T>=85% | 1500-15500 nm; T < 1% | Germanium | 0.3, 0.5 |
| STO-WBP8600-12500 | LWIR | 8600 ± 150 – 12500 ± 150 | 8980-12000 | T>=85% | 1500-15500 nm; T < 1% | Germanium | 0.3, 0.8 |
| STO-WBP8700-9400 | LWIR | 8700 ± 100 – 9400 ± 100 | 8900-9300 | T>=85% | 1500-13000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP8770-9550 | LWIR | 8770 ± 50 – 9550 ± 50 | 9000-9400 | T>=85% | 1500-13000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP8800-9700 | LWIR | 8850 ± 50 – 9650 ± 50 | 9000-9500 | T>=85% | 1500-13000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP8900-9500 | LWIR | 8900 ± 100 – 9500 ± 100 | 9000-9400 | T>=85% | 1500-13000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP8900-9600 | LWIR | 8900 ± 100 – 9600 ± 100 | 9000-9500 | T>=85% | 1500-13000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP8900-9700 | LWIR | 8900 ± 100 – 9700 ± 100 | 9100-9500 | T>=85% | 1500-13000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP8900-9800 | LWIR | 8900 ± 100 – 9800 ± 100 | 9100-9500 | T>=85% | 1500-13000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP9000-9850 | LWIR | 9000 ± 100 – 9850 ± 100 | 9100-9500 | T>=85% | 1500-13000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP9600-14800 | LWIR | 9600 ± 100 – 14800 ± 100 | 9900-14400 | T>=85% | 400-20000 nm; T < 1% | Zinc selenide | 0.3 |
| STO-WBP9800-15100 | LWIR | 9800 ± 100 – 15100 ± 100 | 11000-14700 | T>=85% | 400-20000 nm; T < 1% | Zinc selenide | 0.3 |
| STO-WBP10100-11100 | LWIR | 10100 ± 100 – 11100 ± 100 | 10350-10850 | T>=90% | 7600-14000 nm; T < 1% | Germanium | 0.3 |
| STO-WBP10160-11180 | LWIR | 10160 ± 50 – 11180 ± 50 | 10310-11030 | T>=90% | 2000-15000 nm; T < 1% | Germanium | 3 |
| STO-WBP10200-11600 | LWIR | 10200 ± 100 – 11600 ± 100 | 10600-11300 | T>=85% | 7000-14000 nm; T < 1% | Germanium | 1 |
| STO-WBP10240-10840 | LWIR | 10240 ± 50 – 10840 ± 50 | 10340-10740 | T>=80% | 590-14090 nm; T < 1% | Germanium | 0.3 |
| STO-WBP10240-11260 | LWIR | 10240 ± 50 – 11260 ± 50 | 10400-11100 | T>=90% | 2000-15000 nm; T < 1% | Germanium | 3 |
| STO-WBP10290-11490 | LWIR | 10290 ± 100 – 11490 ± 100 | 10490-11290 | T>=80% | 1590-16090 nm; T < 1% | Germanium | 0.8 |
| STO-WBP10300-11400 | LWIR | 10300 ± 100 – 11400 ± 100 | 10500-11100 | T>=80% | 7000-14000 nm; T < 1% | Germanium | 0.9 |
| STO-WBP10300-11500 | LWIR | 10300 ± 120 – 11500 ± 120 | 10800-11300 | T>=85% | 1590-16090 nm; T < 1% | Germanium | 0.8 |
| STO-WBP10250-10850 | LWIR | 10340 ± 50 – 10940 ± 50 | 10440-10840 | T>=80% | 590-14090 nm; T < 1% | Germanium | 0.3 |
| STO-WBP10340-10840 | LWIR | 10340 ± 50 – 10840 ± 50 | 10440-10740 | T>=80% | 590-14090 nm; T < 1% | Germanium | 0.3 |
| STO-WBP10340-11040 | LWIR | 10340 ± 50 – 11040 ± 50 | 10440-10940 | T>=80% | 590-14090 nm; T < 1% | Germanium | 0.3 |
| STO-WBP10360-10860 | LWIR | 10360 ± 50 – 10860 ± 50 | 10460-10760 | T>=90% | 1060-14060 nm; T < 1% | Germanium | 0.3 |
| STO-WBP10400-11300 | LWIR | 10400 ± 100 – 11300 ± 100 | 10700-11100 | T>=90% | 7000-14000 nm; T < 1% | Germanium | 1 |
| STO-WBP10440-11040 | LWIR | 10440 ± 50 – 11040 ± 50 | 10600-10900 | T>=80% | 590-14090 nm; T < 1% | Germanium | 0.3 |
| STO-WBP10540-11140 | LWIR | 10540 ± 50 – 11140 ± 50 | 10700-11000 | T>=80% | 590-14090 nm; T < 1% | Germanium | 0.3 |
| STO-WBP10600-11450 | LWIR | 10600 ± 100 – 11450 ± 100 | 10700-11350 | T>=85% | 7500-14000 nm; T < 1% | Germanium | 0.7 |
| STO-WBP10600-11800 | LWIR | 10600 ± 100 – 11800 ± 100 | 10980-11750 | T>=80% | 1590-16090 nm; T < 1% | Germanium | 0.8 |
| STO-WBP11300-15600 | LWIR | 11300 ± 100 – 15600 ± 100 | 11500-15000 | T>=70% | 10080-16080 nm; T < 1% | Wedge germanium | 2 |
| STO-WBP11400-12380 | LWIR | 11400 ± 60 – 12380 ± 60 | 11550-12230 | T>=85% | 2000-15000 nm; T < 1% | Germanium | 3 |
| STO-WBP11400-12600 | LWIR | 11490 ± 100 – 12690 ± 100 | 12000-12490 | T>=85% | 1590-16090 nm; T < 1% | Germanium | 0.8 |
| STO-WBP11500-12500 | LWIR | 11500 ± 50 – 12500 ± 50 | 11650-12350 | T>=85% | 2000-15000 nm; T < 1% | Germanium | 3 |
| STO-WBP11570-12570 | LWIR | 11570 ± 50 – 12570 ± 50 | 11770-12370 | T>=85% | 2000-15000 nm; T < 1% | Germanium | 3 |
Daha uzun dalga boylu kızılötesi enerjiyi geçirip daha kısa dalga boylarını engelleyen ek uzun geçiren modeller.
| Model | Spektral aralık | Cut-on (nm) | Geçirgenlik | Geçirgenlik aralığı (nm) | Engelleme | Altlık | Altlık kalınlığı (mm) |
|---|---|---|---|---|---|---|---|
| STO-LP1500 | SWIR | 1500 ± 100 | T>=85% | 1600-5300 | 400-1400 nm; T < 1% | Sapphire | 0.3 |
| STO-LP1700 | SWIR | 1700 ± 100 | T>=80% | 1750-3400 | 800-1600 nm; T < 1% | Silicon | 0.5 |
| STO-LP1800 | SWIR | 1800 ± 50 | T>=80% | 1850-3400 | 800-1600 nm; T < 1% | Silicon | 0.5 |
| STO-LP2200 | SWIR | 2200 ± 100 | T>=90% | 2700-3500 | 400-1800 nm; T < 1% | Silicon | 0.762 |
| STO-LP2250 | SWIR | 2250 ± 50 | T>=90% | 2400-3600 | 1500-2100 nm; T < 1% | Silicon | 1 |
| STO-LP2900 | MWIR | 2900 ± 50 | T>=90% | 3050-5100 | 1300-2600 nm; T < 1% | Zinc selenide | 0.5 |
| CUT3200 | MWIR | 3400 ± 10 | T>=90% | 3480-5350 | 1500-3266 nm; T < 1% | Germanium | 0.3 |
| CUT3500 | MWIR | 3670 ± 50 | T>=90% | 3800-5600 | 1500-3500 nm; T < 1% | Germanium | 1, 2.5 |
| STO-LP3710+DLC | MWIR | 3710 ± 50 | T>=70% | 4000-5500 | 1500-3400 nm; T < 1% | Silicon | 0.5 |
| STO-LP3730 | MWIR | 3730 ± 50 | T>=90% | 4400-4900 | 1700-3700反射; T < 1% | Germanium | 0.5, 0.7 |
| STO-LP3760 | MWIR | 3760 ± 60 | T>=90% | 3960-4800 | 1600-3480 nm; T < 1% | Germanium | 0.5 |
| STO-LP3850 | MWIR | 3850 ± 50 | T>=90% | 4000-5000 | 1500-3500 nm; T < 1% | Germanium | 0.5 |
| STO-LP4730 | MWIR | 4730 ± 200 | T>=80% | 4900-5150 | 400-4200 nm; T < 1% | Sapphire | 1 |
| STO-LP5800 | MWIR/LWIR transition | 5800 ± 150 | T>=80% | 6000-13000 | 2000-5500 nm; T < 1% | Silicon | 0.5 |
| STO-LP6200 | MWIR/LWIR transition | 6200 ± 100 | T>=90% | 6400-12600 | 2000-6000 nm; T < 1% | Germanium | 0.9, 3, 3.5 |
| STO-LP6300 | MWIR/LWIR transition | 6300 ± 100 | T>=90% | 6550-14500 | 1500-6100 nm; T < 1% | Germanium | 0.3 |
| STO-LP6400 | MWIR/LWIR transition | 6400 ± 100 | T>=90% | 6500-12600 | 2000-6000 nm; T < 1% | Germanium | 0.9, 3 |
| STO-LP6500 | MWIR/LWIR transition | 6500 ± 50 | T>=85% | 6800-11000 | 1500-6200 nm; T < 1% | Germanium | 0.9, 2.8, 3 |
| STO-LP7250 | MWIR/LWIR transition | 7250 ± 50 | T>=90% | 7450-11000 | 1400-7000 nm; T < 1% | Germanium | 2.5 |
| STO-LP7570 | MWIR/LWIR transition | 7570 ± 70 | T>=90% | 7770-12600 | 1010-7320 nm; T < 1% | Germanium | 0.3 |
| STO-LP7675 | MWIR/LWIR transition | 7675 ± 75 | T>=90% | 8000-14000 | 1500-7550 nm; T < 1% | Germanium | 0.3 |
| STO-LP7770 | MWIR/LWIR transition | 7770 ± 70 | T>=90% | 7870-12600 | 1010-7320 nm; T < 1% | Germanium | 0.3 |
| STO-LP7950 | MWIR/LWIR transition | 7950 ± 150 | T>=85% | 8050-14000 | 190-7800 nm; T < 1% | Germanium | 1 |
| STO-LP9000 | LWIR | 9000 ± 300 | T>=90% | 9500-12500 | 400-8500 nm; T < 1% | Germanium | 0.5 |
| STO-LP10000 | LWIR | 10000 ± 70 | T>=90% | 10150-14300 | 1500-9800 nm; T < 1% | Zinc selenide | 0.5 |
| STO-LP10015 | LWIR | 10015 ± 100 | T>=85% | 10450-14500 | 1500-9800 nm; T < 1% | Germanium | 0.3 |
| STO-LP10600 | LWIR | 10600 ± 100 | T>=80% | 11000-14000 | 1500-10000 nm; T < 1% | Germanium | 2.7 |
| STO-LP10900 | LWIR | 10900 ± 100 | T>=80% | 11200-15400 | 1500-10750 nm; T < 1% | Germanium | 1 |
| STO-LP11050 | LWIR | 11050 ± 50 | T>=80% | 11200-15400 | 1500-10750 nm; T < 1% | Germanium | 0.8, 0.9 |
| STO-LP11190 | LWIR | 11190 ± 100 | T>=80% | 11500-15700 | 1500-10750 nm; T < 1% | Germanium | 0.8, 1 |
| STO-LP11600 | LWIR | 11600 ± 100 | T>=85% | 11800-12200 | 7000-11200 nm; T < 1% | Germanium | 0.9 |
| STO-LP11700 | LWIR | 11700 ± 100 | T>=80% | 11900-12300 | 7000-11200 nm; T < 1% | Germanium | 0.8, 0.9, 1, 2.7 |
Ek kızılötesi yansıma önleyici kaplama aralıkları. Kaynakta doğrulanmadıkça boyut ve malzeme ayrıntıları teklif için referans verisidir.
| Model | Spektral aralık | Geçirgenlik aralığı (nm) | Ortalama geçirgenlik | Altlık kalınlığı (mm) |
|---|---|---|---|---|
| STO-AR1000~2600 | SWIR | 1000-2600 | T>=90% | 1, 1.6, 6 |
| STO-AR1000~5100 | MWIR | 1000-5100 | T>=80% | 0.5, 1 |
| STO-AR1200~5500 | MWIR | 1200-5500 | T>=85% | 0.5 |
| STO-AR1250-1650 | SWIR | 1250-1650 | T>=99% | 0.3 |
| STO-AR1500~1600 | SWIR | 1500-1600 | T>=97% | 0.3, 1 |
| STO-AR1580~6900 | MWIR | 1580-6900 | T>=85% | 0.5, 1 |
| STO-AR1600~5300 | MWIR | 1600-5300 | T>=90% | 0.5, 1 |
| STO-AR1800~10000 | MWIR/LWIR transition | 1800-10000 | T>=90% | 1.2 |
| STO-AR1800~6000 | MWIR | 1500-5000 | T>=95% | 0.5 |
| STO-AR2000~12000 | MWIR/LWIR transition | 2000-12000 | T>=85% | 0.5 |
| STO-AR2000~14000 | LWIR | 2000-14000 | T>=80% | 0.5 |
| STO-AR2000~5600 | MWIR | 2000-5600 | T>=85% | 0.3, 1 |
| STO-AR2000~6000 | MWIR | 2000-6000 | T>=90% | 1, 5 |
| STO-AR2100~5500 | MWIR | 2100-5500 | T>=90% | 0.9, 1 |
| STO-AR2300~12600 | MWIR/LWIR transition | 2300-12600 | T>=90% | 1, 1.6 |
| STO-AR2300~5500 | MWIR | 2300-5500 | T>=92% | 1 |
| STO-AR2400~14000 | LWIR | 2400-14000 | T>=80% | 0.8, 2 |
| STO-AR2500~12000 | MWIR/LWIR transition | 2500-12000 | T>=90% | 1, 1.6 |
| STO-AR2500~12600 | MWIR/LWIR transition | 2500-12600 | T>=90% | 1.6 |
| STO-AR2500~14000 | LWIR | 2500-14000 | T>=85% | 0.5 |
| STO-AR2500~3300 | MWIR | 2500-3300 | T>=90% | 0.65, 1, 3 |
| STO-AR2500~4600 | MWIR | 2500-4600 | T>=90% | 0.5 |
| STO-AR2500~4700 | MWIR | 2500-4700 | T>=90% | 0.7, 0.8, 2.9, 12 |
| STO-AR2500~6000 | MWIR | 2500-6000 | T>=85% | 0.5 |
| STO-AR2600~5200 | MWIR | 2600-5200 | T>=90% | 0.5, 4 |
| STO-AR2680~4520 | MWIR | 2680-4520 | T>=90% | 0.5, 2.8, 3 |
| STO-AR2700~5300 | MWIR | 2700-5300 | T>=95% | 0.5 |
| STO-AR2700~9100 | MWIR/LWIR transition | 2700-9100 | T>=90% | 0.5, 5 |
| STO-AR2800~4900 | MWIR | 2800-4900 | T>=90% | 0.9 |
| STO-AR2800~5500 | MWIR | 2800-5500 | T>=90% | 0.5 |
| STO-AR2850~4850 | MWIR | 2850-4850 | T>=90% | 0.5 |
| STO-AR2900~5400 | MWIR | 2900-5400 | T>=90% | 6 |
| STO-AR3000~11000 | MWIR/LWIR transition | 3000-11000 | T>=90% | 0.38, 1.6 |
| STO-AR3000~12600 | MWIR/LWIR transition | 3000-12600 | T>=90% | 0.4, 0.9, 1.6 |
| STO-AR3000~14000 | LWIR | 3000-14000 | T>=90% | 0.3, 0.6, 0.7, 0.75, 0.8, 0.9, 1 |
| STO-AR3100~3600 | MWIR | 3100-3600 | T>=90% | 1 |
| STO-AR3200~3600 | MWIR | 3200-3600 | T>=85% | 0.45, 0.9 |
| STO-AR3200~5500 | MWIR | 3200-5500 | T>=85% | 0.9, 1 |
| STO-AR3400~12500 | MWIR/LWIR transition | 3400-12500 | T>=90% | 1 |
| STO-AR3500~10000 | MWIR/LWIR transition | 3500-10000 | T>=90% | 0.5, 1 |
| STO-AR3500~5000 | MWIR | 3500-5000 | T>=95% | 0.5, 1, 1.6 |
| STO-AR3600~4800 | MWIR | 3600-4800 | T>=95% | 0.5, 1 |
| STO-AR3600~5000 | MWIR | 3600-5000 | T>=95% | 0.5 |
| STO-AR3700~4800 | MWIR | 3700-4800 | T>=90% | 0.5, 1 |
| STO-AR3700~5000 | MWIR | 3700-5000 | T>=95% | 0.9 |
| STO-AR400~1700 | NIR | 400-1700 | T>=90% | 0.85, 1 |
| STO-AR400~3000 | SWIR | 400-3000 | T>=85% | 1.5 |
| STO-AR400~880 | NIR | 400-880 | T>=90% | 0.5 |
| STO-AR420~780 | NIR | 420-780 | T>=90% | 1 |
| STO-AR4300 | IR | 4300 | T>=90% | 1 |
| STO-AR4500~13000 | LWIR | 4500-13000 | T>=90% | 0.8, 1 |
| STO-AR5500~11000 | LWIR | 5500-11000 | T>=90% | 0.8, 2.5 |
| STO-AR5500~14000 | LWIR | 5500-14000 | T>=80% | 0.5 |
| STO-AR6000~10500 | LWIR | 6000-10500 | T>=90% | 0.9, 1 |
| STO-AR6000~11000 | LWIR | 6000-11000 | T>=90% | 2.5 |
| STO-AR6000~13000 | LWIR | 6000-13000 | T>=90% | 1 |
| STO-AR6000~18000 | LWIR | 6000-18000 | T>=48% | 0.8, 1 |
| STO-AR6200~12600 | LWIR | 6200-12600 | T>=90% | 0.5, 0.6, 0.9, 3, 6 |
| STO-AR6500~11000 | LWIR | 6500-11000 | T>=95% | 1 |
| STO-AR7000~12500 | LWIR | 7000-12500 | T>=95% | 0.4, 2.5, 2.8 |
| STO-AR7000~12600 | LWIR | 7000-12600 | T>=90% | 0.7, 0.9, 1, 3 |
| STO-AR7000~14000 | LWIR | 7000-14000 | T>=90% | 1 |
| STO-AR7000~14500 | LWIR | 7000-14500 | T>=90% | 0.8, 1 |
| STO-AR7000~14600 | LWIR | 7000-14600 | T>=90% | 0.9, 1, 3 |
| STO-AR7000~16000 | LWIR | 7000-16000 | T>=90% | 0.8, 0.9, 1, 3.5 |
| STO-AR7400~10700 | LWIR | 7400-10700 | T>=95% | 2.6, 3 |
| STO-AR7400~10900 | LWIR | 7400-10900 | T>=94% | 0.8, 2.9 |
| STO-AR7400~12800 | LWIR | 7400-12800 | T>=90% | 0.9, 1 |
| STO-AR7500~10100 | LWIR | 7500-10100 | T>=90% | 0.7, 0.9, 1, 2.9, 8.7 |
| STO-AR7500~10500 | LWIR | 7500-10500 | T>=93% | 0.7, 1 |
| STO-AR7500~10700 | LWIR | 7500-10700 | T>=90% | 1 |
| STO-AR7500~11000 | LWIR | 7500-11000 | T>=90% | 2.5, 2.8 |
| STO-AR7500~13000 | LWIR | 7500-13000 | T>=90% | 0.9, 5 |
| STO-AR7500~13500 | LWIR | 7500-13500 | T>=90% | 0.8 |
| STO-AR7500~9700 | LWIR | 7500-9700 | T>=85% | 0.75 |
| STO-AR7600~12700 | LWIR | 7600-12700 | T>=93% | 1 |
| STO-AR7700~11000 | LWIR | 7700-11000 | T>=95% | 0.9, 3 |
| STO-AR7700~9300 | LWIR | 7700-9300 | T>=93% | 0.3, 0.75 |
| STO-AR7800~10000 | LWIR | 7800-10000 | T>=95% | 0.9, 1 |
| STO-AR8000~10000 | LWIR | 8000-10000 | T>=92% | 0.9, 2.7, 2.8, 3 |
| STO-AR8000~13500 | LWIR | 8000-13500 | T>=90% | 3 |
| STO-AR8000~15000 | LWIR | 8000-15000 | T>=93% | 2 |
| STO-AR800~4000 | SWIR | 800-4000 | T>=80% | 1 |
| STO-AR9000~16500 | LWIR | 9000-16500 | T>=90% | 1.6 |
| STO-AR900~1700 | SWIR | 900-1700 | T>=90% | 1.6 |
| STO-AR9500~17000 | LWIR | 9500-17000 | T>=80% | 0.7, 1.6 |
IR filtrelerini dedektör malzemesine, altlık geçirgenliğine ve çalışma sıcaklığına göre eşleştirin. Tüm IR bantları birbirinin yerine kullanılamaz.
Kaplama performansından önce malzeme seçimi kullanılabilir dalga boyu aralığını sınırlayabilir. IR uygulamalarında önce altlığı doğrulayın.
Termal görüntüleme veya gaz algılama için hedef soğurma bandını, engelleme aralığını ve çalışma ortamını belirtin.
Sayfa, verilerin bulunduğu durumlarda yakın kızılötesi, kısa dalga, orta dalga ve uzun dalga kızılötesi filtre gereksinimlerini kapsar.
Altlık malzemelerinin geçirgenlik aralıkları farklıdır; bu nedenle malzeme, hedeflenen kızılötesi dalga boyu bandını desteklemelidir.
Evet. Kızılötesi sistemler için özel dalga boyu bantları, boyutlar, altlık seçenekleri ve kaplamalar talep edilebilir.
Kalite ve mevzuata uygunluk
OEM programları, laboratuvar cihazları ve endüstriyel sistemler için OPTOStokes, tedarikçi değerlendirmesinin başından itibaren kaliteyi, malzeme uygunluğunu ve mühendislik desteğini açıkça sunar.
Üretim amaçlı optik bileşenlerde proses kontrolü, muayene kayıtları ve tekrarlanabilir kaplama iş akışları.
Uygun projeler ve düzenlemeye tabi tedarik zincirleri için uygunluk belgeleri hazırlanabilir.
Dalga boyu, FWHM, altlık, AOI, boyut ve montaj gereksinimleri mühendislik ekibiyle değerlendirilebilir.
Size özel bir teklif için hedef dalga boyunu, engelleme seviyesini, geçirgenliği ve teknik çizim gereksinimlerini paylaşın.
Mühendislerimiz en uygun optik çözümü seçmenize yardımcı olur.