Mirror DB

  
Please select the best matching items for your application.
Unit:
Main Type:
Sub-type:
Angle of incidence:
The numbers between the parentheses do show the number of available designs in the given category
Spectral filtering:
Min nm

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Max nm

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* CE (eV) = Central Energy * AOI = Angle of Incidence in degrees * Pol = Polarization
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Results 1 - 284 of 206

Name Min (nm) Max (nm) CW (nm) Reflectivity GDD (fs2) AOI Pol Comments
AR400 400 700 550 0.00 % 0 both Broad-band anti-reflection …
AR550-1130 580 1125 852 0.00 % 0 p Broad-band anti-reflection …
AR770 770 810 790 0.00 % 0 p Broad-band IR anti-reflection …
ARIR16 1550 3200 2375 0.00 % 5 p Broad-band IR anti-reflection …
ARIR17 1500 4000 2750 0.00 % 0 p Broad-band IR anti-reflection …
ARIR19 1500 3200 2350 0.00 % 0 p Broad-band IR anti-reflection …
BS101 1550 2150 1850 50.00 % 0 7 p Beam splitter
BS1201 290 310 300 97.00 % 75 p Beam splitter
BS1202 1015 1050 1032 0.00 % 45 p Thin-film polarizer
BS1311_RC2 840 860 850 99.99 % 45 s Thin-film polarizer
BS1412 500 950 725 99.98 % 45 s Beam splitter, GDD …
BS1501 500 750 625 99.00 % -40 5 p Beam splitter, GDD …
BS1502 700 1400 1050 % 0 45 p Beam splitter, GDD …
BS1503 700 1350 1025 % 0 45 p Beam splitter, GDD …
BS1504 450 1050 750 50.00 % 0 55 p Beam splitter, GDD …
BS1551 845 855 850 99.00 % 45 s Beam splitter, GDD …
BS32 625 975 800 8.00 % 0 45 p Beam splitter, GDD …
BS41 375 460 417 98.00 % -20 45 p Beam splitter
BS45deg 1520 1680 1600 45.00 % 45 p Beam splitter
BS71 525 925 725 33.00 % 0 5 p Beam splitter, GDD …
BSIR3 1000 1500 1250 1.00 % 0 45 p Beam splitter, GDD …
BS_NP 1500 1700 1600 45.00 % 45 p Beam splitter
CM101 730 880 805 99.00 % -115 7 p High-dispersive …
CM130 970 1120 1045 99.00 % -50 5 p Dispersive mirror …
CM1302 250 275 262 98.00 % 0 p High-reflective …
CM1321_RC2 770 840 805 99.95 % 0 0 p High-reflective …
CM1322_RC2 850 920 885 99.80 % 0 0 p High-reflective …
CM1331 760 840 800 99.00 % -30 0 p Broad-band dispersive …
CM135 270 273 271 98.00 % -60 7 p High-dispersive …
CM1401 258 270 264 99.95 % 0 0 p High-reflective …
CM1405_RC1 1000 1500 1250 99.70 % -60 0 p Broad-band complementary …
CM1405_RC2 1000 1375 1187 99.95 % -100 45 p Broad-band complementary …
CM1405_RC3 1000 1375 1187 99.98 % -60 45 p Broad-band complementary …
CM150 980 1100 1040 99.00 % -150 5 p Dispersive mirror …
CM1531 1900 2200 2050 99.70 % -200 5 p Dispersive mirror …
CM1601 505 540 522.5 99.90 % 0 7 p Dispersive mirror …
CM31 250 360 305 98.00 % 0 5 p Broad-band high-reflective …
CM313 230 270 250 95.00 % -65 8 s High-dispersive …
CM39 980 1080 1030 99.00 % -500 5 p Dispersive mirror …
CM53 450 650 550 99.00 % 0 5 p Broad-band high-reflective …
CM55 1200 1400 1300 99.00 % -60 5 p Dispersive mirror …
CM58 240 370 305 95.00 % 0 5 p Broad-band dichroic …
CM61 700 900 800 99.00 % 0 5 p Broad-band high-reflection …
CM63 720 1000 860 99.00 % -150 5 p Broad-band dispersive …
CM65 450 1200 825 94.00 % -30 5 p Ultra-broad-band …
CM68 725 1000 862 99.50 % -70 45 p Dispersive mirror
CM71 500 1000 750 98.00 % 0 45 p Beam splitter (dispersion …
CM81 700 900 800 99.00 % 0 5 p Broad-band high-reflection …
CM82 350 450 400 99.00 % -50 5 p Broad-band dispersive …
CM83 700 900 800 99.00 % -50 5 p Dispersive mirror …
DA2 680 880 780 99.00 % -100 5 p Broad-band double-angle …
F1203 720 880 800 99.00 % 0 45 p Beam splitter
F1204 650 900 775 99.00 % 0 45 s Beam splitter
F1306 250 280 265 49.00 % -20 45 p Beam splitter
F1307 750 850 800 50.00 % 0 10 p Beam splitter
F1308 950 1200 1075 98.00 % 0 p Beam splitter
F1309 720 900 810 99.00 % 45 s Beam splitter
F1310 300 430 365 90.00 % 0 p Beam splitter
F1311 500 850 675 50.00 % 0 45 s Beam splitter
F1351_RC3 1010 1030 1020 99.98 % 15 p Beam splitter, GDD …
F1401 800 1000 900 99.99 % 15 p Beam splitter, GDD …
F1402_RC1 650 900 775 90.00 % 75 s Thin-film polarizer
F1402_RC2 650 900 775 90.00 % 0 75 s Thin-film polarizer
F1403 240 260 250 90.00 % 0 p High-reflective …
F1502 650 900 775 93.00 % 0 75 s Thin-film polarizer
F1551 450 1000 725 5.00 % 0 0 p Beam splitter, GDD …
F1601 650 950 800 % 0 72 s Beam splitter, GDD …
FIR1 4700 6300 5500 99.00 % 0 p IR filter
FIR2 4650 6550 5600 65.00 % 0 p High-dispersive …
HD100 250 277 263 96.00 % -140 5 p High-dispersive …
HD103 1030 1050 1040 99.00 % 1750 5 p High-dispersive …
HD111 710 880 795 99.00 % -270 7 p High-dispersive …
HD116 700 870 785 99.00 % -250 7 s High-dispersive …
HD120 950 1120 1035 99.00 % -200 0 p High-dispersive …
HD121 1010 1050 1030 99.00 % -1000 5 p High-dispersive …
HD122 1010 1055 1032.5 99.00 % -1200 8 s High-dispersive …
HD123 1010 1060 1035 99.00 % -300 8 s High-dispersive …
HD1310 1010 1070 1040 99.00 % -1000 7 s High-dispersive …
HD1312 1050 1075 1062.5 99.00 % -3200 3 p High-dispersive …
HD1321 730 900 815 99.00 % -180 5 p High-dispersive …
HD1342 700 860 780 99.00 % -275 45 p High-dispersive …
HD1401_RC1 725 825 775 99.00 % -450 5 p High-dispersive …
HD1401_RC2 725 825 775 99.00 % 450 5 p High-dispersive …
HD1403_RC2 720 850 785 99.00 % p
HD15 780 830 805 99.00 % -1300 5 p High-dispersive …
HD1561 710 980 845 99.80 % 100 5 p Mirror with high …
HD1565 1010 1060 1035 99.80 % -1000 5 p High-dispersive …
HD1601 1027 1033 1030 99.93 % -3000 3 p High-dispersive …
HD1601_v2 600 800 700 99.50 % -150 7 p High-dispersive …
HD1607 760 800 780 99.90 % -1000 5 p High-dispersive …
HD301 770 1220 995 99.00 % -100 5 p Broad-band double-angle …
HD31 730 840 785 99.70 % -500 10 p High-dispersive …
HD40 1020 1040 1030 99.00 % -2500 5 p High-dispersive …
HD51 1028 1037 1032 99.50 % -4000 5 p High-dispersive …
HD58 690 880 785 99.50 % -275 7 p High-dispersive …
HD59 1000 1060 1030 99.00 % -500 5 p High-dispersive …
HD61 1020 1060 1040 99.50 % -1050 0 p High-dispersive …
HD64 1010 1050 1030 99.50 % -1000 5 p High-dispersive …
HD65 1010 1070 1040 99.50 % -1000 5 p High-dispersive …
HD67 690 880 785 99.50 % -320 5 p High-dispersive …
HD68 775 835 805 99.50 % -1000 5 p High-dispersive …
HD69 500 700 600 98.00 % -100 5 p High-dispersive …
HD71 400 650 525 99.00 % -50 5 p Broad-band double-angle …
HD86 1030 1050 1040 99.00 % -1200 3 p High-dispersive …
HD90 1020 1060 1040 99.00 % -1200 7 p High-dispersive …
HR101 300 1000 650 98.00 % 45 s Broad-band high-reflective …
HR1201 720 900 810 99.00 % 45 s Broad-band high-reflective …
HR1511 1032 1038 1035 99.90 % 0 45 s High-reflective …
HR24 660 1400 1030 99.00 % 19 p Broad-band high-reflective …
HR257 235 285 260 99.00 % 45 s UV high-reflector
HR266 255 275 265 98.00 % 45 s Dichroic mirror
HR45 660 1400 1030 99.00 % 40 p Broad-band high-reflective …
HRIR1 1990 3200 2595 99.00 % 5 p Broad-band high-reflective …
HRIR2 2000 3200 2600 99.00 % 5 p Dichroic mirror
HRVLT 460 940 700 98.00 % 45 p High-reflective …
IC1501 2050 2850 2450 98.50 % -450 5 p Broad-band dispersive …
IR11 2600 3200 2900 99.00 % 450 5 p Dispersive dichroic …
IR13 1900 3200 2550 99.00 % 5 p Dichroic mirror
IR1301 2100 2600 2350 98.00 % -100 0 p Broad-band dispersive …
IR1321_OC_RC1 4000 4600 4300 99.00 % -400 0 p Broad-band dispersive …
IR1321_OC_RC4 4000 4600 4300 98.00 % 0 0 p Broad-band dispersive …
IR1321_OC_RC5 3850 4700 4275 90.00 % 0 0 p Broad-band dispersive …
IR1322_RC1 3100 3950 3525 98.00 % -200 0 p Broad-band dispersive …
IR1332_RC3_L_S 3000 3800 3400 98.00 % -200 0 p Broad-band dispersive …
IR1401 1650 1950 1800 95.00 % 0 45 s Broad-band dispersive …
IR1401_RC2 1650 1950 1800 95.00 % 0 45 s Broad-band dispersive …
IR1402_RC2 1800 2400 2100 99.00 % 500 45 s Broad-band dispersive …
IR15 3000 4000 3500 98.00 % -500 5 p Broad-band dispersive …
IR1501 3500 4500 4000 99.00 % 45 s Dispersive mirror …
IR1502 1380 1760 1570 98.50 % 0 5 p Dispersive mirror …
IR16 1450 2050 1750 98.00 % -250 5 p Dispersive dichroic …
IR21 2850 3700 3275 98.00 % 0 p Beam splitter
IR24 2100 2850 2475 97.00 % -250 0 p Broad-band dispersive …
IR25 2000 3000 2500 97.00 % -200 0 p Broad-band dispersive …
IR26 2800 3400 3100 99.00 % 500 0 p Broad-band mirror …
IR41 2200 3200 2700 97.00 % -300 5 p Broad-band dispersive …
IRIC 2300 3500 2900 99.00 % 0 p Dichroic mirror
PC105 650 1350 1000 98.00 % -40 5 p Broad-band double-angle …
PC108_RC1 600 1050 825 99.50 % -50 5 p Broad-band double-angle …
PC109_RC1 500 800 650 97.00 % -25 5 p Broad-band dispersive …
PC109_RC2 500 800 650 97.00 % -25 5 p Broad-band double-angle …
PC120_RC1 450 675 562 99.00 % -30 5 p Broad-band dispersive …
PC120_RC2 450 675 562 99.00 % -30 5 p Broad-band double-angle …
PC122 500 1050 775 94.00 % -50 5 p Broad-band double-angle …
PC129 1250 2150 1700 95.00 % -100 7 p Broad-band double-angle …
PC1305 850 1200 1025 99.00 % -200 5 p Broad-band double-angle …
PC1305 _ RC2 690 870 780 99.00 % 150 p Broad-band double-angle …
PC1306 680 920 800 99.00 % -120 5 p Broad-band double-angle …
PC1315 1400 2200 1800 88.00 % 0 0 p Mirror with third …
PC1321 700 970 835 99.00 % -30 5 p Broad-band complementary …
PC1331 650 1380 1015 99.00 % -50 5 p Broad-band complementary …
PC1334_RC4 500 1000 750 98.00 % -40 5 p Broad-band double-angle …
PC139 660 880 770 99.00 % -150 5 p Broad-band dispersive …
PC139_RC2 660 900 780 99.00 % 150 5 p Broad-band complementary …
PC147 650 1350 1000 99.00 % -60 3 p Broad-band complementary …
PC148 760 960 860 99.00 % -50 5 p Dispersive mirror …
PC149_DA 750 1450 1100 99.00 % -30 5 p Broad-band double-angle …
PC149_LS 750 1500 1125 96.00 % 30 5 p Broad-band complementary …
PC150 570 960 765 99.00 % -50 5 p Broad-band complementary …
PC1541 650 950 800 99.30 % -35 5 p Broad-band dispersive …
PC1542 730 1300 1015 99.00 % -50 5 p Broad-band dispersive …
PC1581 1250 1550 1400 99.90 % -100 5 p Broad-band dispersive …
PC1601 800 1300 1050 99.50 % -100 5 p Broad-band double-angle …
PC1605 730 1300 1015 98.50 % 70 7 p Broad-band complementary …
PC32 550 1050 800 99.00 % -40 5 p Broad-band double-angle …
PC37_1 450 950 700 99.00 % -30 5 s Broad-band double-angle …
PC37_2 450 950 700 99.00 % -30 5 s Broad-band double-angle …
PC37_3 450 950 700 98.00 % -30 5 p Broad-band double-angle …
PC37_4 480 960 720 99.00 % -40 5 p Broad-band complementary …
PC40 730 970 850 99.00 % -50 0 p Broad-band dispersive …
PC41 700 940 820 99.00 % -60 5 p Dispersive dichroic …
PC42 500 1000 750 99.00 % -45 5 p Broad-band double-angle …
PC45 550 1100 825 99.00 % -40 7 p Broad-band complementary …
PC47 550 1100 825 98.00 % -60 7 p Broad-band complementary …
PC5 550 1100 825 99.00 % -40 5 p Broad-band complementary …
PC523_RC2_S_L 820 1220 1020 98.00 % -50 5 s Broad-band dispersive …
PC53 650 1230 940 99.00 % -60 5 p Broad-band double-angle …
PC54 925 1125 1025 99.00 % -50 12 both Broad-band dispersive …
PC55 450 600 525 99.00 % -40 5 p Broad-band dispersive …
PC61 1000 1750 1375 99.00 % -150 5 p Broad-band complementary …
PC70 500 1050 775 99.00 % -40 5 p Broad-band double-angle …
PC75 500 900 700 99.00 % -40 5 p Broad-band double-angle …
PC84 650 1000 825 99.00 % -70 5 p Broad-band double-angle …
PC93 650 1100 875 99.00 % -40 5 p Broad-band double-angle …
PC94 700 1350 1025 99.90 % -65 45 s Broad-band complementary …
PD1401_RC1 1020 1040 1030 99.00 % 5000 7 p Mirror with high …
PD1404_RC1 765 880 822 99.00 % 200 5 p Mirror with high …
PD1521 730 880 805 99.80 % 250 5 p Mirror with high …
PD1565 1010 1060 1035 99.80 % 1000 5 p Mirror with high …
PD1602 750 850 800 99.92 % 250 5 p Mirror with high …
PD41 1015 1045 1030 99.00 % 1000 6 p Mirror with high …
PD5 730 860 795 99.00 % 150 5 p Mirror with high …
PD51 775 840 807 99.00 % 1000 5 p Mirror with high …
RHD4 750 840 795 99.00 % -500 10 p High-dispersive …
TFP11 258 274 266 95.00 % 56 s Thin-film polarizer
TOD1 700 1000 850 99.00 % 0 10 p Mirror with third …
TOD1301 700 1400 1050 92.00 % 0 5 p Double-angle mirror …
TOD1501 1010 1110 1060 99.90 % 0 6 s Mirror with third …
TOD51 750 850 800 99.00 % 0 5 p Mirror with third …
TOD71 600 1200 900 94.00 % 0 5 p Mirror with negative …
TOD72 555 625 590 99.00 % 0 5 p Mirror with negative …
TOD9 740 860 800 99.00 % 7 p Mirror with third …
UBCM 400 1200 800 94.00 % -25 5 p Broad-band complementary …
UHR11 970 1120 1045 99.00 % 0 3 p High-reflective …
UHR1301 500 580 540 99.00 % 0 3 p High-reflective …
UHR1302 580 680 630 99.00 % 0 3 p High-reflective …
UHR17 1010 1110 1060 99.00 % 0 3 p High-reflective …
UHR21 750 850 800 99.00 % -8 0 p High-reflective …
UHR22 750 850 800 99.00 % -7 2 p High-reflective …
UHR23 760 810 785 99.00 % 3 p TOD dichroic mirror
UHR24 750 850 800 99.00 % 0 0 p High-reflective …
UHR35 530 625 577 99.00 % 0 0 p High-reflective …
UHR99 750 840 795 99.00 % 0 0 s High-reflective …
XUV100BW10 11.3 13.6 12.4 42.00 % -0.01 45 s XUV mirror
XUV101BW10 11.2 13.8 12.3 15.00 % 0.001 5 s XUV mirror
XUV105BW5 10.2 12.9 11.8 40.00 % -0.014 5 s XUV mirror
XUV107BW2 11.3 11.9 11.6 25.00 % -0.01 5 s XUV mirror
XUV109BW10 9.9 12.8 11.4 15.00 % -0.006 2 s XUV mirror
XUV112BW2 10.8 11.4 11.1 27.00 % -0.02 5 s XUV mirror
XUV112BW5 9.7 12 11.1 33.00 % -0.017 5 s XUV mirror
XUV115BW11 9.5 11.5 10.8 15.00 % 0.001 0 s XUV mirror
XUV125BW2 9.5 10.3 9.9 19.00 % 0.006 5 s XUV mirror
XUV130BW4 8.7 10.3 9.5 6.00 % 0.003 45 s XUV mirror
XUV130BW8 8.9 10.2 9.5 13.00 % -0.002 45 s XUV mirror
XUV134BW5 8.9 9.7 9.3 9.00 % -0.01 5 s XUV mirror
XUV135BW3 8.7 10.3 9.2 9.00 % -0.001 5 s XUV mirror
XUV145BW3 8.2 9.5 8.6 8.00 % 0.008 5 s XUV mirror
XUV150BW3 7.8 9 8.3 9.00 % 0.001 5 s XUV mirror
XUV155BW5 7.7 8.9 8 6.00 % 0.005 5 s XUV mirror
XUV170BW3 7.1 7.5 7.3 20.00 % -0.008 45 s XUV mirror
XUV180BW2 6.9 7.3 6.7 8.00 % -0.015 5 s XUV mirror
XUV200BW7 6 6.7 6.2 5.00 % 0.003 45 s XUV mirror
XUV22BW7 38.7 72.9 56.4 18.00 % 0.023 5 s XUV mirror
XUV25BW10 22.5 65.3 49.6 12.00 % 0.035 5 s XUV mirror
XUV26BW6 40 62 47.7 25.00 % 0.007 5 s XUV mirror
XUV28BW2 35.4 51.7 44.3 11.00 % -0.01 15 p XUV mirror
XUV300BW1 4.1 4.2 4.1 8.00 % -0.15 5 s XUV mirror
XUV32BW2 31 45.9 38.7 22.00 % 0.04 5 s XUV mirror
XUV35BW3 28.8 41.3 35.4 23.00 % -0.028 4 p XUV mirror
XUV35BW4 31 41.3 35.4 19.00 % 0.006 5 s XUV mirror
XUV37BW2 27.6 41.3 33.5 15.00 % -0.002 15 p XUV mirror
XUV38BW3 27.6 41.3 32.6 23.00 % 0.025 5 s XUV mirror
XUV41BW17 22.5 49.6 30.2 11.00 % 0.008 5 s XUV mirror
XUV42BW4 25.3 35.4 29.5 18.00 % -0.017 5 p XUV mirror
XUV43BW2 25.8 32.6 28.8 19.00 % 0.005 10 s XUV mirror
XUV46BW17 17.2 38.7 27 11.00 % 0.003 5 s XUV mirror
XUV50BW4 20.7 31 24.8 30.00 % 0.019 45 s XUV mirror
XUV50BW5 22.5 31 24.8 12.00 % 0.005 0 s XUV mirror
XUV53BW2 21.8 27.6 23.4 20.00 % -0.06 15 p XUV mirror
XUV54BW4 21 25.3 23 13.00 % 0.005 0 s XUV mirror
XUV57BW10 17.2 31 21.8 23.00 % 0.004 5 s XUV mirror
XUV59BW4 17.7 24.8 21 31.00 % 0.023 45 s XUV mirror
XUV60BW5 18.2 25.8 20.7 31.00 % -0.019 45 s XUV mirror
XUV63BW7 16.5 31 19.7 35.00 % 0.008 0 s XUV mirror
XUV65BW5 16.5 22.5 19.1 40.00 % 0.03 5 p XUV mirror
XUV65BW6 15.9 31 19.1 38.00 % 0.015 2 s XUV mirror
XUV66BW13 14.6 32.6 19.1 39.00 % 0.003 45 s XUV mirror
XUV67BW2 17.7 20 18.5 25.00 % -0.03 5 s XUV mirror
XUV67BW3 17 20.7 18.5 38.00 % 0.02 5 s XUV mirror
XUV68BW30 12.4 37.6 18.2 5.00 % 0.001 5 s XUV mirror
XUV70BW6 15.5 20.7 17.7 44.00 % 0.01 5 s XUV mirror
XUV70BW9 15.7 20.3 17.7 30.00 % -0.001 5 s XUV mirror
XUV75BW16 13.8 20.7 16.5 12.00 % -0.001 5 s XUV mirror
XUV82BW8 12.4 17.7 15.1 66.00 % 0.013 45 s XUV mirror
XUV82BW9 13.6 17 15.1 25.00 % -0.002 5 s XUV mirror
XUV83BW8 13.5 16.5 14.9 27.00 % -0.002 5 s XUV mirror
XUV85BW10 13.1 16.5 14.6 18.00 % -0.002 5 s XUV mirror
XUV87BW18 11.7 17.7 14.3 8.00 % -0.001 5 s XUV mirror
XUV90BW10 12.5 15.3 13.8 18.00 % -0.002 5 s XUV mirror
XUV90BW5 13.1 14.6 13.8 51.00 % -0.006 5 p XUV mirror
XUV90BW6 13.1 14.6 13.8 41.00 % -0.004 5 s XUV mirror
XUV90BW8 12.4 15.5 13.8 67.00 % 0.001 45 s XUV mirror
XUV92BW10 12.4 14.8 13.5 53.00 % -0.002 45 s XUV mirror
XUV92BW17 10.3 41.3 13.5 68.00 % -0.01 66 s XUV mirror
XUV92BW7 12.2 15.5 13.5 69.00 % 0.002 45 s XUV mirror
XUV92BW8 12.5 14.6 13.5 26.00 % -0.002 2 s XUV mirror
XUV93BW10 12.2 15.1 13.3 16.00 % -0.001 0 s XUV mirror
XUV93BW16 11.3 16.1 13.3 7.00 % -0.005 5 s XUV mirror
XUV93BW2 12.9 13.8 13.3 29.00 % -0.005 5 s XUV mirror
XUV93BW5 12.8 13.9 13.3 52.00 % -0.006 5 s XUV mirror
XUV93BW7 12.4 14.3 13.3 28.00 % -0.002 5 p XUV mirror
XUV94BW3 12.7 13.8 13.2 48.00 % -0.024 5 s XUV mirror
XUV95BW5 12.5 13.6 13.1 53.00 % -0.004 5 s XUV mirror
XUV95BW8 12.2 14.1 13.1 24.00 % 0.004 2 s XUV mirror