LAK9G15  691548.353

Radiation Resistance 2_klein_bearbeitet.jpg
SCHOTT Advanced Optics offers a variety of radiation resistant glass types with different dispersion properties. These glass types are well-suited to use in surroundings with high radioactivity.
Characteristics
nd 1.69064 νd 54.76
ne 1.69364 νe 54.53
nF-nC 0.012612 nF'-nC' 0.012721
Characteristics λ [nm]
n2,325.4 2,325.4 1.65362
n1,970.1 1,970.1 1.66043
n1,529.6 1,529.6 1.66783
n1,060.0 1,060.0 1.67552
nt 1,014.0 1.67639
ns 852.1 1.67999
nr 706.5 1.68462
nC 656.3 1.68680
nC' 643.8 1.68741
Characteristics λ [nm]
n632.8 632.8 1.68798
nD 589.3 1.69052
nd 587.6 1.69064
ne 546.1 1.69364
nF 486.1 1.69941
nF' 480.0 1.70013
ng 435.8 1.70630
nh 404.7 1.71205
ni 365.0
Characteristics λ [nm]
n334.1 334.1
n312.6 312.6
n296.7 296.7
n280.4 280.4
n248.3 248.3
Characteristics λ [nm]
τ25/2500 2,500 0.160
τ25/2325 2,325 0.490
τ25/1970 1,970 0.910
τ25/1530 1,530 0.987
τ25/1060 1,060 0.996
τ25/700 700 0.986
τ25/660 660 0.982
τ25/620 620 0.978
τ25/580 580 0.973
τ25/546 546 0.964
τ25/500 500 0.930
τ25/460 460 0.810
τ25/436 436 0.570
τ25/420 420 0.320
τ25/405 405 0.090
τ25/400 400 0.040
τ25/390 390 0.010
τ25/380 380 0.000
τ25/370 370
τ25/365 365
τ25/350 350
τ25/334 334
τ25/320 320
τ25/310 310
τ25/300 300
τ25/290 290
τ25/280 280
τ25/270 270
τ25/260 260
τ25/250 250
Characteristics λ [nm]
τ10/2500 2,500 0.480
τ10/2325 2,325 0.752
τ10/1970 1,970 0.963
τ10/1530 1,530 0.995
τ10/1060 1,060 0.998
τ10/700 700 0.994
τ10/660 660 0.993
τ10/620 620 0.991
τ10/580 580 0.989
τ10/546 546 0.985
τ10/500 500 0.971
τ10/460 460 0.919
τ10/436 436 0.799
τ10/420 420 0.634
τ10/405 405 0.382
τ10/400 400 0.292
τ10/390 390 0.122
τ10/380 380 0.026
τ10/370 370
τ10/365 365
τ10/350 350
τ10/334 334
τ10/320 320
τ10/310 310
τ10/300 300
τ10/290 290
τ10/280 280
τ10/270 270
τ10/260 260
τ10/250 250
Characteristics
Ps,t 0.2852
PC,s 0.5400
Pd,C 0.3040
Pe,d 0.2383
Pg,F 0.5462
Pi,h
P's,t 0.2828
P'C',s 0.5834
P'd,C' 0.2533
P'e,d 0.2362
P'g,F' 0.4849
P'i,h
Characteristics
ΔPC,t 0.0205
ΔPC,s 0.0095
ΔPF,e -0.0018
ΔPg,F -0.0055
ΔPi,g