Page 371 - Tunable Lasers Handbook
P. 371
7 Optical Parametric Oscillators 33 1
TABLE 5 Sellmeier Coefficients for Selected Nonlinear Crystalsa
Crystal A B C D E or,,
ADP o 1.37892 0.91996 0.01219 0.15771 5.7600 0.00015
e 1.35302 0.80752 0.01227 0.02612 3.3156 0.000 11
KDP o 1.41314 0.84308 0.01229 0.26923 10.2180 0.0.3011
e 1.40442 0.72733 0.01201 0.07971 12.4840 0.00007
CD”X 0 1.65075 0.75762 0.022 18 0.03942 1.1399 0.00072
e 1.69749 0.653 13 0.02365 0.01710 7.5095 0.00065
LiNbO, o 2.33907 2.58395 0.04588 13.8169 519.658 0.00022
e 2.35081 2.22518 0.01371 15.9773 711.146 9.00025
BBO o 1.71283 1.01790 0.01790 2.23130 138.650 0.000 13
e 1.50569 0.86544 0.0 15 12 0.56178 218.360 0.00014
KTP I 2.22337 0.78681 0.04746 0.67167 51.90 0.00039
1’ 2.30590 0.71572 0.05387 1.00870 77.50 0.00043
2.3 5 119 0.96655 0.058 12 1.21673 77.50 0.00065
LBO I 2.07557 0 38193 0.02597 2.60858 191.01 0.00052
1 1.61856 0.97317 0.01355 1.48336 201.16 0.00109
2.00372 0.58147 0.02176 2.5 5 7 7 7 155.81 0.00077
AgGaS, o 3.02917 2.76318 0.08343 2.03585 910.18 1 0.00055
e 3.31365 2.22509 0.10018 2.01258 911.181 0 0005 1
XgCaSr, o 1.08903 2.76132 0 15669 1 1.72 170 9502.6 0 OOC65
e 4.44502 2.23190 0.20592 8.61981 7051.1 0.00037
CdSe o 1.16222 1.82886 0.12118 2.4863 1 3810.03 0.00014
1.01216 2.07361 0.10709 13.8 169 2235.17 0.00022
ZnGeP, o 4.61167 5.10087 0.13656 1.27777 1653.89 0.00018
e 4.71531 526358 0.11386 2.39310 1000.82 0.00058
T13AsSe3 o 1 .o 9.977 0 18923 0.067 100.0
e 1 .o 8.782 0.18923 0.05 1 100.0
GVavelengths are in micrometers.
combinations can be obtained in a straightforward manner once the Sellmeier
constants are known.
ADP, KDP. and CD*A can be used to generate output at wa\yelengths in the
visible and near infrared, to about 1.1 pm or somewhat beyond. ADP and KDP
are very similar, even to the shape of the phase-matching curve (Fig. 12). CD*;A,
on the other hand, does not have enough birefringence to be pumped by a 0.355-
pm pump. However, by using a 0.532-pm pump. a parametric device tunable at
wavelengths longer than about 0.85 pm is possible (Fig. 13). 4s phase matching
can be obtained very near 90”, long nonlinear crystals may be employed without
seriously affecting efficiency through the deleterious effects of birefrin, Vence.

