Laser Induced Damage in Optical Materials: Proceedings of a Symposium Sponsored by the American Society for Testing and Materials and by the National Bureau of StandardsU.S. Department of Commerce, National Bureau of Standards, 1989 |
No grāmatas satura
1.5. rezultāts no 39.
5. lappuse
... discussed in other categories of the meeting proper . Multi - pulse damage , the performance of materials in adverse environments and in particular short - wave lengths . In fact , considerable progress has been made in the damage ...
... discussed in other categories of the meeting proper . Multi - pulse damage , the performance of materials in adverse environments and in particular short - wave lengths . In fact , considerable progress has been made in the damage ...
8. lappuse
... discussed the importance of thermal cracking and thermal explosion of particulates as an important source of damage . An analysis of major damage to a cracked large optic at the Livermore National Laboratory was given . By examining the ...
... discussed the importance of thermal cracking and thermal explosion of particulates as an important source of damage . An analysis of major damage to a cracked large optic at the Livermore National Laboratory was given . By examining the ...
15. lappuse
... discussed above for four different temperatures . in KBr . The solid lines are the model predictions for these temperatures . All four curves were obtained using the same values for the adjustable parameters . The model matches the the ...
... discussed above for four different temperatures . in KBr . The solid lines are the model predictions for these temperatures . All four curves were obtained using the same values for the adjustable parameters . The model matches the the ...
27. lappuse
... discussed above . Figure 5 shows the results for SiO2 , where we measure the photoacoustic signal induced by both 266 and 1064 nm laser pulses as a function of the polarization of the heating pulse under the condition of constant pulse ...
... discussed above . Figure 5 shows the results for SiO2 , where we measure the photoacoustic signal induced by both 266 and 1064 nm laser pulses as a function of the polarization of the heating pulse under the condition of constant pulse ...
29. lappuse
... discussed in Sec . III . 1000 100 ACOUSTIC SIGNAL ( arb . units ) 10 10 ( a ) ( b ) 30 PULSE ENERGY ( arb . units ) 100 Figure 2. Photoacoustic signal as a function of the energy of a 266 nm laser pulse in ( a ) NaCl and ( b ) SiO2 ...
... discussed in Sec . III . 1000 100 ACOUSTIC SIGNAL ( arb . units ) 10 10 ( a ) ( b ) 30 PULSE ENERGY ( arb . units ) 100 Figure 2. Photoacoustic signal as a function of the energy of a 266 nm laser pulse in ( a ) NaCl and ( b ) SiO2 ...
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Citi izdevumi - Skatīt visu
Bieži izmantoti vārdi un frāzes
absorption Alamos approximately avalanche BaF2 band gap BDH sample Boulder Damage Symposium BRDF CaF2 calculated cerium chamfers coefficient crystal curve Damage in Optical damage testing damage threshold defects density dependence deposited detector diameter dielectric dye laser effect electron avalanche emission excimer excimer laser experimental F-center fluence fluoride fused silica glass Guenther heating imaging impurities incident increase intensity interface ionization irradiation J/cm² laser beam laser damage threshold Laser Induced Damage laser irradiation laser pulse laser-induced layer lens Livermore measured MgF2 mirror MOSFETs multiphoton Nd:YAG nonlinear observed optical coatings Optical Materials P.O. Box parameters particles peak photodiodes photon Phys polished poly-silicon pulse energy radiation reflectance reflectivity loss reflectors refractive index scan scatter shot shown in figure shows SiO2 slab spectra sputtering stress structure substrate surface technique temperature thickness thin films TiO2 transient values wavelength
Populāri fragmenti
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