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 98.
xvi. lappuse
... peak powers associated with the picosecond micropulses , stimulated Raman scattering and self focusing may produce phase distortion in window materials . Finally , thermal distortion must be considered as the lowest order threat ...
... peak powers associated with the picosecond micropulses , stimulated Raman scattering and self focusing may produce phase distortion in window materials . Finally , thermal distortion must be considered as the lowest order threat ...
2. lappuse
... peak power , inertial confinement fusion systems . Such beam splitters seem to suffer mechanical degradation thought to be related to stimulated Brillouin scattering in these systems . This meeting has always addressed issues from ...
... peak power , inertial confinement fusion systems . Such beam splitters seem to suffer mechanical degradation thought to be related to stimulated Brillouin scattering in these systems . This meeting has always addressed issues from ...
12. lappuse
... peak temperatures approaching the melting point can be reached with no indication of damage . This suggests that melting is the mode of failure under these conditions . Shen , et al . [ 16 ] have since been able to provide additional ...
... peak temperatures approaching the melting point can be reached with no indication of damage . This suggests that melting is the mode of failure under these conditions . Shen , et al . [ 16 ] have since been able to provide additional ...
14. lappuse
... peak temperature increase , during the laser pulse , is very nearly proportional to the fourth power of the photon flux at 532 nm in KBr . Therefore , the thermal stress is στ = Cak Fo ( 6 ) a is the coefficient of thermal expansion , C ...
... peak temperature increase , during the laser pulse , is very nearly proportional to the fourth power of the photon flux at 532 nm in KBr . Therefore , the thermal stress is στ = Cak Fo ( 6 ) a is the coefficient of thermal expansion , C ...
15. lappuse
... peak photon flux . The experimental procedure is to expose the sample to a series of laser pulses of uniform peak power at a repetition frequency of about one Hertz . The sample is mounted on the cold finger of a closed cycle optical ...
... peak photon flux . The experimental procedure is to expose the sample to a series of laser pulses of uniform peak power at a repetition frequency of about one Hertz . The sample is mounted on the cold finger of a closed cycle optical ...
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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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