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6. J. Smrz, Phys. Rev. Lett. 73,2700 11. S. E. Bodner, Phys. Rev. Lett. 33,761 7. V. N. Goncharov, R. Betti, R. L. McCrory, P. Sorotokin, Verdon, Phys. Plasmas 3, 1402 (1996). and C. P. 12. R. Betti, V. N. Goncharov, Plasmas 5, 1446 (1998). 8. V. N. D thesis, University of Rochester, 1998. 13. R. L. McCrory and C. P. Verdon, in ConrputerApplicorions in Plasma Science and Engineering, edited by A. T. Drobot (Springer-Verlag, New York, 1991). 9. ( 1994). ( 1974). R. L. McCrory, and C. P. Verdon, Phys.
In to corroborate this correlation from literature data. In the same vein, there should be a damage-initiation stress effect for ( OZZ= O) and (b) the stressed sample (aZZ = –6 psi). Note that in Fig. 28(a) the crack growth has pushed the crack tip displayed sur- mismatch between the substrate interracial stress. This would be most readily observable in antireflective coatings as these permit significant laser intensity to reach the substrate interface. Finally, there remains an urgent question to be resolved as to whether this phenomenon is unique to fused silica or may be present also in other glasses.
Yaakobi, D. D. Meyerhofer, R. P. J. Town, J. A. Delettrez, V. Glebov, D. K. Bradley, J. P. Knauer, M. D. Cable, and T. J. Ognibene, Bull. Am. Phys. Sot. 43, 1784 ( 1998). 13. E. Goldman, Laboratory for Laser Energetic sity of Rochester ( 1973). 14. H. Brysk, Plasma Phys. 15,611 (1973). 15. W. H. $cienrijlc Comparing, 2nd ed. (Cambridge University Press, Cambridge, England, 1992). to times in the using the NTD. Further, a comparison with detailed mixing models may enable the identification conditions IN COMPRESSEDICF TARGETS of ( 1981).