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I. Ashley T. M. l)onov,ill, l. l'l. W. Wt)_devt,r. and R. Z, l)albev. h,ctron Microscopy co,ltings for Iusiotl ta_gt,ls," 1, _tt, Sit. , Ig (3), 73h (IqSI). Ih. N1. Slaggs, M, l_,dooch, M, R. ]. _: 1'184, N BS 5pt, cia I l'ub, 727, Iq84, p, 3qt_, •1. M. R. Ko/lowski, M, Staggs, M. I]alooch, R. TIw Inlt, rn,ltitmal 5oeh,lv for ()pitt al lillgitlt't'ril/g, Iiellinghaln, _V,,\, Iqq I; I'r_,_. ' 16241, p, 37q. 17, NI. (,. Staggs, lkl. R. Kozlmvski, W. I. _it, kh,lus. ,ind M. llgillt,t,rillg, lk, llingham, WA.
I(a), The ir_tro. duction of randturt phase pl,_tes (Rl'l's) in the be,_rn produces ,a laser spot that is unit:orn'_on the I,_rge scale Ishown in Fig. I(b) ft,r tlw Nova laserl. Spatial sm_,t,tl'tit-g reduces the spectral intt, nsity irt the lower sp,_ti,_lwave numbers. Tl_is reduction is predictt, d to limit signitit:,mtly the growth t,! til,_ment,_tion. veil known (negative t,xpt,nential) intensity distributitm. 'lbmpt,ral smt,t_tlfing rapidly varies in time the finest:die speckle structt_rt, prt_dtlct, d by an RI'I'.
NI_IS5pet'. I'ub. 509, _,u",',,//,p. 2(_11. m, cr Ittdttted l)mlt, lg¢ lit ()ptt, al A|,l,'rtal,: Iqt_2, (SI'II: .... Tht, Intt,rn,ltion,d Socit, lv hlr ()ptical tingitlt,t,rJtlg, l_t'llitlghdtll, I,V/\, Iqqt; I_t,,_. ,':,1'1118481. 13() TECHNIQUES FOR MBAR TO NEAR-GBAR EQUATION-OF-STATE MEASUREMENTS WITH THE NOVA LASER R. Catll,h' L. B. Da Sih,a S, G. Gh,patiltlliJl_ S. M. Ladle T. S, lh'rI31 D, W. _ars, Direct ilhimination of metals by a Nova-class teraw lit laser beam can produce pwssures ,if nearly loll Mbar.