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7 Apr 2011: lasers. Here, we report a high-power passively mode-locked Nd:YVO4 laser using GSA, with 1W average power. ... We use a 3315mm3 Nd:YVO4 crystal with a Nd3+-doping concentration of 0.3 at.% as the gain medium.

25 Jan 2008: fnes. s af. ter. actu. atio. n a. nd e. xte. ... nd e. xte. rnal. load. , K. Boundar. y d. ispla.

4 Dec 2006: 12140. nd. h. ts. beatal. inf. o. sea-. of. caused by hexagonal diamond.8,10 However, it is nowknown3 that hexagonal diamond has a Raman mode at 1cm21, just below that ... n-. d. nd. B. e,. and. nd. ys. ev. , J.

13 Nov 2006: 1 and 22.Figure 3 shows that K of nD, which has sp3 content and Ejust marginally higher than ta-C, is significantly bigger thanthat of ta-C. ... If the sp3 phase orders, evenin small grains such as in nD, a strong K increase occurs fora given density,

3 Feb 2014: Other activationodes are possible, but only under different electrode lay-ups,. nd are excluded from study here.During activation, independent electric fields give rise to. ... nd substituting for the terms A, B and C with Eqs.

22 Jan 2007: of a Nd: yttrium aluminum garnetYAG! laser. Clusterfluxes have been characterized with a quartz microbalaand with a Faraday cup placed in the deposition chamafter the first skimmersee Fig. ... of a Nd:YAG laser. 5794 J. Appl. Phys., Vol. 82, No.

18 Oct 2012: Tang, “Mode locking of ceramic Nd:YAG withgraphene as a saturable absorber,” Appl. ... 0.6. 0.8. 1.0. Inte. nsity. (a.u. ). Wavelength (nm). (b)(a) Data Fit.

12 Dec 2006: t. an. d-. nd. iond-entopy. pythe. of. nout. er-stic. edbyeVthede-. ,d se-nts,. ... Y. oat. L. ech-. ltz,. 2,. s-. ys. nd. Dia-. I.

4 Dec 2006: s-. ,. sra-. -n. -. h. nd. e. er-. f-. ... inat. not. ec.d-he. er. eneasnd,b-. aree-. cangyect,ybe-. edich. ofbesof. ld,ionme-nd. tesrmi.

6 Dec 2006: p. e. i-. -. lent. er-non. mice.nd-y. thes–. The background radiation clearly falls if nitrogen is intrduced into the chamber. ... M. lat. on. al-. ge. -E. a-. nd. G. ls-. B.