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Advances in Solid-State Lasers: Development and Applications 1 doc

Advances in Solid-State Lasers: Development and Applicationsduration and in the end limits Part 2 docx

Advances in Solid-State Lasers: Development and Applicationsduration and in the end limits Part 2 docx

... Sample 1 2 3 4 5 Peak [eV] 16 6.0 (16 0.6) 16 4.9 (15 9.5) FWHM [eV] 1. 7 1. 7 A4 Height 10 0.0 64.6 Peak [eV] 16 6.2 (16 0.8) 16 5 .1( 159.8) FWHM [eV] 1. 9 1. 9 A5 Height 50.6 10 0.0 Peak [eV] 16 5.9 (16 0.6) ... 16 5.9 (16 0.6) 16 4.6 (15 9.3) 16 3.8 (15 8.5) FWHM [eV] 1. 8 1. 4 1. 4 NaBiO3 Height 38.6 35.0 10 0.0 Peak [eV] 16 4.7 (15 9.4) 16 3.7 (15 8.4) FWHM [eV] 1. 4 1. 4 α-Bi2O3 Height 19 .9 10 0.0 Peak [eV] 16 4.6 (15 9.3) ... 3.89E-03 1. 11 2.32 4.06E-03 1. 65 A3 2.05 2.08 3.89E-03 1. 33 2. 31 4.06E-03 2.50 A4 1. 81 2 .11 3.89E-03 1. 05 2. 31 4.06E-03 2.84 A5 1. 86 2 .13 3.89E-03 0.99 2.33 4.06E-03 3.04 Table 4. FEFF fitting...
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Advances in Solid-State Lasers: Development and Applicationsduration and in the end limits Part 4 doc

Advances in Solid-State Lasers: Development and Applicationsduration and in the end limits Part 4 doc

... [kW] 10 00 1 1.725 1. 725 14 6 11 .8 400 1 1.725 4. 31 1 01 42.7 200 1 1.5 41 7.7 70 11 0 13 3 1 1.38 10 .35 46.8 2 21 10 0 .1 0 .10 5 10 .5 22 447 Table 2. Results of Q-switching experiments; frep – pulse ... within 0.2 km in this condition. The Y(L) of the in- line type lidar Advances in Solid-State Lasers: Development and Applications 11 8 Koechner, W. (19 96). Solid-State Laser Engineering. Springer ... composition. Advances in Solid-State Lasers: Development and Applications 14 8 particle and an ice-crystal are illustrated in Fig. 3-3. In the scattering, the backscattering echoes keep the incident...
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Advances in Solid-State Lasers: Development and Applicationsduration and in the end limits Part 5 docx

Advances in Solid-State Lasers: Development and Applicationsduration and in the end limits Part 5 docx

... and the wide spectral bandwidth, which allows precision Advances in Solid-State Lasers: Development and Applications 16 6 Neuber, P. Rairoux, and U. Wandinger eds.(Springer-Verlag, Berlin, ... Research, Vol. 94, No. D 11, 13 , 313 13 , 318 , 19 89 E. Franzblau and C. J. Popp, “Nitrogen oxides produced from lightning”, J. Geophys. Res., Vol.94, No.D8, pp .11 .089 -11 .10 4, 19 89 E. Franzblau, “Electrical ... Advances in Solid-State Lasers: Development and Applications 17 2 the spectral bandwidth of more than 10 0 nm in wavelength (There are approximately 10 5 or more longitudinal modes.) and...
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Advances in Solid-State Lasers: Development and Applicationsduration and in the end limits Part 6 pot

Advances in Solid-State Lasers: Development and Applicationsduration and in the end limits Part 6 pot

... depleting the population inversion in the gain media. Since the ASE generated in the one Advances in Solid-State Lasers: Development and Applications 218 (10 ) (11 ) We may now use the ... Heidelberg Advances in Solid-State Lasers: Development and Applications 228 The amplification stage setup is shown in detail in Fig. 11 . The seed emerging from the pulse picker is injected into ... Laser cleaning of optical windows in internal combustion engines, Opt. Eng. vol.46, no .10 , pp .10 43 01- 1 to 8, Oct. Micro -Solid-State Laser for Ignition of Automobile Engines 2 01 pump duration...
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Advances in Solid-State Lasers: Development and Applicationsduration and in the end limits Part 10 pdf

Advances in Solid-State Lasers: Development and Applicationsduration and in the end limits Part 10 pdf

... modulation in chirped-pulse amplification”, Opt.Lett, Vol. 19 , pp. 214 9- 215 1 (19 94) Advances in Solid-State Lasers: Development and Applications 374 12 . The ouput pulse is estimated by multiplying ... ()()()0tanddxfλθλ θλ=⎡− ⎤⎣⎦ (17 ) Expanding x as a power series in angular frequency ω gives Advances in Solid-State Lasers: Development and Applications 368 L being the interaction length along ... systems”, Opt.Lett. Vol.20, pp. 11 63 -11 65 (19 95) Martinez O.E., (19 86), “Grating and prism compressors in the case of finite beam size”, J.Opt.Soc.Am.B vol.3, pp.929-934 (19 86) Monmayrant A., Chatel...
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Advances in Solid-State Lasers: Development and Applicationsduration and in the end limits Part 11 pptx

Advances in Solid-State Lasers: Development and Applicationsduration and in the end limits Part 11 pptx

... condition (T=273 .15 K, p=1atm), we have (Dalgarno & Kingston, 19 60): 511 172324024 6 800 0 05 .15 10 4 .19 10 4.09 10 4.32 10 1 5.547 10 1nλλλλ−⎛⎞×× × ×−= × + + + +⎜⎟⎝⎠ (34) In the above ... filaments, single beam equilibria, and radiation. Phys. Rev. Lett., Vol. 77, No. 7, (Aug. 19 96) page numbers (12 82 -12 85), ISSN: 00 31- 9007 Advances in Solid-State Lasers: Development and Applications ... 10 , the term "input arm" refers to the two collimators and indicates the distance between the source and the vertex of mirror M1 and Advances in Solid-State Lasers: Development and...
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Advances in Solid-State Lasers: Development and Applicationsduration and in the end limits Part 12 pptx

Advances in Solid-State Lasers: Development and Applicationsduration and in the end limits Part 12 pptx

... fundamental intensity. The results are shown in Fig. 15 for the cases of IH27 = 10 13 W/cm2 and IF = 5 × 10 13 , 8 × 10 13 , 3 × 10 14 , 5 × 10 14 , 10 15 W/cm2. The curve for IF = 5 × 10 13 W/cm2 ... to a 35 fs Gaussian combined driving and XUV pulse (ωX = 17 .05eV), the former (λ = 16 00 nm) with a peak intensity of 1. 6 × 10 14 W/cm2 and the latter 2.3 × 10 11 W/cm2. Lower curve: ... and detected by microchannel plate with CCD camera. Advances in Solid-State Lasers: Development and Applications 462 induce direct ionization, the obtained pulses are mainly due to H11...
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Advances in Solid-State Lasers: Development and Applicationsduration and in the end limits Part 13 pptx

Advances in Solid-State Lasers: Development and Applicationsduration and in the end limits Part 13 pptx

... (February 19 99) 14 22 - 14 25, ISSN 10 79- 711 4 (online), 00 31- 9007 (print) 22 Relativistic Nonlinear Thomson Scattering: Toward Intense Attosecond Pulse Kitae Lee 1 , Sang-Young Chung2, and Dong-Eon ... K. C. (19 93). Above threshold ionization beyond the high harmonic cutoff. Physical Review Letters, 70, 11 , (March 19 93) 15 99 - 16 02, ISSN 10 79- 711 4 (online), 00 31- 9007 (print) Stebbings, S.L.; ... harmonic-generation in laser-produced ions using a near-infrared laser Phys Rev A 51, 585-5 91. Advances in Solid-State Lasers: Development and Applications 500 Fig. 9. Theoretical intensity...
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Advances in Solid-State Lasers: Development and Applicationsduration and in the end limits Part 14 pdf

Advances in Solid-State Lasers: Development and Applicationsduration and in the end limits Part 14 pdf

... considered from a single charge state; Ne8+ at 2 10 17 W/cm2, Ar 10 + at 2 × 10 18 W/cm2, Ar 16 + at 1. 2 × 10 19 W/cm2, Na 10 + at 5 × 10 19 W/cm2, and Na 11 + at 1. 2 × 10 20 W/cm2. ... adequate as an interaction geometry. Advances in Solid-State Lasers: Development and Applications 512 of intense laser pulse with solids (Linde et al., 19 95, 19 96, 19 99; Norreys et al., 19 96; Lichters ... obtained in numerical simulations. Advances in Solid-State Lasers: Development and Applications 524 fields having linear polarization in the x-direction (zeroth-order) and propagating in...
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Advances in Solid-State Lasers: Development and Applications_1 doc

Advances in Solid-State Lasers: Development and Applications_1 doc

... Sample 1 2 3 4 5 Peak [eV] 16 6.0 (16 0.6) 16 4.9 (15 9.5) FWHM [eV] 1. 7 1. 7 A4 Height 10 0.0 64.6 Peak [eV] 16 6.2 (16 0.8) 16 5 .1( 159.8) FWHM [eV] 1. 9 1. 9 A5 Height 50.6 10 0.0 Peak [eV] 16 5.9 (16 0.6) ... 16 5.9 (16 0.6) 16 4.6 (15 9.3) 16 3.8 (15 8.5) FWHM [eV] 1. 8 1. 4 1. 4 NaBiO3 Height 38.6 35.0 10 0.0 Peak [eV] 16 4.7 (15 9.4) 16 3.7 (15 8.4) FWHM [eV] 1. 4 1. 4 α-Bi2O3 Height 19 .9 10 0.0 Peak [eV] 16 4.6 (15 9.3) ... (FWHM) were recognized as 11 82 and 300 nm at 500-nm excitation, 11 44 and 19 2 nm at 700 nm, 12 65 and 336 nm at 800 nm, and 11 30 and 18 8 nm at 10 00 nm. A similarity of the luminescent spectra can...
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