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 NaBiO 3 Height 38.6 35.0 10 0.0 Peak [eV] 16 4.7 (15 9.4) 16 3.7 (15 8...

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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; f rep – 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...

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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...

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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 s...

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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 ... ( ) ( ) ( ) 0 tan dd xf λ θλ θλ = ⎡− ⎤ ⎣ ⎦ (17 ) Expanding x as a power series in angular frequency ω gives Advances in Solid-State Lasers: Developm...

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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 1723 24 0 24 6 8 00 0 0 5 .15 10 4 .19 10 4.09 10 4.32 10 1 5.547 10 1n λλλλ − ⎛⎞ ×× × × −= × + + + + ⎜⎟ ⎝⎠ (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 Sol...

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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 I H27 = 10 13 W/cm 2 and I F = 5 × 10 13 , 8 × 10 13 , 3 × 10 14 , 5 × 10 14 , 10 15 W/cm 2 . The curve for I F = 5 × 10 13 W/cm 2 ... to a 35 fs Gaussian combined driving and XUV pulse ( ω X = 17 .05eV), the former ( λ = 16 00 nm) with a peak intensity of 1. 6 × 10 14 W/cm 2...

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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 Chung 2 , 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),...

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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; Ne 8+ at 2 10 17 W/cm 2 , Ar 10 + at 2 × 10 18 W/cm 2 , Ar 16 + at 1. 2 × 10 19 W/cm 2 , Na 10 + at 5 × 10 19 W/cm 2 , and Na 11 + at 1. 2 × 10 20 W/cm 2 . ... adequate as an interaction geometry. Advances in Solid-State Lasers: Development and Applications 512 of intense laser pulse with solids (Linde et...

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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 NaBiO 3 Height 38.6 35.0 10 0.0 Peak [eV] 16 4.7 (15 9.4) 16 3.7 (15 8...

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