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
... degree is 1/γ) 2 1 2 π /Ap ( ) 22 2 4 2 4 8 ab A p − ξ π ξ>1.3 ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ ++ 42 4 2 2 4 3 2 1 6 ξξ π Aa p polarization losses γ 1 22 1 2 πξ /Ap ( ) 1 2 2 2 2 1 2 + ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ − ξ π π Ap ... to within terms of order 4 l δ and )( 0 2 ccl δδδ − we obtain 2 2 2 2 424 2 2 ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ −+ ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ −Ψ=Γ π δ π π δ cl sin . (19) The substitution...
Ngày tải lên: 21/06/2014, 10:20
Advances in Solid-State Lasers: Development and Applicationsduration and in the end limits Part 5 docx
... km, the combined Advances in Solid-State Lasers: Development and Applications 190 standard uncertainty is estimated only as 6.4 nm according to the table 3-4. The other is for positioning ... adjusting the beam size of a pumping laser to have more gain in the only high intensity area as shown in figure 2- 1 (b). The other is removal of the continuous wav...
Ngày tải lên: 21/06/2014, 10:20
Advances in Solid-State Lasers: Development and Applicationsduration and in the end limits Part 4 doc
... within 0 .2 km in this condition. The Y(L) of the in- line type lidar Advances in Solid-State Lasers: Development and Applications 118 Koechner, W. (1996). Solid-State Laser Engineering. Springer ... prevent the light directly reflected from the in- line optics from entering the detectors. Its aperture was determined in combination with the tilts of t...
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Advances in Solid-State Lasers: Development and Applicationsduration and in the end limits Part 6 pot
... with the amplifying beam in depleting the population inversion in the gain media. Since the ASE generated in the one Advances in Solid-State Lasers: Development and Applications 21 8 ... micro-laser and (b) a spark plug in a stoichiometric mixture. Advances in Solid-State Lasers: Development and Applications 22 6 in Section 2. 1....
Ngày tải lên: 21/06/2014, 10:20
Advances in Solid-State Lasers: Development and Applicationsduration and in the end limits Part 10 pdf
... (a) (b) (c) (d) P2 P1 P2 P1 P2 P1 P2 P1 r 21 =0.08 r 21 =0.01 r 21 =0.0004 r 21 =0.001 -2. 5 2. 5 -0 .25 0 .25 z x -2. 5 2. 5 -0 .25 0 .25 z x 5E -2 -5E -2 5E -2 -5E -2 5E -2 -5E -2 5E -2 -5E -2 5E-4 -5E-4 5E-4 -5E-4 5E-4 -5E-4 5E-4 -5E-4 ... The width of the Gaussian function expressed in frequency is Advances in Solid-State Lasers: Development an...
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Advances in Solid-State Lasers: Development and Applicationsduration and in the end limits Part 11 pptx
... 1964): 2 22 32 1 /2 2.405 1 22 2(1) v av αλ π + ⎛⎞ = ⎜⎟ − ⎝⎠ (29 ) 2 2 1 2. 405 1 22 waveguide a πλ β λπ ⎡ ⎤ ⎛⎞ =− ⎢ ⎥ ⎜⎟ ⎝⎠ ⎢ ⎥ ⎣ ⎦ (30) where v is the refractive index ratio between the material ... fact, in the linear gradient shape case, a moderately increasing the length of the tube (corresponding to decreasing the slope of the linear line) or decreasi...
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Advances in Solid-State Lasers: Development and Applicationsduration and in the end limits Part 12 pptx
... (51) containing ca. 5 pulses, composed of the 15th to 23 rd harmonics. The harmonic mixing ratio is 22 222 15 17 19 21 23 (,,, , ) f ffff= (0.0 625 , 0 .25 , 0.375, 0 .25 ,0.0 625 ), and the common ... numbers by replacing a l by (Kulander et al., 19 92) , Advances in Solid-State Lasers: Development and Applications 4 52 • As in the case of the cos pu...
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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 Applications 5 02 dependent ionisation within the capillary waveguide. However further developments including the incorporation of pressure dependence ... al., 20 07), electron transport in condensed matter (Cavalieri et al., 20 07). The demand on and the emphasis to the understanding of the ultrafast phenomen...
Ngày tải lên: 21/06/2014, 10:20
Advances in Solid-State Lasers: Development and Applicationsduration and in the end limits Part 14 pdf
... 524 fields having linear polarization in the x-direction (zeroth-order) and propagating in the +z direction (Davis, 1979; Salamin, 20 07), (28 ) (29 ) (30) (31) ( 32) (33) The laser ... o zo na γβ ω θ ω γβ β − = − −⋅+ − . (9) Relativistic Nonlinear Thomson Scattering: Toward Intense Attosecond Pulse 529 (1) 2 ˆ FECz ξε = ⎡ ⎤ ⎣ ⎦ . (50) 42...
Ngày tải lên: 21/06/2014, 10:20
Tài liệu Speaking and Writing Strategies for the TOEFL iBT part 7 docx
... First, I from China. I now working in US. That mean my family and friend back in Beijing is very far away. Yet by using internet, I can talk to them as much as I want using email and IM. Best ... Step #6 Independent Essay - 57 TASK: Check this essay for coherence using the Independent Essay Proficiency Checklist on page 310, then rate it using the Independent Ess...
Ngày tải lên: 24/12/2013, 09:17