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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

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 24 2 48abAp −ξπ ξ>1.3 ⎟⎠⎞⎜⎝⎛++ 42 4 2 243 2 16ξξπAap polarization losses γ1 22 1 2 πξ/Ap ()1 2 2 2 21 2 +⎟⎠⎞⎜⎝⎛−ξππAp ... to within terms of order 4lδ and )(0 2 cclδδδ− we obtain 2 2 2 2 424 2 2⎟⎠⎞⎜⎝⎛−+⎟⎠⎞⎜⎝⎛−Ψ=Γπδππδclsin. (19) The substitution of (4, 10, 12) into (19), and the subsequent ... about 2. 1 and 2. 3 Å, respectively; on the other hand, the Bi-O distances for α-Bi 2 O3 were 2. 2 and 2. 4 Å, respectively. The Bi-O distance of 2. 1 Å in BiSG is in good agreement with the previously...
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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

... 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 wave by a slit in figure 2- 1 (c). ... Hanning window after zero-padding to improve the resolution in the spectral domain. The initial phase of each line can be extracted at the peak of the amplitude in the spectral domain. The phase...
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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

... 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 the in- line optics. In the in- line type ... composition. Advances in Solid-State Lasers: Development and Applications 148 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 6 pot

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. The following physical parameters of the laser ... 22 4 inside the amplifier, both the thickness of the pumped region and the Rayleigh range of the focused beam should be taken into account. In particular the pumped region length along the...
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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

... (a) (b)(c)(d)P2P1P2P1P2P1P2P1r 21 =0.08r 21 =0.01r 21 =0.0004r 21 =0.001 -2. 5 2. 5-0 .25 0 .25 zx -2. 5 2. 5-0 .25 0 .25 zx5E -2 -5E -2 5E -2 -5E -2 5E -2 -5E -2 5E -2 -5E -2 5E-4-5E-45E-4-5E-45E-4-5E-45E-4-5E-4 ... The width of the Gaussian function expressed in frequency is Advances in Solid-State Lasers: Development and Applications 376 z -2. 5 2. 5 -2. 5 2. 5 -2. 5 2. 5 -2. 5 2. 5 -2. 5 2. 5 -2. 5 2. 5 -2. 5 ... accommodate the entire bandwidth of the input pulse. The “mask bandwidth” depends upon the width of the mask L, the focal length of the lens f, the line spacing of the grating p and the angle...
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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

... 1964): 2 22 32 1 /2 2.405 1 22 2(1)vavαλπ+⎛⎞=⎜⎟−⎝⎠ (29 ) 2 2 1 2. 4051 22 waveguideaπλβλπ⎡⎤⎛⎞=−⎢⎥⎜⎟⎝⎠⎢⎥⎣⎦ (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 decreasing the peak power of the input ... coatings in normal incidence. Therefore, the gratings have to be operated in grazing incidence. The compensation in this case is harder, due to the intrinsic difficulties arising from grazing-incidence...
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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

... (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 (,,, , )fffff= (0.0 625 , 0 .25 , 0.375, 0 .25 ,0.0 625 ), and the common ... numbers by replacing al by (Kulander et al., 19 92) , Advances in Solid-State Lasers: Development and Applications 4 52 • As in the case of the cos pulse, the emission from the short (long) ... ⎤⎣⎦ (6) and we also obtain, for the kinetic energy Ekin, () 2 () =2 sin sin .kin p iEUθθθ− (7) One obtains the time (phase) of recombination tr (θr) as the roots of the equation...
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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

... 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 phenomena and the control of them is ever increasing. ... propagate in time in the presence of the applied laser field. The final step is to carry out a numerical integration using the Crank-Nicholson scheme in order to solve equation 4 () 22 2 22 static...
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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

... 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 ... ozonaγβωθωγββ−=−−⋅+−. (9) Relativistic Nonlinear Thomson Scattering: Toward Intense Attosecond Pulse 529 (1) 2 ˆFECzξε=⎡⎤⎣⎦. (50) 42 2 22 22 4 (2) 3 3ˆˆ(1 ) 42 2SFE SxES xρρ ρεβξβ εξβ⎧⎫⎡⎤⎡⎤⎪⎪=−− ... ×1019W/cm 2 . Advances in Solid-State Lasers: Development and Applications 528 The average photon energy can be approximated to the mean photon energy and then it can be estimated from the inverse...
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Tài liệu Speaking and Writing Strategies for the TOEFL iBT part 7 docx

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 Essay Rating Guide ... that the internet has changed my life the most. First, I am from China. I am now working in the US. That means my family and friends back in Beijing are very far away. Yet by using internet,...
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