Recent Optical and Photonic Technologies 2012 Part 2 pot

Recent Optical and Photonic Technologies 2012 Part 2 pot

Recent Optical and Photonic Technologies 2012 Part 2 pot

... R. A., and Miguez, H. (20 07). “Effect of extinction on the high-energy optical response of photonic crystals ,” Phys. Rev. B. 75, 24 1101. Recent Optical and Photonic Technologies 22 one ... 1999; Ryu et al., 20 02; Akahane et al., 20 03; Zhang & Qiu, 20 04; Nozaki & Baba, 20 06; Akahane et al., 20 05; Song et al., 20 05; Asano et al., 20 06; Tanaka et...
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Recent Optical and Photonic Technologies 2012 Part 5 potx

Recent Optical and Photonic Technologies 2012 Part 5 potx

... geometric relation of A, B and C, A 2 C 2 =B 2 C 2 =A 2 B 2 , as shown in Fig.11(c). () () ()() ⎟ ⎟ ⎟ ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎜ ⎜ ⎜ ⎝ ⎛ +−− ++− = 2 21 2 21 2 2 2 21 4 / 16 arccos2 kkkk n kk THzTHz λ π α ... x-axis and B for y-axis are represented by following equations, () () 12 12 24 , cos sin 22 AB kk kk ππ α α == −+ (3) where k 1 =2 n 1 /λ 1 and k 2 =2 n 2...
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Recent Optical and Photonic Technologies 2012 Part 9 potx

Recent Optical and Photonic Technologies 2012 Part 9 potx

... Vol. 2 20 02, 983-987 Böttcher, C. J. (19 42) . Zur Theorie der inneren elektrischen Feldstärke. Physica, Vol. 9, No. 10, 19 42, 937-943 Recent Optical and Photonic Technologies 25 4 1 22 2 2 12 2 tan 1tan ab rr θ θ − ⎛⎞ + == ⎜⎟ + ⎝⎠ . ... 3. Recent Optical and Photonic Technologies 25 2 2. Local field polarization vector detection on nanoscale 2....
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Recent Optical and Photonic Technologies 2012 Part 1 ppt

Recent Optical and Photonic Technologies 2012 Part 1 ppt

... amplitude and phase 22 2 00 22 0 () 1 /2 2 1 = 1 cos 1 cos2 ( ) 21 2 dx kxx dx k c c L φωωε π εγφ γ ⎡ ⎤ Δ ⎛⎞⎛ ⎞ −+ + + ⎢ ⎥ ⎜⎟⎜ ⎟ + ⎝⎠⎝ ⎠ ⎣ ⎦ (25 ) 2 2 0 log ( ) 1 /2 2 =1cossin2(). 21 dAx xx dx ... that Recent Optical and Photonic Technologies 2 Vlasov et al., 20 05), optical memories (Scheuer et al., 20 05), and to enhanced nonlinear interactions...
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Recent Optical and Photonic Technologies 2012 Part 3 pptx

Recent Optical and Photonic Technologies 2012 Part 3 pptx

... intensity distribution I in 3D space: 22 2 123 12 21 2 13 3 1 2 23 3 2 111 ()cos[(2sin)( )] 22 2 ()cos[(2sin())(sin)( )] 2 ( )cos[ (2 sin ( )) ( sin ) ( )] 2 IE E EEE k x EE k z k x EE k z k x θ δδ θ θδδ θ θδδ =+++ ... 18( 12) : 23 29 23 30. Song, B S., Asano, T. &Noda, S. (20 07). Heterostructures in two-dimensional photonic- crystal slabs and their application to...
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Recent Optical and Photonic Technologies 2012 Part 4 pdf

Recent Optical and Photonic Technologies 2012 Part 4 pdf

... g Ue π = can be manipulated. Moreover, if 1 / 2( 1 ,2, 3,4) i i α == , we have out 1 2 1 2 (1 / 2 )( )rg Ψ =−++ [where 22 2 12( ) g r−= − and 22 2 12( ) g r+= + ], which is the generation of the ... Real (a) and imaginary (b) parts of the reflection coefficients for initial QD states, 12 rr , 12 rg , 12 g r , and 12 g g . Here we assume 12 () () 2gr gr = =Γ ...
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Recent Optical and Photonic Technologies 2012 Part 6 doc

Recent Optical and Photonic Technologies 2012 Part 6 doc

... 1977). In fact Recent Optical and Photonic Technologies 146 12 21 0 =0, 001 i i μμ μμ ⎛⎞ ⎜⎟ − ⎜⎟ ⎜⎟ ⎝⎠ μ (8) where 2 10 =1 ( ), AS B MY Y μμγ +− ++ (9) 2 20 =(), AS B MY Y μμγ +− − ... k 2y is real in the bulk regions and imaginary in the reststrahl regions. First we consider power flow for k 2y real (i.e. in the bulk regions). Equations 27 and 28 the...
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Recent Optical and Photonic Technologies 2012 Part 10 doc

Recent Optical and Photonic Technologies 2012 Part 10 doc

... 1999), ( ) ( ) ()( ) ()( ) ( ) () 22 0 12 22 1 120 21 2 120 3 121 20 0,0 90,0 , 0,0 90,0 cos2 cos2 , 45 ,0 135 ,0 cos cos 2 sin 2 , 45 , 135 , sin sin 2 . 22 sI I a a sI I a a s sI I aa s sI I aa ... Nano-Optics, Cambridge University Press, ISBN- 13: 9780 521 8 322 43 ; ISBN-10: 0 521 8 322 41, New York Recent Optical and Photonic Technologies 28 2 microlithog...
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Recent Optical and Photonic Technologies 2012 Part 14 pdf

Recent Optical and Photonic Technologies 2012 Part 14 pdf

... () 22 10 12 =1 , 22 2 dq h qq q q dt βω ⎛⎞ −++ +Ω− ⎜⎟ ⎝⎠ () 22 20 21 =1 , 22 2 dq h qq q q dt βω ⎛⎞ −++ −Ω+ ⎜⎟ ⎝⎠ ( 12) where the dimensionless amplitudes are defined by q 1 = q cos ψ and ... Electronics, vol. 12, no. 6, 1636-1641. Boyraz O. & Jalali, B. (20 04). Demonstration of a silicon Raman laser. Optics Express, vol. 12, no. 21 , 526 9- 527 3. Recent Opt...
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Recent Optical and Photonic Technologies 2012 Part 15 pptx

Recent Optical and Photonic Technologies 2012 Part 15 pptx

... yx Dtrtrt θθ Δ =Δ−Δ, and the sum of the ACFs, ( ) ( ) ( ) ACF xx yy Strtrt θθ Δ =Δ+Δ, are invariant with respect to θ : () () || 2 t CCF e DtD St φ φφ −Δ Ω Δ =Δ (19) and () () () || 2 2 2 2 22 22 2 2||. t ACF e StD ... CtSt φ φ θ αθθ φφ φ −Δ ⎛⎞ ΔΩ Δ= Δ+Δ − ⎜⎟ ⎝⎠ (21 ) and () () ( ) () () () || 2 2 2 ,2 ||sin2cos2. t ACF e Dt D CtSt φ φ θ αθθ φφ φ −Δ ⎛⎞ ΔΩ Δ=−...
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