Recent Optical and Photonic Technologies Part 2 ppt

... 20 07; Baba & Mori, 20 07; Baba, 20 08) and quantum optics (Yoshie et al., 20 04; Lodahl et al., 20 04; Englund et al., 20 05). Recent Optical and Photonic Technologies 28 Fleischer, J. W., ... Recent Optical and Photonic Technologies 30 Stefanou, N. & Modinos, A. (1998). “Impurity bands in photonic insulators,” Phys. Rev. B 57, 121 27- 121 33...

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... 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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... N c = 1, and γ c 2 = 0 in relationship (5.6) and find (Fig. 2, curve 2) Recent Optical and Photonic Technologies 322 n eff spher A/A= nano bulk n+ε -x(ε -1) cr ⎡ ⎤ ⎢ ⎥ ⎣ ⎦ 2 3 2 . (3.10) ... No.11, (22 09 -22 12) , ISSN 1063-7834; [ (20 03). Radiative transitions and spectral hole- burning in MgO: Cr 3+ nanocrystals. Fiz. Tverd. Tela, Vol.45, No.11, (21 04...

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... al., 20 07a). The correlation matrix results: The Photonic Torque Microscope: Measuring Non-conservative Force-fields 421 () () () () () () () () () ( ) () () || 2 2 2 22 22 || 2 2 2 22 22 || 2 || 1|| 1|| || t xx t yy t xy t yx e rt ... ) () 2 , ||St Ct S t φ α φφ φ ⎧ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎪ ⎡⎤ ΩΔ ⎪ −Δ+ Δ+ Δ ⎢⎥ ⎪ ⎣⎦ ⎩ (13) where () 2 2 22 2 φ α φ φ = +Ω−Δ (14...

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... 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 ... Technologies Recent Optical and Photonic Technologies 2 Vlasov et al., 20 05), optical memories (Scheuer et al., 20 05), and to enhanced nonlinear int...

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... 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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... 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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... Beams of Dielectrics and Semiconductors. Journal of Optical Society of America B, Vol. 7, No. 10, (October 1990) pp. 20 06 20 15, ISSN 0740- 322 4 Recent Optical and Photonic Technologies 168 ... Phys. Rev. B 43(4): 3 626 –3636. Wild, W. J. & Giles, C. L. (19 82) . Goos-Hänchen shifts from absorbing media, Phys. Rev. A 25 (4): 20 99 21 01. Recent Optical an...

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... Letters, 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 24 6 ( ) 3 33 1 RWWSS ... , and the square rooted intensity is calculated as, Recent Optical and Photonic Technologies 24 2 The inclined reader finds a detailed discussi...

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... 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 ... Mlynek, J. & Sandoghdar, V. (20 01). A single gold particle as a probe for apertureless scanning near-field optical microscopy. J. Microsc., 20 2, (APR 20 01), ( 72- 76...

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