Wave Propagation 2011 Part 3 pdf

... Motivated by simulating the propagation of a variety of waves, such as sound waves, light waves and water waves, we discuss a novel numerical scheme to solve the wave equation with time dependent ... Constant and Time-Dependent Wave Equations. 73 holds with numbers K ≥ 0 and ω ∈ R, cf. [6]. The estimations (37 ) and (38 ) result in EO 2 1 =(), inin KB eττ ∞− +    (39...

Ngày tải lên: 21/06/2014, 23:20

... () 66 32 2 1 2 2 21 E mm mc m aJaJa aa ξξ ξ + − ⎡ ⎤ =− ⎢ ⎥ ⎣ ⎦ , () () () () 2 36 6 66 13 1 3 3 13 3 13 3 13 3 2 22 1 EE EE m m cc aJaikcecmmJa aa ξ ξ ημ ξ ξ + ⎡⎤ =++−+− ⎢⎥ ⎣⎦ , () () () 23 3 44 3 ... () 66 32 2 1 2 2 21 E mm mc m aIaIa aa ξξ ξ + − ⎡ ⎤ =− + ⎢ ⎥ ⎣ ⎦ , () () () () 2 36 6 66 13 13 3 13 3 13 3 13 3 2 2 2 1 E E EE m m c c aIaikcecmmIa aa ξ ξημξ ξ + ⎡⎤ =− +...

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... imaging chips range from sub-retinal implant imagers [33 ] to glare detection [34 ] to fluorescence imaging [35 , 36 ] and x-ray imaging [37 ], to name a few. A study of three common photodiode ... 17(5&6),(20 03) 225- 233 Pittman T.B., Jacobs, B.C., & Franson, J.D., (2002). Single photon on pseudodemand from stored parametric down-conversion, Phys. Rev. A 66 (2002)04 230 3 Ph...

Ngày tải lên: 19/06/2014, 21:20

... ≥ 0} satisfies (3. 18) where Rxxx ∈∀= Δ + ),0,max( , then we must have (3. 19) Proof: See [XG00, Lemma 3. 3]. 3. 3 .3 Proof of Theorem 3. 1 Proof of Theorem 3. 1: We divide the proof ... Eqs. (3. 5)— (3. 13) can asymptotically stabilize the corresponding noise-free system, i.e. (3. 16) 3. 3.2 Preliminary Lemmas To prove Theorem 3. 1, we need the following Le...

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... Issue 3, pp. 101-1 03, ISSN: 00 036 951. Basore, P. A. (1990). Numerical modeling of textured silicon solar cells using PC-1D, IEEE Transaction on Electron Devices, Vol. 37 , No. 2, pp. 33 7 -34 3, ISSN: ... coefficients of GaAs (InAs) at 1. 531 , 1.589, and 1.621 eV are 1.41 × 10 -3 (6.95 × 10 -3 ), 1.77 × 10 -3 (7.69 × 10 -3 ), and 1.96 × 10 -3 (8.09 × 10 -3 ) nm -1 , res...

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... expression which is valid for any values of d ε and p ε : 1cos 12,12,1, 2 1 1cos 32 ,32 ,2, 2 1 cos 1 cos 1 32 ,32 ,2, 1 32 ,32 ,2, 22 1cos 1cos 1 12,12,1, 1 12,12,1, 22 d cr pp p dd pp dd F F FF FF γ ε γ ω εε γγ ω εε εε γγ εε ⎧ − ⎛⎞ ⎜⎟ ⎪ ⎝⎠ ⎪ +× − ⎛⎞ ⎪ ⎜⎟ ⎪ ⎝⎠ = ⎨ ⎛⎞ ... (56) 226 Wave Propagation 18 Electromagnetic Wa ves The above is an equation for the second moment of the wave...

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... applications, 36 ~40(1990). [30 ] Li Fang, Liu Yingetc. [J]. Metaltlc Functional Materlals. 11 (3) ( 2004). [31 ] S.Sugimoto,T.Kagotani etc. [J] Journal of Alloys and Compounds 33 0 33 2, 30 1 (2002). [32 ] ... Shengji, Tu Ming-jing. [J].Journal of theChinese Rare Earth Socity. 23( 3) :30 3(2005). Wave Propagation 35 6 II. Microwave Electromagnetic Properties of Nd 2 Fe 1...

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... 4 - 4 - 2 0 2 4 ε r μ r 90 0 |α| / degree Z c = Z 0 - 0.6 - 0 .3 0 0 .3 0.6 - 0.6 - 0 .3 0 0 .3 0.6 10 5 0 ε r μ r L + L - - 0.6 - 0 .3 0 0 .3 0.6 - 0.6 - 0 .3 0 0 .3 0.6 ε r μ r 90 0 |α| / degree Z c = Z 0 (a) (b) (c) α ... corresponds to LCP (RCP) waves. Section 4 .3 and Eqs. (30 ) and (35 )- (38 ) show that the incident CP wave is not converted into the other CP wave on...

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... in the following based on Eq. (33 ). 3. 3 Method for forward scattering analysis Let us rewrite Eq. (33 ) in the following form: (34 ) where is given by (35 ) which can be treated as a given ... Guo 13. Differential Quadrature Method for Linear Long Wave Propagation in Open Channels 2 53 Birol Kaya and Yalcin Arisoy 14. A Parabolic Equation for Wave...

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... characterised by r 4 j 0. 23 = − , r 1μ= and 0 d0.15 = λ . Wave Propagation in Materials for Modern Applications 32 Hörmander, L. (19 83) , The analysis of linear partial differential operators ... dcos 12 23 11 j2k dcos 12 23 RRe RR 1R R e θ θ + == +    22 22 j2k d cos 12 23 22 j2k d cos 12 23 RRe RR 1R R e θ ⊥⊥ ⊥ θ ⊥⊥ + == + (57) 12 21 RR0 = = (58) 22 22 jk dco...

Ngày tải lên: 21/06/2014, 23:20