2-D Niblett-Bostick magnetotelluric inversion - MTNet
2-D Niblett-Bostick magnetotelluric inversion - MTNet 2-D Niblett-Bostick magnetotelluric inversion - MTNet
J. RODRÍGUEZ et al. Geologica Acta, 8(1), 15-30 (2010) DOI: 10.1344/105.000001513 2-D Niblett-Bostick 28 oriented in the i direction. On the other hand, the horizontal magnetic field satisfies the following differential equation (A.16 ) The solution of this equation for a homogeneous half- space is simply (A.17) Therefore, the horizontal electric field is given by (A.18) Since E for TM mode is (Ex,0,Ez) and for a homogeneous half-space Ez is zero, we only need g 11 to compute δEx. The expression for g 11 is given in Lee and Morrison (1980). (A.19) Combining equations (A14), (A15), (A18), and (A19), we find the Fréchet derivative for TM mode: (A.20) 2 Integral of Fréchet derivatives for TE and TM modes Here we find the integral of the Fréchet derivatives for a typical cell. For TE mode we integrate equation (A11) in the region xi≤x’≤xi+1, zj≤z’≤zj+1. That is (B.1) The result is (B.2) For TM mode we integrate equation (A20) in the same region, the result is (B.3) The integrals ITE and ITM as defined by Eqs. (B2) and (B3) are complex numbers. However, the real part of each one represents the corresponding integral of the Fréchet derivate of usau. The horizontal axis is divided into n elements, from x1 to xm, and the vertical distance is divided into m elements, from z1 to xm, then Eqs. (B2) and (B3) can be used to find the integral of the Fréchet derivative in the rectangular region defined by [xi, xi+1], and [zi, zi+1]. To take into account the whole half-space we have to consider (-∞, x1] and [xn, +∞) in the horizontal coordinate and [zm, +∞) in the vertical coordinate. The first case can be computed by noting that the corresponding sine transform for the argument x-b with b→±∞ is zero. The second case can be easily computed, considering that the corresponding exponential in equations (B2) or (B3) is null. In all cases, the actual computations are performed using the digital filters for sine and cosine transforms of Anderson (1975). Further details are available in the thesis of Esparza (1991). 3 Series and parallel impedances and their derivatives The series-parallel transformation The horizontal components of the electromagnetic field are linearly related through a second order impedance tensor (e.g., Swift, 1967). That is, (C.1) where Zxx, Zxy, Zyx and Zyy are complex numbers. Ex, Zy are the orthogonal components of the electric field and Hx, Hy are the corresponding magnetic field components. Following the work of Romo et al. (2005), we use an alternative representation defined by the following transformation (C.2) where (C.3) (C.4) (C.5) (C.6) If we consider a 2-D case in which the magnetotelluric responses are solely characterized by ZTM = Zxy and ZTE = 4 u + λ . | ) 0 , ( ) 0 , ( | | | 2 0 x E x H x y a ωµ σ = (A.13) ]. ) 0 , ( ) 0 , ( ) 0 , ( ) 0 , ( Re[ | | 2 | | x H x H x E x E y y x x a a δ δ σ σ δ − − = (A.14) '. ' ) ' , ' ( ) ' , ' ( ) , , ( ) , ( 13 12 11 dz dx z x z x g g g z x x δσ = ∫ E (A.15) . 1 0 2 ρ ρ σ ωµ ∇ × ∇ − = − ∇ y y y H H i H (A.16) . ) 0 ( ) , ( 2 z i y e H z x H − = (A.17) . 2 ) 0 ( ) , ( 2 z i x e i H z x E − = σδ (A.18) 4 . ) 2 ( ' ) 2 ( z i u TE e u i G + − λ + λ λ + + λ = (A.12) . | ) 0 , ( ) 0 , ( | | | 2 0 x E x H x y a ωµ σ = (A.13) ]. ) 0 , ( ) 0 , ( ) 0 , ( ) 0 , ( Re[ | | 2 | | x H x H x E x E y y x x a a δ δ σ σ δ − − = (A.14) '. ' ) ' , ' ( ) ' , ' ( ) , , ( ) , ( 13 12 11 dz dx z x z x g g g z x dE x δσ = ∫ E (A.15) . 1 0 2 ρ ρ σ ωµ ∇ × ∇ − = − ∇ y y y H H i H (A.16) . ) 0 ( ) , ( 2 z i y e H z x H − = (A.17) . 2 ) 0 ( ) , ( 2 z i x e i H z x E − = σδ (A.18) 5 11 g x E δ 11 g . )] ' ( cos[ ] [ 2 1 ) ' , ' ; , ( ) ' ( | ' | 0 2 11 λ − λ + πσδ − = + − − − ∞ ∫ d x x e e u z x z x g z z u z z u (A.19) ]. )] ' ( cos[ 2 Re[ ' ) 2 ( 0 2 λ − λ πδ = + − ∞ ∫ d x x ue G z i u TM (A.20) 1, 1 ' ' i i j j x x x z z z + + ≤ ≤ ≤ ≤ '. ' ) ' , ' , ( 2 1 1 dz dx z x x G I TE x x z z TE i i j j δ = ∫ ∫ + + (B.1) × − + λ + λ + λ + λ π = + − + − ∞ + ∫ ] [ ) 2 )( ( ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u TE e e i u u i I . )]] ( sin[ )] ( [sin[ 1 λ λ λ d x x x x i i − − − + (B.2) × − + λ π = + − + − ∞ + ∫ ] [ ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u TM e e i u u I . )]] ( sin[ )] ( [sin[ 1 λ − λ − − λ + d x x x x i i (B.3) TE I TM I | | a σ 1 x m x 1 z m z [ ] 1 , + i i x x [ ] 1 , + i i z z ] , ( 1 x −∞ ) , [ +∞ n x ) , [ +∞ m z , ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ = ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ y x yy yx xy xx y x H H Z Z Z Z E E (C.1) xx Z xy Z yx Z yy Z x E y E . )] ' ( cos[ ] [ 2 1 ) ' , ' ; , ) ' ( | ' | 0 2 λ − λ + πσδ − = + − − − ∞ ∫ d x x e e u z x z z z u z z u (A.19) ]. )] ' ( cos[ 2 Re[ ' ) 2 ( 0 2 λ − λ πδ = + − ∞ ∫ d x x ue G z i u TM (A.20) 1 ' j j z z + ≤ ≤ '. ' ) ' , ' , ( 2 1 1 dz dx z x x G I TE x x z z TE i i j j δ = ∫ ∫ + + (B.1) × − + λ + λ + λ + λ π + − + − ∞ + ∫ ] [ ) 2 )( ( ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u e e i u u i . )]] ( sin[ )] ( [sin[ 1 λ λ λ d x x x x i i − − − + (B.2) × − + λ π + − + − ∞ + ∫ ] [ ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u e e i u u . )]] ( sin[ )] ( [sin[ 1 λ − λ − − λ + d x x x x i i (B.3) , ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ = ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ y x yy yx xy xx y x H H Z Z Z Z E E (C.1) 11 g x E δ 11 g . )] ' ( cos[ ] [ 2 1 ) ' , ' ; , ( ) ' ( | ' | 0 2 11 λ − λ + πσδ − = + − − − ∞ ∫ d x x e e u z x z x g z z u z z u (A.19) ]. )] ' ( cos[ 2 Re[ ' ) 2 ( 0 2 λ − λ πδ = + − ∞ ∫ d x x ue G z i u TM (A.20) 1, 1 ' ' i i j j x x x z z z + + ≤ ≤ ≤ ≤ '. ' ) ' , ' , ( 2 1 1 dz dx z x x G I TE x x z z TE i i j j δ = ∫ ∫ + + (B.1) × − + λ + λ + λ + λ π = + − + − ∞ + ∫ ] [ ) 2 )( ( ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u TE e e i u u i I . )]] ( sin[ )] ( [sin[ 1 λ λ λ d x x x x i i − − − + (B.2) × − + λ π = + − + − ∞ + ∫ ] [ ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u TM e e i u u I . )]] ( sin[ )] ( [sin[ 1 λ − λ − − λ + d x x x x i i (B.3) TE I TM I | | a σ 1 x m x 1 z m z [ ] 1 , + i i x x [ ] 1 , + i i z z ] , ( 1 x −∞ ) , [ +∞ n x ) , [ +∞ m z , ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ = ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ y x yy yx xy xx y x H H Z Z Z Z E E (C.1) xx Z xy Z yx Z yy Z . )] ' ( cos[ ] [ 2 1 ) ' , ' ; , ( ) ' ( | ' | 0 2 11 λ − λ + πσδ − = + − − − ∞ ∫ d x x e e u z x z x g z z u z z u (A.19) ]. )] ' ( cos[ 2 Re[ ' ) 2 ( 0 2 λ − λ πδ = + − ∞ ∫ d x x ue G z i u TM (A.20) 1, 1 ' ' i j j x x z z z + + ≤ ≤ ≤ '. ' ) ' , ' , ( 2 1 1 dz dx z x x G I TE x x z z TE i i j j δ = ∫ ∫ + + (B.1) × − + λ + λ + λ + λ π = + − + − ∞ + ∫ ] [ ) 2 )( ( ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u TE e e i u u i I . )]] ( sin[ )] ( [sin[ 1 λ λ λ d x x x x i i − − − + (B.2) × − + λ π = + − + − ∞ + ∫ ] [ ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u TM e e i u u I . )]] ( sin[ )] ( [sin[ 1 λ − λ − − λ + d x x x x i i (B.3) | ] 1 + i ] 1 + i ] , 1 x ) ∞ ) +∞ 11 g x E δ 11 g . )] ' ( cos[ ] [ 2 1 ) ' , ' ; , ( ) ' ( | ' | 0 2 11 λ − λ + πσδ − = + − − − ∞ ∫ d x x e e u z x z x g z z u z z u (A.19) ]. )] ' ( cos[ 2 Re[ ' ) 2 ( 0 2 λ − λ πδ = + − ∞ ∫ d x x ue G z i u TM (A.20) 1, 1 ' ' i i j j x x x z z z + + ≤ ≤ ≤ ≤ '. ' ) ' , ' , ( 2 1 1 dz dx z x x G I TE x x z z TE i i j j δ = ∫ ∫ + + (B.1) × − + λ + λ + λ + λ π = + − + − ∞ + ∫ ] [ ) 2 )( ( ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u TE e e i u u i I . )]] ( sin[ )] ( [sin[ 1 λ λ λ d x x x x i i − − − + (B.2) × − + λ π = + − + − ∞ + ∫ ] [ ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u TM e e i u u I . )]] ( sin[ )] ( [sin[ 1 λ − λ − − λ + d x x x x i i (B.3) TE I TM I | | a σ 1 x m x 1 z m z [ ] 1 , + i i x x [ ] 1 , + i i z z ] , ( 1 x −∞ ) , [ +∞ n x . )] ' ( cos[ ] [ 2 1 ) ' , ' ; , ) ' ( | ' | 0 2 λ − λ + πσδ − = + − − − ∞ ∫ d x x e e u z x z z z u z z u (A.19) ]. )] ' ( cos[ 2 Re[ ' ) 2 ( 0 2 λ − λ πδ = + − ∞ ∫ d x x ue G z i u TM (A.20) 1 ' j j z z + ≤ ≤ '. ' ) ' , ' , ( 2 1 1 dz dx z x x G I TE x x z z TE i i j j δ = ∫ ∫ + + (B.1) × − + λ + λ + λ + λ π + − + − ∞ + ∫ ] [ ) 2 )( ( ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u e e i u u i . )]] ( sin[ )] ( [sin[ 1 λ λ λ d x x x x i i − − − + (B.2) × − + λ π + − + − ∞ + ∫ ] [ ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u e e i u u . )]] ( sin[ )] ( [sin[ 1 λ − λ − − λ + d x x x x i i (B.3) , ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ = ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ y x yy yx xy xx y x H H Z Z Z Z E E (C.1) 11 g x E δ 11 g . )] ' ( cos[ ] [ 2 1 ) ' , ' ; , ( ) ' ( | ' | 0 2 11 λ − λ + πσδ − = + − − − ∞ ∫ d x x e e u z x z x g z z u z z u (A.19) ]. )] ' ( cos[ 2 Re[ ' ) 2 ( 0 2 λ − λ πδ = + − ∞ ∫ d x x ue G z i u TM (A.20) 1, 1 ' ' i i j j x x x z z z + + ≤ ≤ ≤ ≤ '. ' ) ' , ' , ( 2 1 1 dz dx z x x G I TE x x z z TE i i j j δ = ∫ ∫ + + (B.1) × − + λ + λ + λ + λ π = + − + − ∞ + ∫ ] [ ) 2 )( ( ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u TE e e i u u i I . )]] ( sin[ )] ( [sin[ 1 λ λ λ d x x x x i i − − − + (B.2) × − + λ π = + − + − ∞ + ∫ ] [ ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u TM e e i u u I . )]] ( sin[ )] ( [sin[ 1 λ − λ − − λ + d x x x x i i (B.3) TE I TM I | | a σ 1 x m x 1 z m z [ ] , x x 5 . )] ' ( cos[ ] [ 2 1 ) ' , ' ; , ( ) ' ( | ' | 0 2 11 λ − λ + πσδ − = + − − − ∞ ∫ d x x e e u z x z x g z z u z z u (A.19) ]. )] ' ( cos[ 2 Re[ ' ) 2 ( 0 2 λ − λ πδ = + − ∞ ∫ d x x ue G z i u TM (A.20) 1, 1 ' ' i i j j x x x z z z + + ≤ ≤ ≤ ≤ '. ' ) ' , ' , ( 2 1 1 dz dx z x x G I TE x x z z TE i i j j δ = ∫ ∫ + + (B.1) × − + λ + λ + λ + λ π = + − + − ∞ + ∫ ] [ ) 2 )( ( ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u TE e e i u u i I . )]] ( sin[ )] ( [sin[ 1 λ λ λ d x x x x i i − − − + (B.2) × − + λ π = + − + − ∞ + ∫ ] [ ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u TM e e i u u I . )]] ( sin[ )] ( [sin[ 1 λ − λ − − λ + d x x x x i i (B.3) TE I TM I | | a σ 1 x m x 1 z m z [ ] 1 , + i i x x [ ] 1 , + i i z z ] , ( 1 x −∞ ) , [ +∞ n x ) , [ +∞ m z , ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ = ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ y x yy yx xy xx y x H H Z Z Z Z E E (C.1) xx Z xy Z yx Z yy Z x E y E x H y H }, , , , { } , , , { θ θ ∆ ⇔ P S yy yx xy xx Z Z Z Z Z Z (C.2) , ) 2 ( 2 / 1 2 2 2 2 yx yy xy xx S Z Z Z Z Z + + + = (C.3) , ) ( 2 2 / 1 2 2 2 2 yx yy xy xx yy xx xy yx P Z Z Z Z Z Z Z Z Z + + + − = (C.4) ), arctan( yx xy yy xx Z Z Z Z − + = ∆θ (C.5) ). arctan( 2 1 yx xy xx yy Z Z Z Z + − = θ (C.6) TM xy Z Z = TE yx Z Z = S Z P Z ), ( 2 1 2 2 2 TE TM S Z Z Z + = (C.7) ). 1 1 ( 2 1 1 2 2 2 TE TM P Z Z Z + = (C.8) S a ρ ), ( 2 1 TE a TM a S a ρ ρ ρ + = (C.9) S a ρ ), ( 1 TE a TM a S a ρ ρ ρ ∂ + ∂ = ∂ (C.10) x H y H }, , , , { } , , , { θ θ ∆ ⇔ P S yy yx xy xx Z Z Z Z Z Z (C.2) , ) 2 ( 2 / 1 2 2 2 2 yx yy xy xx S Z Z Z Z Z + + + = (C.3) , ) ( 2 2 / 1 2 2 2 2 yx yy xy xx yy xx xy yx P Z Z Z Z Z Z Z Z Z + + + − = (C.4) ), arctan( yx xy yy xx Z Z Z Z − + = ∆θ (C.5) ). arctan( 2 1 yx xy xx yy Z Z Z Z + − = θ (C.6) TM xy Z Z = TE yx Z Z = S Z P Z ), ( 2 1 2 2 2 TE TM S Z Z Z + = (C.7) ). 1 1 ( 2 1 1 2 2 2 TE TM P Z Z Z + = (C.8) S a ρ ), ( 2 1 TE a TM a S a ρ ρ ρ + = (C.9) S a ρ x H y H }, , , , { } , , , { θ θ ∆ ⇔ P S yy yx xy xx Z Z Z Z Z Z (C.2) , ) 2 ( 2 / 1 2 2 2 2 yx yy xy xx S Z Z Z Z Z + + + = (C.3) , ) ( 2 2 / 1 2 2 2 2 yx yy xy xx yy xx xy yx P Z Z Z Z Z Z Z Z Z + + + − = (C.4) ), arctan( yx xy yy xx Z Z Z Z − + = ∆θ (C.5) ). arctan( 2 1 yx xy xx yy Z Z Z Z + − = θ (C.6) TM xy Z Z = TE yx Z Z = S Z P Z ), ( 2 1 2 2 2 TE TM S Z Z Z + = (C.7) ). 1 1 ( 2 1 1 2 2 2 TE TM P Z Z Z + = (C.8) S a ρ ), ( 2 1 TE a TM a S a ρ ρ ρ + = (C.9) S x H y H }, , , , { } , , , { θ θ ∆ ⇔ P S yy yx xy xx Z Z Z Z Z Z (C.2) , ) 2 ( 2 / 1 2 2 2 2 yx yy xy xx S Z Z Z Z Z + + + = (C.3) , ) ( 2 2 / 1 2 2 2 2 yx yy xy xx yy xx xy yx P Z Z Z Z Z Z Z Z Z + + + − = (C.4) ), arctan( yx xy yy xx Z Z Z Z − + = ∆θ (C.5) ). arctan( 2 1 yx xy xx yy Z Z Z Z + − = θ (C.6) TM xy Z Z = TE yx Z Z = S Z P Z ), ( 2 1 2 2 2 TE TM S Z Z Z + = (C.7) ). 1 1 ( 2 1 1 2 2 2 TE TM P Z Z Z + = (C.8) S a ρ ), ( 1 TE a TM a S a ρ ρ ρ + = (C.9) x H y H }, , , , { } , , , { θ θ ∆ ⇔ P S yy yx xy xx Z Z Z Z Z Z (C.2) , ) 2 ( 2 / 1 2 2 2 2 yx yy xy xx S Z Z Z Z Z + + + = (C.3) , ) ( 2 2 / 1 2 2 2 2 yx yy xy xx yy xx xy yx P Z Z Z Z Z Z Z Z Z + + + − = (C.4) ), arctan( yx xy yy xx Z Z Z Z − + = ∆θ (C.5) ). arctan( 2 1 yx xy xx yy Z Z Z Z + − = θ (C.6) TM xy Z Z = TE yx Z Z = S Z P Z ), ( 2 1 2 2 2 TE TM S Z Z Z + = (C.7) ). 1 1 ( 2 1 1 2 2 2 TE TM P Z Z Z + = (C.8) S a ρ 1 4 ]. ) 0 , ( ) 0 , ( ) 0 , ( ) 0 , ( Re[ | | 2 | | x H x H x E x E y y x x a a δ δ σ σ δ − − = (A.14) '. ' ) ' , ' ( ) ' , ' ( ) , , ( ) , ( 13 12 11 dz dx z x z x g g g z x dE x δσ = ∫ E (A.15) . 1 0 2 ρ ρ σ ωµ ∇ × ∇ − = − ∇ y y y H H i H (A.16) . ) 0 ( ) , ( 2 z i y e H z x H − = (A.17) . 2 ) 0 ( ) , ( 2 z i x e i H z x E − = σδ (A.18) ) , z E . )] ' ( cos[ ] [ 2 1 ) ' , ' ) ' ( | ' | 0 2 λ − λ + πσδ − = + − − − ∞ ∫ d x x e e u z x z z u z z u (A.19) ]. )] ' ( cos[ 2 Re[ ' ) 2 ( 0 2 λ − λ πδ = + − ∞ ∫ d x x ue z i u (A.20) 1 ' j z + ≤ '. ' ) ' , ' , ( 2 1 1 dz dx z x x G I TE x x z z TE i i j j δ = ∫ ∫ + + (B.1) × − + λ + λ + λ + λ + − + − ∞ + ] [ ) 2 )( ( ) 2 ( ) 2 ( ) 2 ( 0 1 j j z i u z i u e e i u u i . )]] ( sin[ )] ( [sin[ 1 λ λ λ d x x x x i i − − − + (B.2) × − + λ + − + − ∞ + ∫ ] [ ) 2 ( ) 2 ( ) 2 ( 0 1 j j z i u z i u e e i u u . )]] ( sin[ )] ( [sin[ 1 λ − λ − − λ + d x x x x i i (B.3) 3 . )] ' ( cos[ ] [ ) ' ( | ' | λ − λ + + − − − d x x e e z z u z z u (A.19) ]. )] ' ( cos[ ' ) 2 λ − λ + d x x z i (A.20) '. ' ) ' , ' , ( dz dx z x x G TE (B.1) × − + − + − + ] [ ) ) 2 ( ) 2 ( 1 j j z i u z i u e e . )]] ( sin[ )] ( [sin[ 1 λ λ λ d x x x x i i − − − + (B.2) × − + − + + ] ) 2 ( ) 2 1 j j z i u z i e . )]] ( sin[ )] ( [sin[ 1 λ − λ − − λ + d x x x x i i (B.3) . )] ' ( cos[ ] ) ' ( | ' | λ − λ + + − − d x x e z z u z z (A.19) ]. )] ' ( cos[ ' λ − λ d x x z (A.20) '. ' ) ' , ' , ( dz dx z x x (B.1) × − + − + − + ] ) 2 ( ) 2 ( 1 j j z i u z i u e . )]] ( sin[ )] ( sin[ 1 λ λ λ d x x x x i i − − − + (B.2) × − + − + ] ) 2 ( 1 j j z i u z e . )]] ( sin[ )] ( [sin[ 1 λ − λ − − λ + d x x x x i i (B.3)
Geologica Acta, 8(1), 15-30 (2010) DOI: 10.1344/105.000001513 J. RODRÍGUEZ et al. 2-D Niblett-Bostick 29 Zyx modes, we have that ∆θ = 0, and θ is simply the strike direction. ZS and ZP, the series and parallel impedances, respectively, can be written as (C.7) and (C.8) Series impedance derivative We can express the series apparent resistivity r a S in terms of the TE and TM apparent resistivities as (C.9) in this equation the three apparent resistivities are complex quantities. The partial derivate of r a S is (C.10) r j is the resistivity of the j-th block in the model. We also know that (C.11) Using Eqs. (C10) and (C11), we have (C.12) Using a relation similar to Eq. (C11) for r a TM and ra TE , (C.13) in terms of apparent conductivities this is: (C.14) The general expression for the elements of matrix A is (C.15) All quantities are obtained directly from the data. Parallel impedance derivative For the parallel data, it is better to deal with apparent conductivities (C.16) The partial derivative with respect to σj is (C.17) Writing parallel apparent conductivity as (C.18) then (C.19) Using Eq. (C17) (C.20) Using a relation similar to Eq. (C11) but for σa TM and σa TE , we have (C.21) The general expression for the elements of matrix A is (C.22) Again, all quantities are obtained directly from the data. 4 Generalized Model in a Hopfield Artificial Neural Network It is necessary to define models with more realistic conductivity values (not only 0’s and 1’s). Therefore, a general model whose states are formed by an ordered set of 0’s and 1’s is defined to represent a finite precision real number. We will refer to this model as the general sequence model. The general sequence model {s i g }1 N has a typical element: 6 ), arctan( yx xy yy xx Z Z Z Z − + = ∆θ (C.5) ). arctan( 2 1 yx xy xx yy Z Z Z Z + − = θ (C.6) ), ( 2 1 2 2 2 TE TM S Z Z Z + = (C.7) ). 1 1 ( 2 1 1 2 2 2 TE TM P Z Z Z + = (C.8) ), ( 2 1 TE a TM a S a ρ ρ ρ + = (C.9) ), ( 2 1 j TE a j TM a j S a ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.10) . | | | | 1 1 j S j S a S a j S a S a i ρ φ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.11) ). 1 1 Re( 2 1 | | | | 1 j TE a S a j TM a S a j S a S a r ρ ρ ρ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.12) + ∂ ∂ + ∂ ∂ = ∂ ∂ ) | | | | 1 ( Re{ 2 1 | | j TM j TM a TM a S a TM a j S a i ρ φ ρ ρ ρ ρ ρ ρ ρ )}, | | | | 1 ( j TE j TE a TE a S a TE a i ρ φ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ (C.13) 6 , ) ( 2 2 / 1 2 2 2 2 yx yy xy xx yy xx xy yx P Z Z Z Z Z Z Z Z Z + + + − = (C.4) ), arctan( yx xy yy xx Z Z Z Z − + = ∆θ (C.5) ). arctan( 2 1 yx xy xx yy Z Z Z Z + − = θ (C.6) ), ( 2 1 2 2 2 TE TM S Z Z Z + = (C.7) ). 1 1 ( 2 1 1 2 2 2 TE TM P Z Z Z + = (C.8) ), ( 2 1 TE a TM a S a ρ ρ ρ + = (C.9) ), ( 2 1 j TE a j TM a j S a ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.10) . | | | | 1 1 j S j S a S a j S a S a i ρ φ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.11) ). 1 1 Re( 2 1 | | | | 1 j TE a S a j TM a S a j S a S a r ρ ρ ρ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.12) + ∂ ∂ + ∂ ∂ = ∂ ∂ ) | | | | 1 ( Re{ 2 1 | | j TM j TM a TM a S a TM a j S a i ρ φ ρ ρ ρ ρ ρ ρ ρ )}, | | | | 1 ( j TE j TE a TE a S a TE a i ρ φ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ (C.13) 6 }, , , , { } , , , { θ θ ∆ ⇔ P S yy yx xy xx Z Z Z Z Z Z (C.2) , ) 2 ( 2 / 1 2 2 2 2 yx yy xy xx S Z Z Z Z Z + + + = (C.3) , ) ( 2 2 / 1 2 2 2 2 yx yy xy xx yy xx xy yx P Z Z Z Z Z Z Z Z Z + + + − = (C.4) ), arctan( yx xy yy xx Z Z Z Z − + = ∆θ (C.5) ). arctan( 2 1 yx xy xx yy Z Z Z Z + − = θ (C.6) ), ( 2 1 2 2 2 TE TM S Z Z Z + = (C.7) ). 1 1 ( 2 1 1 2 2 2 TE TM P Z Z Z + = (C.8) ), ( 2 1 TE a TM a S a ρ ρ ρ + = (C.9) ), ( 2 1 j TE a j TM a j S a ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.10) . | | | | 1 1 j S j S a S a j S a S a i ρ φ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.11) ). 1 1 Re( 2 1 | | | | 1 j TE a S a j TM a S a j S a S a r ρ ρ ρ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.12) + ∂ ∂ + ∂ ∂ = ∂ ∂ ) | | | | 1 ( Re{ 2 1 | | j TM j TM a TM a S a TM a j S a i ρ φ ρ ρ ρ ρ ρ ρ ρ )}, | | | | 1 ( j TE j TE a TE a S a TE a i ρ φ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ (C.13) 6 }, , , , { } , , , { θ θ ∆ ⇔ P S yy yx xy xx Z Z Z Z Z Z (C.2) , ) 2 ( 2 / 1 2 2 2 2 yx yy xy xx S Z Z Z Z Z + + + = (C.3) , ) ( 2 2 / 1 2 2 2 2 yx yy xy xx yy xx xy yx P Z Z Z Z Z Z Z Z Z + + + − = (C.4) ), arctan( yx xy yy xx Z Z Z Z − + = ∆θ (C.5) ). arctan( 2 1 yx xy xx yy Z Z Z Z + − = θ (C.6) ), ( 2 1 2 2 2 TE TM S Z Z Z + = (C.7) ). 1 1 ( 2 1 1 2 2 2 TE TM P Z Z Z + = (C.8) ), ( 2 1 TE a TM a S a ρ ρ ρ + = (C.9) ), ( 2 1 j TE a j TM a j S a ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.10) . | | | | 1 1 j S j S a S a j S a S a i ρ φ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.11) ). 1 1 Re( 2 1 | | | | 1 j TE a S a j TM a S a j S a S a r ρ ρ ρ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.12) + ∂ ∂ + ∂ ∂ = ∂ ∂ ) | | | | 1 ( Re{ 2 1 | | | j TM j TM a TM a S a TM a j S a i ρ φ ρ ρ ρ ρ ρ ρ ρ )}, | | | | 1 ( j TE j TE a TE a S a TE a i ρ φ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ (C.13) 6 }, , , , { } , , , { θ θ ∆ ⇔ P S yy yx xy xx Z Z Z Z Z Z (C.2) , ) 2 ( 2 / 1 2 2 2 2 yx yy xy xx S Z Z Z Z Z + + + = (C.3) , ) ( 2 2 / 1 2 2 2 2 yx yy xy xx yy xx xy yx P Z Z Z Z Z Z Z Z Z + + + − = (C.4) ), arctan( yx xy yy xx Z Z Z Z − + = ∆θ (C.5) ). arctan( 2 1 yx xy xx yy Z Z Z Z + − = θ (C.6) xy x ), ( 2 1 2 2 2 TE TM S Z Z Z + = (C.7) ). 1 1 ( 2 1 1 2 2 2 TE TM P Z Z Z + = (C.8) ), ( 2 1 TE a TM a S a ρ ρ ρ + = (C.9) ), ( 2 1 j TE a j TM a j S a ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.10) . | | | | 1 1 j S j S a S a j S a S a i ρ φ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.11) ). 1 1 Re( 2 1 | | | | 1 j TE a S a j TM a S a j S a S a r ρ ρ ρ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.12) + ∂ ∂ + ∂ ∂ = ∂ ∂ ) | | | | 1 ( Re{ 2 1 | | | | 1 j TM j TM a TM a S a TM a j S a S a i ρ φ ρ ρ ρ ρ ρ ρ ρ ρ )}, | | | | 1 ( j TE j TE a TE a S a TE a i ρ φ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ (C.13) 6 x y }, , , , { } , , , { θ θ ∆ ⇔ P S yy yx xy xx Z Z Z Z Z Z (C.2) , ) 2 ( 2 / 1 2 2 2 2 yx yy xy xx S Z Z Z Z Z + + + = (C.3) , ) ( 2 2 / 1 2 2 2 2 yx yy xy xx yy xx xy yx P Z Z Z Z Z Z Z Z Z + + + − = (C.4) ), arctan( yx xy yy xx Z Z Z Z − + = ∆θ (C.5) ). arctan( 2 1 yx xy xx yy Z Z Z Z + − = θ (C.6) M xy Z = E yx Z = ), ( 2 1 2 2 2 TE TM S Z Z Z + = (C.7) ). 1 1 ( 2 1 1 2 2 2 TE TM P Z Z Z + = (C.8) S ), ( 2 1 TE a TM a S a ρ ρ ρ + = (C.9) S ), ( 2 1 j TE a j TM a j S a ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.10) j . | | | | 1 1 j S j S a S a j S a S a i ρ φ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.11) ). 1 1 Re( 2 1 | | | | 1 j TE a S a j TM a S a j S a S a r ρ ρ ρ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.12) TM TE a + ∂ ∂ + ∂ ∂ = ∂ ∂ ) | | | | 1 ( Re{ 2 1 | | | | 1 j TM j TM a TM a S a TM a j S a S a i ρ φ ρ ρ ρ ρ ρ ρ ρ ρ )}, | | | | 1 ( j TE j TE a TE a S a TE a i ρ φ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ (C.13) 6 x H y H }, , , , { } , , , { θ θ ∆ ⇔ P S yy yx xy xx Z Z Z Z Z Z (C.2) , ) 2 ( 2 / 1 2 2 2 2 yx yy xy xx S Z Z Z Z Z + + + = (C.3) , ) ( 2 2 / 1 2 2 2 2 yx yy xy xx yy xx xy yx P Z Z Z Z Z Z Z Z Z + + + − = (C.4) ), arctan( yx xy yy xx Z Z Z Z − + = ∆θ (C.5) ). arctan( 2 1 yx xy xx yy Z Z Z Z + − = θ (C.6) TM xy Z Z = TE yx Z Z = S Z P Z ), ( 2 1 2 2 2 TE TM S Z Z Z + = (C.7) ). 1 1 ( 2 1 1 2 2 2 TE TM P Z Z Z + = (C.8) S a ρ ), ( 2 1 TE a TM a S a ρ ρ ρ + = (C.9) S a ρ ), ( 2 1 j TE a j TM a j S a ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.10) j ρ . | | | | 1 1 j S j S a S a j S a S a i ρ φ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.11) ). 1 1 Re( 2 1 | | | | 1 j TE a S a j TM a S a j S a S a r ρ ρ ρ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.12) TM a ρ TE a ρ + ∂ ∂ + ∂ ∂ = ∂ ∂ ) | | | | 1 ( Re{ 2 1 | | | | 1 j TM j TM a TM a S a TM a j S a S a i ρ φ ρ ρ ρ ρ ρ ρ ρ ρ )}, | | | | 1 ( j TE j TE a TE a S a TE a i ρ φ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ (C.13) 6 }, , , , { } , , , { θ θ ∆ ⇔ P S yy yx xy xx Z Z Z Z Z Z (C.2) , ) 2 ( 2 / 1 2 2 2 2 yx yy xy xx S Z Z Z Z Z + + + = (C.3) , ) ( 2 2 / 1 2 2 2 2 yx yy xy xx yy xx xy yx P Z Z Z Z Z Z Z Z Z + + + − = (C.4) ), arctan( yx xy yy xx Z Z Z Z − + = ∆θ (C.5) ). arctan( 2 1 yx xy xx yy Z Z Z Z + − = θ (C.6) ), ( 2 1 2 2 2 TE TM S Z Z Z + = (C.7) ). 1 1 ( 2 1 1 2 2 2 TE TM P Z Z Z + = (C.8) ), ( 2 1 TE a TM a S a ρ ρ ρ + = (C.9) ), ( 2 1 j TE a j TM a j S a ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.10) . | | | | 1 1 j S j S a S a j S a S a i ρ φ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.11) ). 1 1 Re( 2 1 | | | | 1 j TE a S a j TM a S a j S a S a r ρ ρ ρ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.12) + ∂ ∂ + ∂ ∂ = ∂ ∂ ) | | | | 1 ( Re{ 2 1 | | | j TM j TM a TM a S a TM a j S a i ρ φ ρ ρ ρ ρ ρ ρ ρ )}, | | | | 1 ( j TE j TE a TE a S a TE a i ρ φ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ (C.13) + ∂ ∂ − ∂ ∂ = ∂ ∂ ) | | | (| | | Re{ 2 1 | | j TM j TM a TM a S a S a TM a j S a i σ φ σ σ ρ ρ ρ ρ σ σ )}. | | | (| | | j TE j TE a TE a S a S a TE a i σ φ σ σ ρ ρ ρ ρ ∂ ∂ − ∂ ∂ (C.14) }. | | | | | | | | Re{ 2 1 TE S a S a TE a TE a TM S a S a TM a TM a I I ρ ρ ρ ρ ρ ρ ρ ρ + (C.15) ). ( 2 1 TE a TM a P a σ σ σ + = (C.16) ). ( 2 1 j TE a j TM a j P a σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.17) , | | P i P a P a e φ σ σ − = (C.18) . | | | | 1 1 j P j P a P a j P a P a i σ φ σ σ σ σ σ σ ∂ ∂ − ∂ ∂ = ∂ ∂ (C.19) 1 1 1 | | 1 TE a TM a P a σ σ σ ∂ ∂ ∂ + ∂ ∂ − ∂ ∂ = ) | | | (| | | Re{ 2 1 j TM j TM a TM a S a S a TM a i σ φ σ σ ρ ρ ρ ρ )}. | | | (| | | j TE j TE a TE a S a S a TE a i σ φ σ σ ρ ρ ρ ρ ∂ ∂ − ∂ ∂ (C.14) }. | | | | | | | | Re{ 2 1 TE S a S a TE a TE a TM S a S a TM a TM a I I ρ ρ ρ ρ ρ ρ ρ ρ + (C.15) ). ( 2 1 TE a TM a P a σ σ σ + = (C.16) ). ( 2 1 j TE a j TM a j P a σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.17) , | | P i P a P a e φ σ σ − = (C.18) . | | | | 1 1 j P j P a P a j P a P a i σ φ σ σ σ σ σ σ ∂ ∂ − ∂ ∂ = ∂ ∂ (C.19) 1 1 1 | | 1 TE a TM a P a σ σ σ ∂ ∂ ∂ 7 + ∂ ∂ − ∂ ∂ = ∂ ∂ ) | | | (| | | Re{ 2 1 | | j TM j TM a TM a S a S a TM a j S a i σ φ σ σ ρ ρ ρ ρ σ σ )}. | | | (| | | j TE j TE a TE a S a S a TE a i σ φ σ σ ρ ρ ρ ρ ∂ ∂ − ∂ ∂ (C.14) }. | | | | | | | | Re{ 2 1 TE S a S a TE a TE a TM S a S a TM a TM a I I ρ ρ ρ ρ ρ ρ ρ ρ + (C.15) ). ( 2 1 TE a TM a P a σ σ σ + = (C.16) ). ( 2 1 j TE a j TM a j P a σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.17) , | | P i P a P a e φ σ σ − = (C.18) . | | | | 1 1 j P j P a P a j P a P a i σ φ σ σ σ σ σ σ ∂ ∂ − ∂ ∂ = ∂ ∂ (C.19) ). 1 1 Re( 2 1 | | | | 1 j TE a P a j TM a P a j P a P a σ σ σ σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.20) TM a σ TE a σ + ∂ ∂ − ∂ ∂ = ∂ ∂ − ) | | | | 1 ( | Re{| 2 1 | | ) ( j TM j TM a TM a i TM a j P a i e TM P σ φ σ σ σ σ σ σ φ φ )}. | | | | 1 ( | | ) ( j TE j TE a TE a i TE a i e TE P σ φ σ σ σ σ φ φ ∂ ∂ − ∂ ∂ − (C.21) }. Re{ 2 1 ) ( ) ( TE i TM i I e I e TE P TM P φ φ φ φ − − + (C.22) N g i 1 } {σ , ,..., 2 , 1 , 2 2 ) ( N i B B U t ij j U D j g i = − = ∑ − = σ (D.1) 0 = ij B ij B N g i 1 } {σ − − − = + = − = = − = = ∑ ∑ ∑ ∑ ∑ ) ( ) ( ) ( 1 1 1 ] 2 [ 2 1 t jn t im kj ki n m M k U D n N j U D m N i B B A A C + + + − + = = = = − = = ∑ ∑ ∑ ∑ ∑ ∑ ) ( ] ) ( 1 1 1 ) ( 2 1 1 ] ) ) 2 ( ) 2 ( ) 2 ( 2 1 [ t im kj ki U m N j M k a k ki m M k t im ki m M k U D m N i B B A A s A B A (a−term−independent−of−the−model). (D.2) 7 + ∂ ∂ − ∂ ∂ = ∂ ∂ ) | | | (| | | Re{ 2 1 | | j TM j TM a TM a S a S a TM a j S a i σ φ σ σ ρ ρ ρ ρ σ σ )}. | | | (| | | j TE j TE a TE a S a S a TE a i σ φ σ σ ρ ρ ρ ρ ∂ ∂ − ∂ ∂ (C.14) }. | | | | | | | | Re{ 2 1 TE S a S a TE a TE a TM S a S a TM a TM a I I ρ ρ ρ ρ ρ ρ ρ ρ + (C.15) ). ( 2 1 TE a TM a P a σ σ σ + = (C.16) ). ( 2 1 j TE a j TM a j P a σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.17) , | | P i P a P a e φ σ σ − = (C.18) . | | | | 1 1 j P j P a P a j P a P a i σ φ σ σ σ σ σ σ ∂ ∂ − ∂ ∂ = ∂ ∂ (C.19) ). 1 1 Re( 2 1 | | | | 1 j TE a P a j TM a P a j P a P a σ σ σ σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.20) TM a σ TE a σ + ∂ ∂ − ∂ ∂ = ∂ ∂ − ) | | | | 1 ( | Re{| 2 1 | | ) ( j TM j TM a TM a i TM a j P a i e TM P σ φ σ σ σ σ σ σ φ φ )}. | | | | 1 ( | | ) ( j TE j TE a TE a i TE a i e TE P σ φ σ σ σ σ φ φ ∂ ∂ − ∂ ∂ − (C.21) }. Re{ 2 1 ) ( ) ( TE i TM i I e I e TE P TM P φ φ φ φ − − + (C.22) N g i 1 } {σ , ,..., 2 , 1 , 2 2 ) ( N i B B U t ij j U D j g i = − = ∑ − = σ (D.1) 0 = ij B ij B N g i 1 } {σ − − − = + = − = = − = = ∑ ∑ ∑ ∑ ∑ ) ( ) ( ) ( 1 1 1 ] 2 [ 2 1 t jn t im kj ki n m M k U D n N j U D m N i B B A A C + + + − + = = = = − = = ∑ ∑ ∑ ∑ ∑ ∑ ) ( ] ) ( 1 1 1 ) ( 2 1 1 ] ) ) 2 ( ) 2 ( ) 2 ( 2 1 [ t im kj ki U m N j M k a k ki m M k t im ki m M k U D m N i B B A A s A B A (a−term−independent−of−the−model). (D.2) 7 + ∂ ∂ − ∂ ∂ = ∂ ∂ ) | | | (| | | Re{ 2 1 | | j TM j TM a TM a S a S a TM a j S a i σ φ σ σ ρ ρ ρ ρ σ σ )}. | | | (| | | j TE j TE a TE a S a S a TE a i σ φ σ σ ρ ρ ρ ρ ∂ ∂ − ∂ ∂ (C.14) }. | | | | | | | | Re{ 2 1 TE S a S a TE a TE a TM S a S a TM a TM a I I ρ ρ ρ ρ ρ ρ ρ ρ + (C.15) ). ( 2 1 TE a TM a P a σ σ σ + = (C.16) ). ( 2 1 j TE a j TM a j P a σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.17) , | | P i P a P a e φ σ σ − = (C.18) . | | | | 1 1 j P j P a P a j P a P a i σ φ σ σ σ σ σ σ ∂ ∂ − ∂ ∂ = ∂ ∂ (C.19) ). 1 1 Re( 2 1 | | | | 1 j TE a P a j TM a P a j P a P a σ σ σ σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.20) TM a σ TE a σ + ∂ ∂ − ∂ ∂ = ∂ ∂ − ) | | | | 1 ( | Re{| 2 1 | | ) ( j TM j TM a TM a i TM a j P a i e TM P σ φ σ σ σ σ σ σ φ φ )}. | | | | 1 ( | | ) ( j TE j TE a TE a i TE a i e TE P σ φ σ σ σ σ φ φ ∂ ∂ − ∂ ∂ − (C.21) }. Re{ 2 1 ) ( ) ( TE i TM i I e I e TE P TM P φ φ φ φ − − + (C.22) N g i 1 } {σ , ,..., 2 , 1 , 2 2 ) ( N i B B U t ij j U D j g i = − = ∑ − = σ (D.1) 0 = ij B ij B N g i 1 } {σ − − − = + = − = = − = = ∑ ∑ ∑ ∑ ∑ ) ( ) ( ) ( 1 1 1 ] 2 [ 2 1 t jn t im kj ki n m M k U D n N j U D m N i B B A A C + + + − + = = = = − = = ∑ ∑ ∑ ∑ ∑ ∑ ) ( ] ) ( 1 1 1 ) ( 2 1 1 ] ) ) 2 ( ) 2 ( ) 2 ( 2 1 [ t im kj ki U m N j M k a k ki m M k t im ki m M k U D m N i B B A A s A B A (a−term−independent−of−the−model). (D.2) 7 + ∂ ∂ − ∂ ∂ = ∂ ∂ ) | | | (| | | Re{ 2 1 | | j TM j TM a TM a S a S a TM a j S a i σ φ σ σ ρ ρ ρ ρ σ σ )}. | | | (| | | j TE j TE a TE a S a S a TE a i σ φ σ σ ρ ρ ρ ρ ∂ ∂ − ∂ ∂ (C.14) }. | | | | | | | | Re{ 2 1 TE S a S a TE a TE a TM S a S a TM a TM a I I ρ ρ ρ ρ ρ ρ ρ ρ + (C.15) ). ( 2 1 TE a TM a P a σ σ σ + = (C.16) ). ( 2 1 j TE a j TM a j P a σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.17) , | | P i P a P a e φ σ σ − = (C.18) . | | | | 1 1 j P j P a P a j P a P a i σ φ σ σ σ σ σ σ ∂ ∂ − ∂ ∂ = ∂ ∂ (C.19) ). 1 1 Re( 2 1 | | | | 1 j TE a P a j TM a P a j P a P a σ σ σ σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.20) TM a σ TE a σ + ∂ ∂ − ∂ ∂ = ∂ ∂ − ) | | | | 1 ( | Re{| 2 1 | | ) ( j TM j TM a TM a i TM a j P a i e TM P σ φ σ σ σ σ σ σ φ φ )}. | | | | 1 ( | | ) ( j TE j TE a TE a i TE a i e TE P σ φ σ σ σ σ φ φ ∂ ∂ − ∂ ∂ − (C.21) }. Re{ 2 1 ) ( ) ( TE i TM i I e I e TE P TM P φ φ φ φ − − + (C.22) N g i 1 } {σ , ,..., 2 , 1 , 2 2 ) ( N i B B U t ij j U D j g i = − = ∑ − = σ (D.1) 0 = ij B ij B N g i 1 } {σ − − − = + = − = = − = = ∑ ∑ ∑ ∑ ∑ ) ( ) ( ) ( 1 1 1 ] 2 [ 2 1 t jn t im kj ki n m M k U D n N j U D m N i B B A A C + + + − + = = = = − = = ∑ ∑ ∑ ∑ ∑ ∑ ) ( ] ) ( 1 1 1 ) ( 2 1 1 ] ) ) 2 ( ) 2 ( ) 2 ( 2 1 [ t im kj ki U m N j M k a k ki m M k t im ki m M k U D m N i B B A A s A B A (a−term−independent−of−the−model). (D.2) 7 + ∂ ∂ − ∂ ∂ = ∂ ∂ ) | | | (| | | Re{ 2 1 | | j TM j TM a TM a S a S a TM a j S a i σ φ σ σ ρ ρ ρ ρ σ σ )}. | | | (| | | j TE j TE a TE a S a S a TE a i σ φ σ σ ρ ρ ρ ρ ∂ ∂ − ∂ ∂ (C. }. | | | | | | | | Re{ 2 1 TE S a S a TE a TE a TM S a S a TM a TM a I I ρ ρ ρ ρ ρ ρ ρ ρ + (C.15) ). ( 2 1 TE a TM a P a σ σ σ + = (C.16) ). ( 2 1 j TE a j TM a j P a σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.17) , | | P i P a P a e φ σ σ − = (C.18) . | | | | 1 1 j P j P a P a j P a P a i σ φ σ σ σ σ σ σ ∂ ∂ − ∂ ∂ = ∂ ∂ (C.19) ). 1 1 Re( 2 1 | | | | 1 j TE a P a j TM a P a j P a P a σ σ σ σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.20) TM a σ TE a σ + ∂ ∂ − ∂ ∂ = ∂ ∂ − ) | | | | 1 ( | Re{| 2 1 | | ) ( j TM j TM a TM a i TM a j P a i e TM P σ φ σ σ σ σ σ σ φ φ )}. | | | | 1 ( | | ) ( j TE j TE a TE a i TE a i e TE P σ φ σ σ σ σ φ φ ∂ ∂ − ∂ ∂ − (C. }. Re{ 2 1 ) ( ) ( TE i TM i I e I e TE P TM P φ φ φ φ − − + (C.22) N g i 1 } {σ , ,..., 2 , 1 , 2 2 ) ( N i B B U t ij j U D j g i = − = ∑ − = σ (D.1) 0 = ij B ij B N g i 1 } {σ − − − = + = − = = − = = ∑ ∑ ∑ ∑ ∑ ) ( ) ( ) ( 1 1 1 ] 2 [ 2 1 t jn t im kj ki n m M k U D n N j U D m N i B B A A C + + − + = = = = − = = ∑ ∑ ∑ ∑ ∑ ∑ ) ( ] ) ( 1 1 1 ) ( 2 1 1 ] ) ) 2 ( ) 2 ( ) 2 ( 2 1 [ t im kj ki U m N j M k a k ki m M k t im ki m M k U D m N i B B A A s A B A (a−term−independent−of−the−model). (D. 7 + ∂ ∂ − ∂ ∂ = ∂ ∂ ) | | | (| | | Re{ 2 1 | | j TM j TM a TM a S a S a TM a j S a i σ φ σ σ ρ ρ ρ ρ σ σ )}. | | | (| | | j TE j TE a TE a S a S a TE a i σ φ σ σ ρ ρ ρ ρ ∂ ∂ − ∂ ∂ }. | | | | | | | | Re{ 2 1 TE S a S a TE a TE a TM S a S a TM a TM a I I ρ ρ ρ ρ ρ ρ ρ ρ + (C.15) ). ( 2 1 TE a TM a P a σ σ σ + = (C.16) ). ( 2 1 j TE a j TM a j P a σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.17) , | | P i P a P a e φ σ σ − = (C.18) . | | | | 1 1 j P j P a P a j P a P a i σ φ σ σ σ σ σ σ ∂ ∂ − ∂ ∂ = ∂ ∂ (C.19) ). 1 1 Re( 2 1 | | | | 1 j TE a P a j TM a P a j P a P a σ σ σ σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.20) TM a σ TE a σ + ∂ ∂ − ∂ ∂ = ∂ ∂ − ) | | | | 1 ( | Re{| 2 1 | | ) ( j TM j TM a TM a i TM a j P a i e TM P σ φ σ σ σ σ σ σ φ φ )} | | | | 1 ( | | ) ( j TE j TE a TE a i TE a i e TE P σ φ σ σ σ σ φ φ ∂ ∂ − ∂ ∂ − }. Re{ 2 1 ) ( ) ( TE i TM i I e I e TE P TM P φ φ φ φ − − + (C.22) N g i 1 } {σ , ,..., 2 , 1 , 2 2 ) ( N i B B U t ij j U D j g i = − = ∑ − = σ (D.1) 0 = ij B ij B N g i 1 } {σ − − − = + = − = = − = = ∑ ∑ ∑ ∑ ∑ ) ( ) ( ) ( 1 1 1 ] 2 [ 2 1 t jn t im kj ki n m M k U D n N j U D m N i B B A A C + + − + = = = = − = = ∑ ∑ ∑ ∑ ∑ ∑ ] ) ( 1 1 1 ) ( 2 1 1 ) ) 2 ( ) 2 ( ) 2 ( 2 1 [ kj ki U m N j M k a k ki m M k t im ki m M k U D m N i B A A s A B A (a−term−independent−of−the−model). 7 + ∂ ∂ − ∂ ∂ = ∂ ∂ ) | | | (| | | Re{ 2 1 | | j TM j TM a TM a S a S a TM a j S a i σ φ σ σ ρ ρ ρ ρ σ σ )}. | | | (| | | j TE j TE a TE a S a S a TE a i σ φ σ σ ρ ρ ρ ρ ∂ ∂ − ∂ ∂ (C.14) }. | | | | | | | | Re{ 2 1 TE S a S a TE a TE a TM S a S a TM a TM a I I ρ ρ ρ ρ ρ ρ ρ ρ + (C.15) ). ( 2 1 TE a TM a P a σ σ σ + = (C.16) ). ( 2 1 j TE a j TM a j P a σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.17) , | | P i P a P a e φ σ σ − = (C.18) . | | | | 1 1 j P j P a P a j P a P a i σ φ σ σ σ σ σ σ ∂ ∂ − ∂ ∂ = ∂ ∂ (C.19) ). 1 1 Re( 2 1 | | | | 1 j TE a P a j TM a P a j P a P a σ σ σ σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.20) TM a σ TE a σ + ∂ ∂ − ∂ ∂ = ∂ ∂ − ) | | | | 1 ( | Re{| 2 1 | | ) ( j TM j TM a TM a i TM a j P a i e TM P σ φ σ σ σ σ σ σ φ φ )}. | | | | 1 ( | | ) ( j TE j TE a TE a i TE a i e TE P σ φ σ σ σ σ φ φ ∂ ∂ − ∂ ∂ − (C.21) }. Re{ 2 1 ) ( ) ( TE i TM i I e I e TE P TM P φ φ φ φ − − + (C.22) N g i 1 } {σ , ,..., 2 , 1 , 2 2 ) ( N i B B U t ij j U D j g i = − = ∑ − = σ (D.1) 0 = ij B ij B N g i 1 } {σ − − − = + = − = = − = = ∑ ∑ ∑ ∑ ∑ ) ( ) ( ) ( 1 1 1 ] 2 [ 2 1 t jn t im kj ki n m M k U D n N j U D m N i B B A A C + + + − + = = = = − = = ∑ ∑ ∑ ∑ ∑ ∑ ) ( ] ) ( 1 1 1 ) ( 2 1 1 ] ) ) 2 ( ) 2 ( ) 2 ( 2 1 [ t im kj ki U m N j M k a k ki m M k t im ki m M k U D m N i B B A A s A B A (a−term−independent−of−the−model). (D.2) 7 + ∂ ∂ − ∂ ∂ = ∂ ∂ ) | | | (| | | Re{ 2 1 | | j TM j TM a TM a S a S a TM a j S a i σ φ σ σ ρ ρ ρ ρ σ σ )}. | | | (| | | j TE j TE a TE a S a S a TE a i σ φ σ σ ρ ρ ρ ρ ∂ ∂ − ∂ ∂ (C.14) }. | | | | | | | | Re{ 2 1 TE S a S a TE a TE a TM S a S a TM a TM a I I ρ ρ ρ ρ ρ ρ ρ ρ + (C.15) ). ( 2 1 TE a TM a P a σ σ σ + = (C.16) ). ( 2 1 j TE a j TM a j P a σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.17) , | | P i P a P a e φ σ σ − = (C.18) . | | | | 1 1 j P j P a P a j P a P a i σ φ σ σ σ σ σ σ ∂ ∂ − ∂ ∂ = ∂ ∂ (C.19) ). 1 1 Re( 2 1 | | | | 1 j TE a P a j TM a P a j P a P a σ σ σ σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.20) TM a σ TE a σ + ∂ ∂ − ∂ ∂ = ∂ ∂ − ) | | | | 1 ( | Re{| 2 1 | | ) ( j TM j TM a TM a i TM a j P a i e TM P σ φ σ σ σ σ σ σ φ φ )}. | | | | 1 ( | | ) ( j TE j TE a TE a i TE a i e TE P σ φ σ σ σ σ φ φ ∂ ∂ − ∂ ∂ − (C.21) }. Re{ 2 1 ) ( ) ( TE i TM i I e I e TE P TM P φ φ φ φ − − + (C.22) N g i 1 } {σ , ,..., 2 , 1 , 2 2 ) ( N i B B U t ij j U D j g i = − = ∑ − = σ (D.1) 0 = ij B ij B N g i 1 } {σ − − − = + = − = = − = = ∑ ∑ ∑ ∑ ∑ ) ( ) ( ) ( 1 1 1 ] 2 [ 2 1 t jn t im kj ki n m M k U D n N j U D m N i B B A A C + + + − + = = = = − = = ∑ ∑ ∑ ∑ ∑ ∑ ) ( ] ) ( 1 1 1 ) ( 2 1 1 ] ) ) 2 ( ) 2 ( ) 2 ( 2 1 [ t im kj ki U m N j M k a k ki m M k t im ki m M k U D m N i B B A A s A B A (a−term−independent−of−the−model). (D.2) 6 , ) 2 ( 2 / 1 S Z = (C.3) , ) ( 2 2 / 1 2 2 2 2 yx yy xy xx yy xx xy yx P Z Z Z Z Z Z Z Z Z + + + − = (C.4) ), arctan( yx xy yy xx Z Z Z Z − + = ∆θ (C.5) ). arctan( 2 1 yx xy xx yy Z Z Z Z + − = θ (C.6) TM xy Z Z = TE yx Z Z = S Z P Z ), ( 2 1 2 2 2 TE TM S Z Z Z + = (C.7) ). 1 1 ( 2 1 1 2 2 2 TE TM P Z Z Z + = (C.8) S a ρ ), ( 2 1 TE a TM a S a ρ ρ ρ + = (C.9) S a ρ ), ( 2 1 j TE a j TM a j S a ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.10) j ρ . | | | | 1 1 j S j S a S a j S a S a i ρ φ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.11) ). 1 1 Re( 2 1 | | | | 1 j TE a S a j TM a S a j S a S a r ρ ρ ρ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.12) TM a ρ TE a ρ + ∂ ∂ + ∂ ∂ = ∂ ∂ ) | | | | 1 ( Re{ 2 1 | | | | 1 j TM j TM a TM a S a TM a j S a S a i ρ φ ρ ρ ρ ρ ρ ρ ρ ρ )}, | | | | 1 ( j TE j TE a TE a S a TE a i ρ φ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ (C.13) 6 }, , , , { θ θ ∆ ⇔ P S Z Z (C.2) , ) 2 2 / 1 2 2 yx yy y Z Z + + (C.3) , ) 2 / 1 2 2 2 yx yy xy yy xx xy Z Z Z Z Z + + − (C.4) ), ( yx xy yy xx Z Z Z Z − + (C.5) ). n( yx xy xx yy Z Z Z Z + − (C.6) ), 2 2 TE TM Z + (C.7) ). 1 1 2 2 TE TM Z + (C.8) ), TE a TM a ρ + (C.9) ), j TE a j TM a ρ ρ ρ ρ ∂ ∂ + (C.10) . | | | j S j S a i ρ φ ρ ρ ∂ ∂ + ∂ ∂ (C.11) ). 1 1 j TE a S a j TM a S a r ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ (C.12) + ∂ ∂ + ∂ ∂ ) | | | 1 j TM j TM a TM a i ρ φ ρ ρ ρ )}, | | | | 1 ( j TE j TE a TE a S a TE a i ρ φ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ (C.13) 6 }, , , , { θ θ ∆ P S Z Z (C.2) , ) 2 / 1 2 2 yx yy Z Z + (C.3) , ) 2 / 1 2 2 yx yy yy xx y Z Z Z Z + + − (C.4) ), yx xy yy xx Z Z − + (C.5) ). yx xy xx yy Z Z + − (C.6) ), 2 TE Z + (C.7) ). 1 2 TE Z + (C.8) ), TE a ρ + (C.9) ), j TE a ρ ρ ∂ ∂ + (C.10) . | | j S j S a i ρ φ ρ ρ ∂ ∂ + ∂ (C.11) ). 1 j TE a S a j TM a r ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ (C.12) + ∂ ∂ + ∂ ∂ ) | | | j TM j TM a M i ρ φ ρ ρ )}, | | | | 1 ( j TE j TE a TE a S a TE a i ρ φ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ (C.13) + ∂ ∂ − ∂ ∂ = ∂ ∂ ) | | | (| | | Re{ 2 1 | | j TM j TM a TM a S a S a TM a j S a i σ φ σ σ ρ ρ ρ ρ σ σ )}. | | | (| | | j TE j TE a TE a S a S a TE a i σ φ σ σ ρ ρ ρ ρ ∂ ∂ − ∂ ∂ (C.14) }. | | | | | | | | Re{ 2 1 TE S a S a TE a TE a TM S a S a TM a TM a I I ρ ρ ρ ρ ρ ρ ρ ρ + (C.15) ). ( 2 1 TE a TM a P a σ σ σ + = (C.16) ). ( 2 1 j TE a j TM a j P a σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.17) , | | P i P a P a e φ σ σ − = (C.18) . | | | | 1 1 j P j P a P a j P a P a i σ φ σ σ σ σ σ σ ∂ ∂ − ∂ ∂ = ∂ ∂ (C.19)
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Geologica Acta, 8(1), 15-30 (2010)<br />
DOI: 10.1344/105.000001513<br />
J. RODRÍGUEZ et al. 2-D <strong>Niblett</strong>-<strong>Bostick</strong><br />
29<br />
Zyx modes, we have that ∆θ = 0, and θ is simply the strike<br />
direction. ZS and ZP, the series and parallel impedances,<br />
respectively, can be written as<br />
(C.7)<br />
and<br />
(C.8)<br />
Series impedance derivative<br />
We can express the series apparent resistivity r a<br />
S in<br />
terms of the TE and TM apparent resistivities as<br />
(C.9)<br />
in this equation the three apparent resistivities are complex<br />
quantities. The partial derivate of r a<br />
S is<br />
(C.10)<br />
r j is the resistivity of the j-th block in the model. We also<br />
know that<br />
(C.11)<br />
Using Eqs. (C10) and (C11), we have<br />
(C.12)<br />
Using a relation similar to Eq. (C11) for r a<br />
TM and ra<br />
TE ,<br />
(C.13)<br />
in terms of apparent conductivities this is:<br />
(C.14)<br />
The general expression for the elements of matrix A is<br />
(C.15)<br />
All quantities are obtained directly from the data.<br />
Parallel impedance derivative<br />
For the parallel data, it is better to deal with apparent<br />
conductivities<br />
(C.16)<br />
The partial derivative with respect to σj is<br />
(C.17)<br />
Writing parallel apparent conductivity as<br />
(C.18)<br />
then<br />
(C.19)<br />
Using Eq. (C17)<br />
(C.20)<br />
Using a relation similar to Eq. (C11) but for σa<br />
TM and<br />
σa<br />
TE , we have<br />
(C.21)<br />
The general expression for the elements of matrix A is<br />
(C.22)<br />
Again, all quantities are obtained directly from the<br />
data.<br />
4 Generalized Model in a Hopfield Artificial Neural<br />
Network<br />
It is necessary to define models with more realistic<br />
conductivity values (not only 0’s and 1’s). Therefore, a<br />
general model whose states are formed by an ordered set<br />
of 0’s and 1’s is defined to represent a finite precision real<br />
number. We will refer to this model as the general sequence<br />
model. The general sequence model {s i<br />
g }1<br />
N has a typical<br />
element:<br />
6<br />
),<br />
arctan(<br />
yx<br />
xy<br />
yy<br />
xx<br />
Z<br />
Z<br />
Z<br />
Z<br />
−<br />
+<br />
=<br />
∆θ (C.5)<br />
).<br />
arctan(<br />
2<br />
1<br />
yx<br />
xy<br />
xx<br />
yy<br />
Z<br />
Z<br />
Z<br />
Z<br />
+<br />
−<br />
=<br />
θ (C.6)<br />
),<br />
(<br />
2<br />
1 2<br />
2<br />
2<br />
TE<br />
TM<br />
S<br />
Z<br />
Z<br />
Z +<br />
= (C.7)<br />
).<br />
1<br />
1<br />
(<br />
2<br />
1<br />
1<br />
2<br />
2<br />
2<br />
TE<br />
TM<br />
P<br />
Z<br />
Z<br />
Z<br />
+<br />
= (C.8)<br />
),<br />
(<br />
2<br />
1 TE<br />
a<br />
TM<br />
a<br />
S<br />
a<br />
ρ<br />
ρ<br />
ρ +<br />
= (C.9)<br />
),<br />
(<br />
2<br />
1<br />
j<br />
TE<br />
a<br />
j<br />
TM<br />
a<br />
j<br />
S<br />
a<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
(C.10)<br />
.<br />
|<br />
|<br />
|<br />
|<br />
1<br />
1<br />
j<br />
S<br />
j<br />
S<br />
a<br />
S<br />
a<br />
j<br />
S<br />
a<br />
S<br />
a<br />
i ρ<br />
φ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ ∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
(C.11)<br />
).<br />
1<br />
1<br />
Re(<br />
2<br />
1<br />
|<br />
|<br />
|<br />
|<br />
1<br />
j<br />
TE<br />
a<br />
S<br />
a<br />
j<br />
TM<br />
a<br />
S<br />
a<br />
j<br />
S<br />
a<br />
S<br />
a r ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ ∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
(C.12)<br />
+<br />
∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
)<br />
|<br />
|<br />
|<br />
|<br />
1<br />
(<br />
Re{<br />
2<br />
1<br />
|<br />
|<br />
j<br />
TM<br />
j<br />
TM<br />
a<br />
TM<br />
a<br />
S<br />
a<br />
TM<br />
a<br />
j<br />
S<br />
a<br />
i ρ<br />
φ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
)},<br />
|<br />
|<br />
|<br />
|<br />
1<br />
(<br />
j<br />
TE<br />
j<br />
TE<br />
a<br />
TE<br />
a<br />
S<br />
a<br />
TE<br />
a<br />
i ρ<br />
φ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
∂<br />
∂<br />
+<br />
∂<br />
∂<br />
(C.13)<br />
6<br />
,<br />
)<br />
(<br />
2 2<br />
/<br />
1<br />
2<br />
2<br />
2<br />
2<br />
yx<br />
yy<br />
xy<br />
xx<br />
yy<br />
xx<br />
xy<br />
yx<br />
P<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
+<br />
+<br />
+<br />
−<br />
= (C.4)<br />
),<br />
arctan(<br />
yx<br />
xy<br />
yy<br />
xx<br />
Z<br />
Z<br />
Z<br />
Z<br />
−<br />
+<br />
=<br />
∆θ (C.5)<br />
).<br />
arctan(<br />
2<br />
1<br />
yx<br />
xy<br />
xx<br />
yy<br />
Z<br />
Z<br />
Z<br />
Z<br />
+<br />
−<br />
=<br />
θ (C.6)<br />
),<br />
(<br />
2<br />
1 2<br />
2<br />
2<br />
TE<br />
TM<br />
S<br />
Z<br />
Z<br />
Z +<br />
= (C.7)<br />
).<br />
1<br />
1<br />
(<br />
2<br />
1<br />
1<br />
2<br />
2<br />
2<br />
TE<br />
TM<br />
P<br />
Z<br />
Z<br />
Z<br />
+<br />
= (C.8)<br />
),<br />
(<br />
2<br />
1 TE<br />
a<br />
TM<br />
a<br />
S<br />
a<br />
ρ<br />
ρ<br />
ρ +<br />
= (C.9)<br />
),<br />
(<br />
2<br />
1<br />
j<br />
TE<br />
a<br />
j<br />
TM<br />
a<br />
j<br />
S<br />
a<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
(C.10)<br />
.<br />
|<br />
|<br />
|<br />
|<br />
1<br />
1<br />
j<br />
S<br />
j<br />
S<br />
a<br />
S<br />
a<br />
j<br />
S<br />
a<br />
S<br />
a<br />
i ρ<br />
φ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ ∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
(C.11)<br />
).<br />
1<br />
1<br />
Re(<br />
2<br />
1<br />
|<br />
|<br />
|<br />
|<br />
1<br />
j<br />
TE<br />
a<br />
S<br />
a<br />
j<br />
TM<br />
a<br />
S<br />
a<br />
j<br />
S<br />
a<br />
S<br />
a r ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ ∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
(C.12)<br />
+<br />
∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
)<br />
|<br />
|<br />
|<br />
|<br />
1<br />
(<br />
Re{<br />
2<br />
1<br />
|<br />
|<br />
j<br />
TM<br />
j<br />
TM<br />
a<br />
TM<br />
a<br />
S<br />
a<br />
TM<br />
a<br />
j<br />
S<br />
a<br />
i ρ<br />
φ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
)},<br />
|<br />
|<br />
|<br />
|<br />
1<br />
(<br />
j<br />
TE<br />
j<br />
TE<br />
a<br />
TE<br />
a<br />
S<br />
a<br />
TE<br />
a<br />
i ρ<br />
φ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
∂<br />
∂<br />
+<br />
∂<br />
∂<br />
(C.13)<br />
6<br />
},<br />
,<br />
,<br />
,<br />
{<br />
}<br />
,<br />
,<br />
,<br />
{ θ<br />
θ ∆<br />
⇔ P<br />
S<br />
yy<br />
yx<br />
xy<br />
xx<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z (C.2)<br />
,<br />
)<br />
2<br />
(<br />
2<br />
/<br />
1<br />
2<br />
2<br />
2<br />
2<br />
yx<br />
yy<br />
xy<br />
xx<br />
S<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
+<br />
+<br />
+<br />
= (C.3)<br />
,<br />
)<br />
(<br />
2 2<br />
/<br />
1<br />
2<br />
2<br />
2<br />
2<br />
yx<br />
yy<br />
xy<br />
xx<br />
yy<br />
xx<br />
xy<br />
yx<br />
P<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
+<br />
+<br />
+<br />
−<br />
= (C.4)<br />
),<br />
arctan(<br />
yx<br />
xy<br />
yy<br />
xx<br />
Z<br />
Z<br />
Z<br />
Z<br />
−<br />
+<br />
=<br />
∆θ (C.5)<br />
).<br />
arctan(<br />
2<br />
1<br />
yx<br />
xy<br />
xx<br />
yy<br />
Z<br />
Z<br />
Z<br />
Z<br />
+<br />
−<br />
=<br />
θ (C.6)<br />
),<br />
(<br />
2<br />
1 2<br />
2<br />
2<br />
TE<br />
TM<br />
S<br />
Z<br />
Z<br />
Z +<br />
= (C.7)<br />
).<br />
1<br />
1<br />
(<br />
2<br />
1<br />
1<br />
2<br />
2<br />
2<br />
TE<br />
TM<br />
P<br />
Z<br />
Z<br />
Z<br />
+<br />
= (C.8)<br />
),<br />
(<br />
2<br />
1 TE<br />
a<br />
TM<br />
a<br />
S<br />
a<br />
ρ<br />
ρ<br />
ρ +<br />
= (C.9)<br />
),<br />
(<br />
2<br />
1<br />
j<br />
TE<br />
a<br />
j<br />
TM<br />
a<br />
j<br />
S<br />
a<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
(C.10)<br />
.<br />
|<br />
|<br />
|<br />
|<br />
1<br />
1<br />
j<br />
S<br />
j<br />
S<br />
a<br />
S<br />
a<br />
j<br />
S<br />
a<br />
S<br />
a<br />
i ρ<br />
φ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ ∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
(C.11)<br />
).<br />
1<br />
1<br />
Re(<br />
2<br />
1<br />
|<br />
|<br />
|<br />
|<br />
1<br />
j<br />
TE<br />
a<br />
S<br />
a<br />
j<br />
TM<br />
a<br />
S<br />
a<br />
j<br />
S<br />
a<br />
S<br />
a r ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ ∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
(C.12)<br />
+<br />
∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
)<br />
|<br />
|<br />
|<br />
|<br />
1<br />
(<br />
Re{<br />
2<br />
1<br />
|<br />
|<br />
j<br />
TM<br />
j<br />
TM<br />
a<br />
TM<br />
a<br />
S<br />
a<br />
TM<br />
a<br />
j<br />
S<br />
a<br />
i ρ<br />
φ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
)},<br />
|<br />
|<br />
|<br />
|<br />
1<br />
(<br />
j<br />
TE<br />
j<br />
TE<br />
a<br />
TE<br />
a<br />
S<br />
a<br />
TE<br />
a<br />
i ρ<br />
φ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
∂<br />
∂<br />
+<br />
∂<br />
∂<br />
(C.13)<br />
6<br />
},<br />
,<br />
,<br />
,<br />
{<br />
}<br />
,<br />
,<br />
,<br />
{ θ<br />
θ ∆<br />
⇔ P<br />
S<br />
yy<br />
yx<br />
xy<br />
xx<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z (C.2)<br />
,<br />
)<br />
2<br />
(<br />
2<br />
/<br />
1<br />
2<br />
2<br />
2<br />
2<br />
yx<br />
yy<br />
xy<br />
xx<br />
S<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
+<br />
+<br />
+<br />
= (C.3)<br />
,<br />
)<br />
(<br />
2 2<br />
/<br />
1<br />
2<br />
2<br />
2<br />
2<br />
yx<br />
yy<br />
xy<br />
xx<br />
yy<br />
xx<br />
xy<br />
yx<br />
P<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
+<br />
+<br />
+<br />
−<br />
= (C.4)<br />
),<br />
arctan(<br />
yx<br />
xy<br />
yy<br />
xx<br />
Z<br />
Z<br />
Z<br />
Z<br />
−<br />
+<br />
=<br />
∆θ (C.5)<br />
).<br />
arctan(<br />
2<br />
1<br />
yx<br />
xy<br />
xx<br />
yy<br />
Z<br />
Z<br />
Z<br />
Z<br />
+<br />
−<br />
=<br />
θ (C.6)<br />
),<br />
(<br />
2<br />
1 2<br />
2<br />
2<br />
TE<br />
TM<br />
S<br />
Z<br />
Z<br />
Z +<br />
= (C.7)<br />
).<br />
1<br />
1<br />
(<br />
2<br />
1<br />
1<br />
2<br />
2<br />
2<br />
TE<br />
TM<br />
P<br />
Z<br />
Z<br />
Z<br />
+<br />
= (C.8)<br />
),<br />
(<br />
2<br />
1 TE<br />
a<br />
TM<br />
a<br />
S<br />
a<br />
ρ<br />
ρ<br />
ρ +<br />
= (C.9)<br />
),<br />
(<br />
2<br />
1<br />
j<br />
TE<br />
a<br />
j<br />
TM<br />
a<br />
j<br />
S<br />
a<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
(C.10)<br />
.<br />
|<br />
|<br />
|<br />
|<br />
1<br />
1<br />
j<br />
S<br />
j<br />
S<br />
a<br />
S<br />
a<br />
j<br />
S<br />
a<br />
S<br />
a<br />
i ρ<br />
φ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ ∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
(C.11)<br />
).<br />
1<br />
1<br />
Re(<br />
2<br />
1<br />
|<br />
|<br />
|<br />
|<br />
1<br />
j<br />
TE<br />
a<br />
S<br />
a<br />
j<br />
TM<br />
a<br />
S<br />
a<br />
j<br />
S<br />
a<br />
S<br />
a r ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ ∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
(C.12)<br />
+<br />
∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
)<br />
|<br />
|<br />
|<br />
|<br />
1<br />
(<br />
Re{<br />
2<br />
1<br />
|<br />
|<br />
| j<br />
TM<br />
j<br />
TM<br />
a<br />
TM<br />
a<br />
S<br />
a<br />
TM<br />
a<br />
j<br />
S<br />
a<br />
i ρ<br />
φ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
)},<br />
|<br />
|<br />
|<br />
|<br />
1<br />
(<br />
j<br />
TE<br />
j<br />
TE<br />
a<br />
TE<br />
a<br />
S<br />
a<br />
TE<br />
a<br />
i ρ<br />
φ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
∂<br />
∂<br />
+<br />
∂<br />
∂<br />
(C.13)<br />
6<br />
},<br />
,<br />
,<br />
,<br />
{<br />
}<br />
,<br />
,<br />
,<br />
{ θ<br />
θ ∆<br />
⇔ P<br />
S<br />
yy<br />
yx<br />
xy<br />
xx<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z (C.2)<br />
,<br />
)<br />
2<br />
(<br />
2<br />
/<br />
1<br />
2<br />
2<br />
2<br />
2<br />
yx<br />
yy<br />
xy<br />
xx<br />
S<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
+<br />
+<br />
+<br />
= (C.3)<br />
,<br />
)<br />
(<br />
2 2<br />
/<br />
1<br />
2<br />
2<br />
2<br />
2<br />
yx<br />
yy<br />
xy<br />
xx<br />
yy<br />
xx<br />
xy<br />
yx<br />
P<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
+<br />
+<br />
+<br />
−<br />
= (C.4)<br />
),<br />
arctan(<br />
yx<br />
xy<br />
yy<br />
xx<br />
Z<br />
Z<br />
Z<br />
Z<br />
−<br />
+<br />
=<br />
∆θ (C.5)<br />
).<br />
arctan(<br />
2<br />
1<br />
yx<br />
xy<br />
xx<br />
yy<br />
Z<br />
Z<br />
Z<br />
Z<br />
+<br />
−<br />
=<br />
θ (C.6)<br />
xy<br />
x<br />
),<br />
(<br />
2<br />
1 2<br />
2<br />
2<br />
TE<br />
TM<br />
S<br />
Z<br />
Z<br />
Z +<br />
= (C.7)<br />
).<br />
1<br />
1<br />
(<br />
2<br />
1<br />
1<br />
2<br />
2<br />
2<br />
TE<br />
TM<br />
P<br />
Z<br />
Z<br />
Z<br />
+<br />
= (C.8)<br />
),<br />
(<br />
2<br />
1 TE<br />
a<br />
TM<br />
a<br />
S<br />
a<br />
ρ<br />
ρ<br />
ρ +<br />
= (C.9)<br />
),<br />
(<br />
2<br />
1<br />
j<br />
TE<br />
a<br />
j<br />
TM<br />
a<br />
j<br />
S<br />
a<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
(C.10)<br />
.<br />
|<br />
|<br />
|<br />
|<br />
1<br />
1<br />
j<br />
S<br />
j<br />
S<br />
a<br />
S<br />
a<br />
j<br />
S<br />
a<br />
S<br />
a<br />
i ρ<br />
φ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ ∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
(C.11)<br />
).<br />
1<br />
1<br />
Re(<br />
2<br />
1<br />
|<br />
|<br />
|<br />
|<br />
1<br />
j<br />
TE<br />
a<br />
S<br />
a<br />
j<br />
TM<br />
a<br />
S<br />
a<br />
j<br />
S<br />
a<br />
S<br />
a r ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ ∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
(C.12)<br />
+<br />
∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
)<br />
|<br />
|<br />
|<br />
|<br />
1<br />
(<br />
Re{<br />
2<br />
1<br />
|<br />
|<br />
|<br />
|<br />
1<br />
j<br />
TM<br />
j<br />
TM<br />
a<br />
TM<br />
a<br />
S<br />
a<br />
TM<br />
a<br />
j<br />
S<br />
a<br />
S<br />
a<br />
i ρ<br />
φ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
)},<br />
|<br />
|<br />
|<br />
|<br />
1<br />
(<br />
j<br />
TE<br />
j<br />
TE<br />
a<br />
TE<br />
a<br />
S<br />
a<br />
TE<br />
a<br />
i ρ<br />
φ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
∂<br />
∂<br />
+<br />
∂<br />
∂<br />
(C.13)<br />
6<br />
x<br />
y<br />
},<br />
,<br />
,<br />
,<br />
{<br />
}<br />
,<br />
,<br />
,<br />
{ θ<br />
θ ∆<br />
⇔ P<br />
S<br />
yy<br />
yx<br />
xy<br />
xx<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z (C.2)<br />
,<br />
)<br />
2<br />
(<br />
2<br />
/<br />
1<br />
2<br />
2<br />
2<br />
2<br />
yx<br />
yy<br />
xy<br />
xx<br />
S<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
+<br />
+<br />
+<br />
= (C.3)<br />
,<br />
)<br />
(<br />
2 2<br />
/<br />
1<br />
2<br />
2<br />
2<br />
2<br />
yx<br />
yy<br />
xy<br />
xx<br />
yy<br />
xx<br />
xy<br />
yx<br />
P<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
+<br />
+<br />
+<br />
−<br />
= (C.4)<br />
),<br />
arctan(<br />
yx<br />
xy<br />
yy<br />
xx<br />
Z<br />
Z<br />
Z<br />
Z<br />
−<br />
+<br />
=<br />
∆θ (C.5)<br />
).<br />
arctan(<br />
2<br />
1<br />
yx<br />
xy<br />
xx<br />
yy<br />
Z<br />
Z<br />
Z<br />
Z<br />
+<br />
−<br />
=<br />
θ (C.6)<br />
M xy<br />
Z<br />
=<br />
E yx<br />
Z<br />
=<br />
),<br />
(<br />
2<br />
1 2<br />
2<br />
2<br />
TE<br />
TM<br />
S<br />
Z<br />
Z<br />
Z +<br />
= (C.7)<br />
).<br />
1<br />
1<br />
(<br />
2<br />
1<br />
1<br />
2<br />
2<br />
2<br />
TE<br />
TM<br />
P<br />
Z<br />
Z<br />
Z<br />
+<br />
= (C.8)<br />
S<br />
),<br />
(<br />
2<br />
1 TE<br />
a<br />
TM<br />
a<br />
S<br />
a<br />
ρ<br />
ρ<br />
ρ +<br />
= (C.9)<br />
S<br />
),<br />
(<br />
2<br />
1<br />
j<br />
TE<br />
a<br />
j<br />
TM<br />
a<br />
j<br />
S<br />
a<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
(C.10)<br />
j<br />
.<br />
|<br />
|<br />
|<br />
|<br />
1<br />
1<br />
j<br />
S<br />
j<br />
S<br />
a<br />
S<br />
a<br />
j<br />
S<br />
a<br />
S<br />
a<br />
i ρ<br />
φ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ ∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
(C.11)<br />
).<br />
1<br />
1<br />
Re(<br />
2<br />
1<br />
|<br />
|<br />
|<br />
|<br />
1<br />
j<br />
TE<br />
a<br />
S<br />
a<br />
j<br />
TM<br />
a<br />
S<br />
a<br />
j<br />
S<br />
a<br />
S<br />
a r ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ ∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
(C.12)<br />
TM<br />
TE<br />
a<br />
+<br />
∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
)<br />
|<br />
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1<br />
(<br />
Re{<br />
2<br />
1<br />
|<br />
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1<br />
j<br />
TM<br />
j<br />
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a<br />
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a<br />
S<br />
a<br />
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a<br />
j<br />
S<br />
a<br />
S<br />
a<br />
i ρ<br />
φ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
)},<br />
|<br />
|<br />
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1<br />
(<br />
j<br />
TE<br />
j<br />
TE<br />
a<br />
TE<br />
a<br />
S<br />
a<br />
TE<br />
a<br />
i ρ<br />
φ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
∂<br />
∂<br />
+<br />
∂<br />
∂<br />
(C.13)<br />
6<br />
x<br />
H<br />
y<br />
H<br />
},<br />
,<br />
,<br />
,<br />
{<br />
}<br />
,<br />
,<br />
,<br />
{ θ<br />
θ ∆<br />
⇔ P<br />
S<br />
yy<br />
yx<br />
xy<br />
xx<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z (C.2)<br />
,<br />
)<br />
2<br />
(<br />
2<br />
/<br />
1<br />
2<br />
2<br />
2<br />
2<br />
yx<br />
yy<br />
xy<br />
xx<br />
S<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
+<br />
+<br />
+<br />
= (C.3)<br />
,<br />
)<br />
(<br />
2 2<br />
/<br />
1<br />
2<br />
2<br />
2<br />
2<br />
yx<br />
yy<br />
xy<br />
xx<br />
yy<br />
xx<br />
xy<br />
yx<br />
P<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
+<br />
+<br />
+<br />
−<br />
= (C.4)<br />
),<br />
arctan(<br />
yx<br />
xy<br />
yy<br />
xx<br />
Z<br />
Z<br />
Z<br />
Z<br />
−<br />
+<br />
=<br />
∆θ (C.5)<br />
).<br />
arctan(<br />
2<br />
1<br />
yx<br />
xy<br />
xx<br />
yy<br />
Z<br />
Z<br />
Z<br />
Z<br />
+<br />
−<br />
=<br />
θ (C.6)<br />
TM xy<br />
Z Z<br />
=<br />
TE yx<br />
Z Z<br />
=<br />
S<br />
Z<br />
P<br />
Z<br />
),<br />
(<br />
2<br />
1 2<br />
2<br />
2<br />
TE<br />
TM<br />
S<br />
Z<br />
Z<br />
Z +<br />
= (C.7)<br />
).<br />
1<br />
1<br />
(<br />
2<br />
1<br />
1<br />
2<br />
2<br />
2<br />
TE<br />
TM<br />
P<br />
Z<br />
Z<br />
Z<br />
+<br />
= (C.8)<br />
S<br />
a<br />
ρ<br />
),<br />
(<br />
2<br />
1 TE<br />
a<br />
TM<br />
a<br />
S<br />
a<br />
ρ<br />
ρ<br />
ρ +<br />
= (C.9)<br />
S<br />
a<br />
ρ<br />
),<br />
(<br />
2<br />
1<br />
j<br />
TE<br />
a<br />
j<br />
TM<br />
a<br />
j<br />
S<br />
a<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
(C.10)<br />
j<br />
ρ<br />
.<br />
|<br />
|<br />
|<br />
|<br />
1<br />
1<br />
j<br />
S<br />
j<br />
S<br />
a<br />
S<br />
a<br />
j<br />
S<br />
a<br />
S<br />
a<br />
i ρ<br />
φ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ ∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
(C.11)<br />
).<br />
1<br />
1<br />
Re(<br />
2<br />
1<br />
|<br />
|<br />
|<br />
|<br />
1<br />
j<br />
TE<br />
a<br />
S<br />
a<br />
j<br />
TM<br />
a<br />
S<br />
a<br />
j<br />
S<br />
a<br />
S<br />
a r ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ ∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
(C.12)<br />
TM<br />
a<br />
ρ<br />
TE<br />
a<br />
ρ<br />
+<br />
∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
)<br />
|<br />
|<br />
|<br />
|<br />
1<br />
(<br />
Re{<br />
2<br />
1<br />
|<br />
|<br />
|<br />
|<br />
1<br />
j<br />
TM<br />
j<br />
TM<br />
a<br />
TM<br />
a<br />
S<br />
a<br />
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a<br />
j<br />
S<br />
a<br />
S<br />
a<br />
i ρ<br />
φ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
)},<br />
|<br />
|<br />
|<br />
|<br />
1<br />
(<br />
j<br />
TE<br />
j<br />
TE<br />
a<br />
TE<br />
a<br />
S<br />
a<br />
TE<br />
a<br />
i ρ<br />
φ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
∂<br />
∂<br />
+<br />
∂<br />
∂<br />
(C.13)<br />
6<br />
},<br />
,<br />
,<br />
,<br />
{<br />
}<br />
,<br />
,<br />
,<br />
{ θ<br />
θ ∆<br />
⇔ P<br />
S<br />
yy<br />
yx<br />
xy<br />
xx<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z (C.2)<br />
,<br />
)<br />
2<br />
(<br />
2<br />
/<br />
1<br />
2<br />
2<br />
2<br />
2<br />
yx<br />
yy<br />
xy<br />
xx<br />
S<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
+<br />
+<br />
+<br />
= (C.3)<br />
,<br />
)<br />
(<br />
2 2<br />
/<br />
1<br />
2<br />
2<br />
2<br />
2<br />
yx<br />
yy<br />
xy<br />
xx<br />
yy<br />
xx<br />
xy<br />
yx<br />
P<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
+<br />
+<br />
+<br />
−<br />
= (C.4)<br />
),<br />
arctan(<br />
yx<br />
xy<br />
yy<br />
xx<br />
Z<br />
Z<br />
Z<br />
Z<br />
−<br />
+<br />
=<br />
∆θ (C.5)<br />
).<br />
arctan(<br />
2<br />
1<br />
yx<br />
xy<br />
xx<br />
yy<br />
Z<br />
Z<br />
Z<br />
Z<br />
+<br />
−<br />
=<br />
θ (C.6)<br />
),<br />
(<br />
2<br />
1 2<br />
2<br />
2<br />
TE<br />
TM<br />
S<br />
Z<br />
Z<br />
Z +<br />
= (C.7)<br />
).<br />
1<br />
1<br />
(<br />
2<br />
1<br />
1<br />
2<br />
2<br />
2<br />
TE<br />
TM<br />
P<br />
Z<br />
Z<br />
Z<br />
+<br />
= (C.8)<br />
),<br />
(<br />
2<br />
1 TE<br />
a<br />
TM<br />
a<br />
S<br />
a<br />
ρ<br />
ρ<br />
ρ +<br />
= (C.9)<br />
),<br />
(<br />
2<br />
1<br />
j<br />
TE<br />
a<br />
j<br />
TM<br />
a<br />
j<br />
S<br />
a<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
(C.10)<br />
.<br />
|<br />
|<br />
|<br />
|<br />
1<br />
1<br />
j<br />
S<br />
j<br />
S<br />
a<br />
S<br />
a<br />
j<br />
S<br />
a<br />
S<br />
a<br />
i ρ<br />
φ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ ∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
(C.11)<br />
).<br />
1<br />
1<br />
Re(<br />
2<br />
1<br />
|<br />
|<br />
|<br />
|<br />
1<br />
j<br />
TE<br />
a<br />
S<br />
a<br />
j<br />
TM<br />
a<br />
S<br />
a<br />
j<br />
S<br />
a<br />
S<br />
a r ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ ∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
(C.12)<br />
+<br />
∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
)<br />
|<br />
|<br />
|<br />
|<br />
1<br />
(<br />
Re{<br />
2<br />
1<br />
|<br />
|<br />
| j<br />
TM<br />
j<br />
TM<br />
a<br />
TM<br />
a<br />
S<br />
a<br />
TM<br />
a<br />
j<br />
S<br />
a<br />
i ρ<br />
φ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
)},<br />
|<br />
|<br />
|<br />
|<br />
1<br />
(<br />
j<br />
TE<br />
j<br />
TE<br />
a<br />
TE<br />
a<br />
S<br />
a<br />
TE<br />
a<br />
i ρ<br />
φ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
∂<br />
∂<br />
+<br />
∂<br />
∂<br />
(C.13)<br />
+<br />
∂<br />
∂<br />
−<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
)<br />
|<br />
|<br />
|<br />
(|<br />
|<br />
|<br />
Re{<br />
2<br />
1<br />
|<br />
|<br />
j<br />
TM<br />
j<br />
TM<br />
a<br />
TM<br />
a<br />
S<br />
a<br />
S<br />
a<br />
TM<br />
a<br />
j<br />
S<br />
a<br />
i σ<br />
φ<br />
σ<br />
σ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
σ<br />
σ<br />
)}.<br />
|<br />
|<br />
|<br />
(|<br />
|<br />
| j<br />
TE<br />
j<br />
TE<br />
a<br />
TE<br />
a<br />
S<br />
a<br />
S<br />
a<br />
TE<br />
a<br />
i σ<br />
φ<br />
σ<br />
σ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
∂<br />
∂<br />
−<br />
∂<br />
∂<br />
(C.14)<br />
}.<br />
|<br />
|<br />
|<br />
|<br />
|<br />
|<br />
|<br />
|<br />
Re{<br />
2<br />
1<br />
TE<br />
S<br />
a<br />
S<br />
a<br />
TE<br />
a<br />
TE<br />
a<br />
TM<br />
S<br />
a<br />
S<br />
a<br />
TM<br />
a<br />
TM<br />
a<br />
I<br />
I<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
+ (C.15)<br />
).<br />
(<br />
2<br />
1 TE<br />
a<br />
TM<br />
a<br />
P<br />
a<br />
σ<br />
σ<br />
σ +<br />
= (C.16)<br />
).<br />
(<br />
2<br />
1<br />
j<br />
TE<br />
a<br />
j<br />
TM<br />
a<br />
j<br />
P<br />
a<br />
σ<br />
σ<br />
σ<br />
σ<br />
σ<br />
σ<br />
∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
(C.17)<br />
,<br />
|<br />
|<br />
P<br />
i<br />
P<br />
a<br />
P<br />
a<br />
e φ<br />
σ<br />
σ<br />
−<br />
= (C.18)<br />
.<br />
|<br />
|<br />
|<br />
|<br />
1<br />
1<br />
j<br />
P<br />
j<br />
P<br />
a<br />
P<br />
a<br />
j<br />
P<br />
a<br />
P<br />
a<br />
i σ<br />
φ<br />
σ<br />
σ<br />
σ<br />
σ<br />
σ<br />
σ ∂<br />
∂<br />
−<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
(C.19)<br />
1<br />
1<br />
1<br />
|<br />
|<br />
1<br />
TE<br />
a<br />
TM<br />
a<br />
P<br />
a<br />
σ<br />
σ<br />
σ ∂<br />
∂<br />
∂<br />
+<br />
∂<br />
∂<br />
−<br />
∂<br />
∂<br />
= )<br />
|<br />
|<br />
|<br />
(|<br />
|<br />
|<br />
Re{<br />
2<br />
1<br />
j<br />
TM<br />
j<br />
TM<br />
a<br />
TM<br />
a<br />
S<br />
a<br />
S<br />
a<br />
TM<br />
a<br />
i σ<br />
φ<br />
σ<br />
σ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
)}.<br />
|<br />
|<br />
|<br />
(|<br />
|<br />
| j<br />
TE<br />
j<br />
TE<br />
a<br />
TE<br />
a<br />
S<br />
a<br />
S<br />
a<br />
TE<br />
a<br />
i σ<br />
φ<br />
σ<br />
σ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
∂<br />
∂<br />
−<br />
∂<br />
∂<br />
(C.14)<br />
}.<br />
|<br />
|<br />
|<br />
|<br />
|<br />
|<br />
|<br />
|<br />
Re{<br />
2<br />
1<br />
TE<br />
S<br />
a<br />
S<br />
a<br />
TE<br />
a<br />
TE<br />
a<br />
TM<br />
S<br />
a<br />
S<br />
a<br />
TM<br />
a<br />
TM<br />
a<br />
I<br />
I<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
+ (C.15)<br />
).<br />
(<br />
2<br />
1 TE<br />
a<br />
TM<br />
a<br />
P<br />
a<br />
σ<br />
σ<br />
σ +<br />
= (C.16)<br />
).<br />
(<br />
2<br />
1<br />
j<br />
TE<br />
a<br />
j<br />
TM<br />
a<br />
j<br />
P<br />
a<br />
σ<br />
σ<br />
σ<br />
σ<br />
σ<br />
σ<br />
∂<br />
∂<br />
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Re{<br />
2<br />
1<br />
TE<br />
S<br />
a<br />
S<br />
a<br />
TE<br />
a<br />
TE<br />
a<br />
TM<br />
S<br />
a<br />
S<br />
a<br />
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a<br />
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a<br />
I<br />
I<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
+ (C.15)<br />
).<br />
(<br />
2<br />
1 TE<br />
a<br />
TM<br />
a<br />
P<br />
a<br />
σ<br />
σ<br />
σ +<br />
= (C.16)<br />
).<br />
(<br />
2<br />
1<br />
j<br />
TE<br />
a<br />
j<br />
TM<br />
a<br />
j<br />
P<br />
a<br />
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σ<br />
σ<br />
σ<br />
σ<br />
σ<br />
∂<br />
∂<br />
+<br />
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=<br />
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∂<br />
(C.17)<br />
,<br />
|<br />
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P<br />
i<br />
P<br />
a<br />
P<br />
a<br />
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σ<br />
σ<br />
−<br />
= (C.18)<br />
.<br />
|<br />
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1<br />
1<br />
j<br />
P<br />
j<br />
P<br />
a<br />
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a<br />
j<br />
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P<br />
a<br />
i σ<br />
φ<br />
σ<br />
σ<br />
σ<br />
σ<br />
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σ ∂<br />
∂<br />
−<br />
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=<br />
∂<br />
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(C.19)<br />
).<br />
1<br />
1<br />
Re(<br />
2<br />
1<br />
|<br />
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1<br />
j<br />
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a<br />
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a<br />
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a<br />
j<br />
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a<br />
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a<br />
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σ<br />
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σ<br />
σ<br />
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∂<br />
+<br />
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=<br />
∂<br />
∂<br />
(C.20)<br />
TM<br />
a<br />
σ<br />
TE<br />
a<br />
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+<br />
∂<br />
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−<br />
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)<br />
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1<br />
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2<br />
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φ<br />
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∂<br />
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−<br />
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(C.21)<br />
}.<br />
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2<br />
1 )<br />
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)<br />
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i<br />
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i<br />
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φ<br />
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+ (C.22)<br />
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{σ<br />
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A<br />
(a−term−independent−of−the−model). (D.2)<br />
6<br />
,<br />
)<br />
2<br />
(<br />
2<br />
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1<br />
S<br />
Z = (C.3)<br />
,<br />
)<br />
(<br />
2 2<br />
/<br />
1<br />
2<br />
2<br />
2<br />
2<br />
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yy<br />
xy<br />
xx<br />
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P<br />
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Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
Z<br />
+<br />
+<br />
+<br />
−<br />
= (C.4)<br />
),<br />
arctan(<br />
yx<br />
xy<br />
yy<br />
xx<br />
Z<br />
Z<br />
Z<br />
Z<br />
−<br />
+<br />
=<br />
∆θ (C.5)<br />
).<br />
arctan(<br />
2<br />
1<br />
yx<br />
xy<br />
xx<br />
yy<br />
Z<br />
Z<br />
Z<br />
Z<br />
+<br />
−<br />
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θ (C.6)<br />
TM xy<br />
Z Z<br />
=<br />
TE yx<br />
Z Z<br />
=<br />
S<br />
Z<br />
P<br />
Z<br />
),<br />
(<br />
2<br />
1 2<br />
2<br />
2<br />
TE<br />
TM<br />
S<br />
Z<br />
Z<br />
Z +<br />
= (C.7)<br />
).<br />
1<br />
1<br />
(<br />
2<br />
1<br />
1<br />
2<br />
2<br />
2<br />
TE<br />
TM<br />
P<br />
Z<br />
Z<br />
Z<br />
+<br />
= (C.8)<br />
S<br />
a<br />
ρ<br />
),<br />
(<br />
2<br />
1 TE<br />
a<br />
TM<br />
a<br />
S<br />
a<br />
ρ<br />
ρ<br />
ρ +<br />
= (C.9)<br />
S<br />
a<br />
ρ<br />
),<br />
(<br />
2<br />
1<br />
j<br />
TE<br />
a<br />
j<br />
TM<br />
a<br />
j<br />
S<br />
a<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
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(C.10)<br />
j<br />
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a<br />
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a<br />
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(C.11)<br />
).<br />
1<br />
1<br />
Re(<br />
2<br />
1<br />
|<br />
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1<br />
j<br />
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a<br />
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a<br />
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a<br />
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S<br />
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S<br />
a r ρ<br />
ρ<br />
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ρ ∂<br />
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(C.12)<br />
TM<br />
a<br />
ρ<br />
TE<br />
a<br />
ρ<br />
+<br />
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=<br />
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)<br />
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1<br />
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Re{<br />
2<br />
1<br />
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φ<br />
ρ<br />
ρ<br />
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j<br />
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a<br />
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6<br />
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θ ∆<br />
⇔ P<br />
S Z<br />
Z (C.2)<br />
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2<br />
2<br />
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1<br />
2<br />
2<br />
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yy<br />
y<br />
Z<br />
Z +<br />
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(C.3)<br />
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1<br />
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yy<br />
xy<br />
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xx<br />
xy<br />
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),<br />
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xy<br />
yy<br />
xx<br />
Z<br />
Z<br />
Z<br />
Z<br />
−<br />
+<br />
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).<br />
n(<br />
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xy<br />
xx<br />
yy<br />
Z<br />
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Z<br />
+<br />
−<br />
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),<br />
2<br />
2<br />
TE<br />
TM<br />
Z<br />
+ (C.7)<br />
).<br />
1<br />
1<br />
2<br />
2<br />
TE<br />
TM<br />
Z<br />
+ (C.8)<br />
),<br />
TE<br />
a<br />
TM<br />
a<br />
ρ<br />
+ (C.9)<br />
),<br />
j<br />
TE<br />
a<br />
j<br />
TM<br />
a<br />
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ρ<br />
ρ<br />
ρ<br />
∂<br />
∂<br />
+ (C.10)<br />
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| j<br />
S<br />
j<br />
S<br />
a i ρ<br />
φ<br />
ρ<br />
ρ<br />
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+<br />
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(C.11)<br />
).<br />
1<br />
1<br />
j<br />
TE<br />
a<br />
S<br />
a<br />
j<br />
TM<br />
a<br />
S<br />
a r ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ ∂<br />
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+<br />
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+<br />
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1<br />
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TM<br />
j<br />
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a<br />
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φ<br />
ρ<br />
ρ<br />
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j<br />
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j<br />
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a<br />
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a<br />
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ρ<br />
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(C.13)<br />
6<br />
},<br />
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,<br />
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θ ∆<br />
P<br />
S Z<br />
Z (C.2)<br />
,<br />
) 2<br />
/<br />
1<br />
2<br />
2<br />
yx<br />
yy<br />
Z<br />
Z +<br />
(C.3)<br />
,<br />
) 2<br />
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1<br />
2<br />
2<br />
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yy<br />
yy<br />
xx<br />
y<br />
Z<br />
Z<br />
Z<br />
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+<br />
+<br />
−<br />
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),<br />
yx<br />
xy<br />
yy<br />
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Z<br />
Z<br />
−<br />
+<br />
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).<br />
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xy<br />
xx<br />
yy<br />
Z<br />
Z<br />
+<br />
−<br />
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),<br />
2<br />
TE<br />
Z<br />
+ (C.7)<br />
).<br />
1 2<br />
TE<br />
Z<br />
+ (C.8)<br />
),<br />
TE<br />
a<br />
ρ<br />
+ (C.9)<br />
),<br />
j<br />
TE<br />
a<br />
ρ<br />
ρ<br />
∂<br />
∂<br />
+ (C.10)<br />
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S<br />
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S<br />
a i ρ<br />
φ<br />
ρ<br />
ρ<br />
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∂<br />
+<br />
∂<br />
(C.11)<br />
).<br />
1<br />
j<br />
TE<br />
a<br />
S<br />
a<br />
j<br />
TM<br />
a<br />
r ρ<br />
ρ<br />
ρ<br />
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+<br />
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+<br />
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)<br />
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| j<br />
TM<br />
j<br />
TM<br />
a<br />
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φ<br />
ρ<br />
ρ<br />
)},<br />
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1<br />
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j<br />
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j<br />
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a<br />
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+<br />
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=<br />
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∂<br />
)<br />
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Re{<br />
2<br />
1<br />
|<br />
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j<br />
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a<br />
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a<br />
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a<br />
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a<br />
j<br />
S<br />
a<br />
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φ<br />
σ<br />
σ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
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)}.<br />
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(|<br />
|<br />
| j<br />
TE<br />
j<br />
TE<br />
a<br />
TE<br />
a<br />
S<br />
a<br />
S<br />
a<br />
TE<br />
a<br />
i σ<br />
φ<br />
σ<br />
σ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
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∂<br />
−<br />
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∂<br />
(C.14)<br />
}.<br />
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Re{<br />
2<br />
1<br />
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a<br />
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a<br />
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a<br />
I<br />
I<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
ρ<br />
+ (C.15)<br />
).<br />
(<br />
2<br />
1 TE<br />
a<br />
TM<br />
a<br />
P<br />
a<br />
σ<br />
σ<br />
σ +<br />
= (C.16)<br />
).<br />
(<br />
2<br />
1<br />
j<br />
TE<br />
a<br />
j<br />
TM<br />
a<br />
j<br />
P<br />
a<br />
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σ<br />
σ<br />
σ<br />
σ<br />
σ<br />
∂<br />
∂<br />
+<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
(C.17)<br />
,<br />
|<br />
|<br />
P<br />
i<br />
P<br />
a<br />
P<br />
a<br />
e φ<br />
σ<br />
σ<br />
−<br />
= (C.18)<br />
.<br />
|<br />
|<br />
|<br />
|<br />
1<br />
1<br />
j<br />
P<br />
j<br />
P<br />
a<br />
P<br />
a<br />
j<br />
P<br />
a<br />
P<br />
a<br />
i σ<br />
φ<br />
σ<br />
σ<br />
σ<br />
σ<br />
σ<br />
σ ∂<br />
∂<br />
−<br />
∂<br />
∂<br />
=<br />
∂<br />
∂<br />
(C.19)