... = f& & &) = Hence fll = f0 and f2 1 = Next, let Eli = and E2i = so that Ei = 2i Then El, = fr2 and Egs = f2 2 From (1.2.9a)= and Ezs = fO( 2S 2i) = f cos Therefore (1.2.9b), El, = and f2 2 = f co& ... light becomes diffuse in scattering by fog, because the index of refraction of water is quite different from air 6.2 Scattering Cylinder by a Finite Approximation Length Cylinder Using the Infinite ... of m is PnmCx> = mb (4 The first few orders of associated For n = 0, - m)! + my cn Legendre (1.4.38) P”(x) n functions are as follows: = P;(cosq (1.4.39) For n = 1, PI-’ (cos 0) = z sin P;(cosq...
... (-l)mty-mfnl @) p + TZZf,,, B-mfnf (h 44 b Pi, 44 i [ mfnf T mnm’n’ C21) mfn,(&, @) c p + +?;;fn,B-mfnf i [ 10 with ,B = v or h Hence, given the T-matrix elements for F can be computed according ... specify one of the following: (1) (2) (3) fi x E everywhere on S, fi x H everywhere on S, fi x E on a part of S and ti x H on the rest of S Thus one cannot specify both fi x E and fi x H on S For ... T-Matrix 83 a12 = cosycospsina a13 = + sinycosar (2.6.5~) -cosysinp a21 = - sinycospcosa a22 = - sinycospsina a32 a33 = - cosysina + cosycosck (2.6.5d) (2.6.5e) (2.6. 5f) = sinysinp = sinpcosa = sinpsina...
... Rf (xl, x2) We first calculate the correlation function of f( xr) (f (Xl >f' (X2>> = lim c-0 (f (Xl >f + - f (Xl >f (x2)) (x2 (21, x2 Rf (21~x2) - aRfk’ + ~> - E E +0 where c is an infinitesimal (f ... = exp (J &f + 2Cq&lkz zl and 22 (4.6.6) + &;) I Correlation Function The correlation defined as function of the random Rf(xl, x2) = process of surface height f( z) is (4.6.7) (f (5l )f( x2)) It ... f( x), f (x) corresponds to the slope function In the following, we will derive the correlation function of slope Rf+a, x2> Rf'(Xl, x2) = (4.6.12) (f (Xl )f (X2>) in terms of the correlation function...
... dielectric constant of Zaneis loam soil at temperature of 295 K as a function of frequency for moisture content of 5% and 30% There is only a small change in the dielectric constant as a function of frequency ... characteristics of microwave emission from soils, we first study the soil of uniform profile with temperature of 295 K In Fig 5.4.4, the brightness temperature is plotted as a function of moisture content ... 10” I 10’ Frequency 10’ @Hz) Figure 5.3.3 Comparison of brightness temperature between coherent and incoherent models for continuous as a function of observation change profile angle frequency...
... the Fourier transform of g (F) - and is known as the structure factor [McQuarrie, 1976; Ziman, 1979; Hansen and McDonald, 19861: 00 & [g (F) - l]P s 42 = Fcos Oil - k cos OS1+ k cos Oi2 + k cos ... product of the coherent field and a complex conjugate of the coherent field by using (6.1.10) We also let - q = ;F, + ?;l = 27~ for the second term Integrating over s d5;A gives V Thus -i;j ;Fj 236 ... scattered at (6.1.3) field is N eiki lFj lls=cf I j=l (6.1.4) ;F- Fj( In the far-field observation direction of rZ-,where h k s= kk s = k sin 8, COS’~,? + k sin 8, sin +& + k cos &ii = k,,$ + keel...
... Phase Matrix -Im (f& fVV) Re (f, *hfVv) Im(fhvf;h) Re (f; hfhv) Re(fvvf;h + fvhflv) -Im(fvvf;h Im(fvvf;h + fvhftv) Re(fvvf;h - fvhfiv) fvhfiv) (7.2.16) Because of the incoherent addition of Stokes parameters, ... terms of forward scattering 27mo E@,$) = j$ -(RelM,, 2Im( -Re( Im(.fvh) fhh) 2Im( fvh) -2Re(fvh) Im(.fhv) fuh) Re(fh,) Im( f v v + fhh) Re(fhh - fvv) 1 -I- ReMhh) (7.2.38a) amplitudes, 2Im( fvv) ... (1 _ TRANSFER THEORY specific intensity padsecO) Tpcadsec8 x2 (7.1.24) The first term is the emission of a layer of thickness d with absorption coefficient K~ The second term is the downward emission...
... (8.1.102) accounts for the differential solid angle The results of copolarized return, depolarized return, degree of polarization, and the phase differences are illustrated for first order and second-order ... solution for C -C - for (8.1.26) by (8.1.24) I 6; 7~- 7d%>cos e-~ ed(sece+sm 0.) a )F, (COS e + cosei) e-lc,d(sece+sec&) - f( k)fiP(e, 4; &6i> COSh Ke(~~~ ei - cos e) COS&P(r0, h> + r(e)r(&)FO K,(~~~ ... k / Figure 8.2.1 where ki, Thermal b.4 emission of half-space of laminar denotes the real part of kl, iYkrz AIs = - lm 2cos8 structure For vertical polarization cos2 28 + 41c’;2,lf cos2 [ cos2...
... LIỆU THAM KHẢO [1] Nguyen Thanh Tien, Le Tuan, Doan Nhat Quang Quantum confinement in Gaussian heavily-doped ZnO surface quantum well, Communication in Physics, (2008) [2] Doan Nhat Quang, Le Tuan, ... of Al-doped ZnMgO Alloy Films for Modulation-doped ZnO/ZnMgO Heterostructures, Japanese Journal of Applied Physics, 44, 3822, (2005) [8] T Ando, Self-Consistent Results for a GaAs/AlxGa1-xAs Heterojunction ... Thanh Tien, Electron scattering from roughnessinduced fluctuations in the donor density in ZnO surface quantum well, Journal of Applied Physics, 107, 123709, (2010) [3] Doan Nhat Quang, Nguyen Huyen...
... lượng thu để khoảng cách 1cm phút tương đương với lượng mà bạn thu để khoảng cách 1m thời gian tu n, hiệu thu lại hoàn toàn khác nhau, sóngđiệntừ hoàn toàn Không nên tiếp xúc gần với sóngđiện ... khoảng từ 250 - 350 tên họ lựa chọn, số thường có số ứng cử viên nhận nhiều đề cử Tháng - tháng 5: Tham khảo ý kiến chuyên gia Hội đồng Nobel gửi tên ứng cử viên ban đầu đến chuyên gia định đặc biệt...