El Método de la Matrix de Transferencia

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1 El Método de la Matrix de Transferencia
Pedro Pereyra Padilla Area de Física Teórica y Materia Condensada Universidad Autónoma Metropolitana-Azcapotzalco, México D.F. Resumen Presentaremos una introducción al Método de la Matriz de Transferencia (MMT) y algunas aplicaciones en la teoría del transporte electrónico cuántico y en la opto-electrónica

2 El Método de la Matrix de Transferencia
Pedro Pereyra Padilla Area de Física Teórica y Materia Condensada Universidad Autónoma Metropolitana-Azcapotzalco, México D.F. INDICE Introduccíon La Matriz de Transferencia (MT) y su relación con la matriz S La MT de la barrera rectangular y el pozo cuántico. Efecto tunel y cuantización La Teoría de Sistemas Periódicos Fínitos. Estructura de bandas (eigenvalores y eigenfunciones). Aproximación de masa efectiva Semiconductores, dispositivos opto-electrónicos, heteroestructuras, (láseres). Tiempo de tunelaje. Paquetes Gaussianos en superredes ópticas Dinámica del spín en superredes magnéticas Conclusiones

3 Introducción OVERVIEW
1. From about 1930 to 1993, the tunneling time has been a controversial issue, because of polemic theoretical results: superluminal velocities ? (MacColl 1932) Hartman effect (1962). These results (obtained using the phase time) were strongly questioned because of possible conflict with causality and the special relativity. As a consequence, besides the phase time, a number of other TT definitions and formulas appeared in the literature, accompanied by intense debate. 2. Since 1993, experiments have shown evidences of superluminality and the striking Hartman effect. It has been shown also that the phase time description agrees extremely well. Nevertheless, old theoretical approaches remain.

4 This was not accepted because:
Condon 1931 y MacColl 1932 V(x) x a This was not accepted because: Possible violation of Causality Principle Violation of Special Theory of Relativity

5 ji =|ji| eiqi tji = |t| eiqt ji rji
In THE 50’s Eisenbud -Wigner & Bohm introduced the phase time ji =|ji| eiqi V(x) tji = |t| eiqt ji rji t1 t2 x

6 ji =|ji| eiqi tji = |t| eiqt ji rji The phase time q1 q2 q V(x) x1 x2
q1 = k x1 + w t1 q2 = k x2 + w t2 = q1 +qt qt = q2 –q1 qt = k (x2- x1)- w (t2- t1)

7 ji V(x) tji = |t| eiqt ji a rji x growing a the tunneling time t tends to a limiting value

8 other TT definitions and formulas appeared in the literature, accompanied by intense debates.

9 the dwelling time (1960) the Larmor time Baz (1966): the spin precesion with constant frequency w, would allow, in principle, to measure the spin component sx and deduce the time spent B w sx sx V(x) z y x

10 h/l = md/t t = lmd/h V(t) = V0 + V1cos wt
the Buttiker-Landauer time defined as the inverse of the characteristic frequency h/l = md/t t = lmd/h of an oscillating potential V(t) = V0 + V1cos wt The incoming particles interchange energy V(t) E + hn E + hn E E E - hn E - hn d x

11 experiment suggests superluminal velocities !!!

12 [fs] Dt tv t [nm] Dt = 1.47 x s v = 1.7 c

13

14 experiment Phase time ¿¿¿ ?????

15 En el experimento de Steinberg et al
En el experimento de Steinberg et al. utilizaron la estructura H(LH)5 que alterna óxido de titanio (H) con silica (L) lS lH lL Eil Eil kil kil Hil Hil Esl x ksl Hsl nH=2.22 nL=1.41

16 ¿Cómo son nuestras predicciones?
En el experimento de Steinberg et al. utilizaron la estructura H(LH)5 que alterna óxido de titanio (H) con silica (L) lS lH lL Eil Eil kil kil Hil Hil Esl x ksl Hsl nH=2.22 nL=1.41 ¿Cómo son nuestras predicciones?

17 Necesitamos obtener la matriz de transferencia de este sistema
lS lH lL Eil Eil kil kil Hil Hil Esl x ksl Hsl nH nL

18 E1r E2l x H1r k1r k2l H2l q1 q2 E2r E1l k1l x H2r k2r H1l e1, m1 e2, m2, s

19 Con esta información se pueden obtener los coeficientes de Fresnal
E2l x H1r k1r k2l H2l q1 q2 E2r E1l k1l x H2r k2r H1l e1, m1 e2, m2, s Con esta información se pueden obtener los coeficientes de Fresnal

20 E1r E2l x H1r k1r k2l H2l q1 q2 E2r E1l k1l x H2r k2r H1l e1, m1 e2, m2, s

21 ¿Cuál es la matriz de transferencia de la celda unitaria?
… lH lL E4r E1r k1r k4r H4r H1r E1l E4l x x k1l k4l H1l H4l nH=2.22 nL=1.41

22 E4r E1r k1r k4r H4r H1r E1l E4l x x k1l k4l H1l H4l En la superred, la matriz de transferencia de una celda es La matriz de transferencia del sistema completo es

23 bn=b pn-1 pn = Un(ar) an = pn - a* pn-1 … Eil Eil kil Hil kil Hil Esl
x ksl Hsl bn=b pn-1 pn = Un(ar) an = pn - a* pn-1

24 Eil Eil kil Hil kil … Hil Esl x ksl Hsl

25 experiment phase time Dt = s

26

27 Efecto Hartman

28 n1 n2 Cómo es la evolución de un paquete electromagnético Gaussiano?
The purpose is to turn into the fundamental laws of nature, i.e. the Maxwell equations, and let them determine the time evolution of wave packets. We will then see whether the EM wave packet motion is superluminal or not. E S H n1 n2

29 For a given Optical Superlattice (OSL),
we have

30 the space-time evolution of a Gaussian WP depends on lo and on the WP width Dk,

31 we will choose lo in the pbgap and in a resonant region
vg < c vg = c vg > c

32 The formalism To determine the wave packet at any point and time we use the Theory of Finite Periodic Systems (TFPS). For z < 0 For z > L Here aT and bT are matrix elements of the global Superlattice Transfer matrix

33

34 For 0 < z < L Replacing these fields into and integrating, we have the wave packet for any value of z and t. Phys. Rev. Lett, 80 (1998) 2677, Ann. Phys. 320 (2005) 1, Phys. Rev. E 75 (2007)

35 For 0 < z < L Replacing these fields into and integrating, we have the wave packet for any value of z and t. Phys. Rev. Lett, 80 (1998) 2677, Ann. Phys. 320 (2005) 1, Phys. Rev. E 75 (2007)

36 Can we determine exactly how much time needs the electromagnetic wave packet to cross the superlattice? The WP peak touches the OSL at ta = zo /c When it leaves the OSL? tl = ta + t When it returns to -zo or moves to zo +L ? tb = 2 ta + t

37 Superluminal motion The WP peak touches the OSL at ta = z o/c = 27.1 fs If t is the phase time where is at tl = ta + tp ? Where is at tb = 2 ta + t p ?

38 Superluminal motion Where will be the WP if vg is NOT vg = L/tp but vg = c ? Since

39

40 Hartman Effect Does the WP move faster when the number of cells of the OSL increases ? if it will move with vg = c The WP peak will be at the left arrows They are at the positions suggested by Spielmann’s experiment !!!