Nonlinear feedback oscillations in resonant tunneling through double barriers
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a r X i v :c o n d -m a t /9709016v 1 [c o n d -m a t .m e s -h a l l ] 1 S e p 1997NONLINEAR FEEDBACK OSCILLATIONS
IN RESONANT TUNNELING THROUGH DOUBLE BARRIERS
C.Presilla Scuola del Dottorato di Ricerca in Fisica dell’Universit´a “La Sapienza”,Roma,I 00185and Dipartimento di Fisica dell’Universit´a ,Perugia,I 06100G.Jona-Lasinio Dipartimento di Fisica dell’Universit´a “La Sapienza”,Roma,I 00185and F.Capasso AT&T Bell Laboratories,600Mountain avenue,Murray Hill,N J 07974Abstract We analyze the dynamical evolution of the resonant tunneling of an ensemble of electrons through a double barrier in the presence of the self-consistent potential created by the charge accumulation in the well.The intrinsic nonlinearity of the transmission process is shown to lead to oscillations of the stored charge and of the transmitted and re-flected fluxes.The dependence on the electrostatic feedback induced by the self-consistent
potential and on the energy width of the incident distribution is discussed.
P.A.C.S.numbers:03.65.-w,73.40Gk
In recent years there has been renewed interest in the phenomenon of resonant tunneling(RT)through double barriers.The unique capabilities of molecular beam epitaxy make it possible to investigate fundamental questions on RT through simple man-made potentials by controlling the barrier and well parameters(e.g.height,thickness or barrier phase area)down to the atomic scale[1].
In this paper we investigate the dynamics of RT of ballistic electrons in the presence of the potential created by the charge trapped within the barriers[2].This problem is interesting not only from a technological point of view but also as a test of quantum mechanical non-equilibrium situations in which many particles are involved.
The model we propose tries to describe the following situation.A bunch of elec-trons is created within a contact layer and launched towards embedded semiconductor layers forming a double barrier potential.The charge dynamically trapped by the reso-nance will produce a reactionfield which modifies the time evolution of the system.An exact treatment of such a problem looks very complicated.We assume a decoupling be-tween the longitudinal(in the direction x of motion perpendicular to the double barrier) and transversal degrees of freedom.This is a common assumption in treating tunneling phenomena.It makes the problem one-dimensional and allows the following factorization of the wave function:
Ψ(x1,x2,...,x N;t)=Φ(x1,x2,...,x N;t)Ω(y1,z1,y2,z2,...,y N,z N;t)(1)
where x≡x,y,z are the coordinates of each electron and t the time.We remark that antisymmetry ofΨis established if we take,for example,Φsymmetric andΩantisymmetric in their arguments.The experimental set-up we have in mind puts ideally all the electrons in the same high-energy longitudinal state while the transversal degrees of freedom are