SEMICONDUCTOR SIMULATIONS USING A COUPLED QUANTUM DRIFT-DIFFUSION SCHRÖDINGER-POISSON MODEL

A coupled quantum drift-diffusion Schrödinger-Poisson model for stationary resonant tunneling simulations in one space dimension is proposed. In the ballistic quantum zone with the resonant quantum barriers, the Schrödinger equation is solved. Near the contacts, where collisional effects are assumed to be important, the quantum drift-diffusion model is employed. The quantum drift-diffusion model have been derived by a quantum moment method from a collisional Wigner equation by Degond et al. The derivation yields an O(~) approximation of the Wigner function which is used as the “alimentation function” in the mixed-state formula for the electron and current densities at the interface. The coupling of the two models is realized by assuming the continuity of the electron and current densities at the interface points. Current-voltage characteristics of a one-dimensional tunneling diode are numerically computed. The results are compared to those from the three models: quantum drift-diffusion equations, Schrödinger-Poisson system, and the coupled drift-diffusion Schrödinger-Poisson equations.

[1]  Ansgar Jüngel,et al.  Quasi-hydrodynamic Semiconductor Equations , 2001 .

[2]  Takao Waho Resonant-Tunneling Diode and its Application to Multi-GHz Analog-to-Digital Converters , 2003 .

[3]  Ferry,et al.  Self-consistent study of the resonant-tunneling diode. , 1989, Physical review. B, Condensed matter.

[4]  Miller,et al.  Simulation of quantum transport in memory-switching double-barrier quantum-well diodes. , 1994, Physical review. B, Condensed matter.

[5]  Carl L. Gardner,et al.  The Quantum Hydrodynamic Model for Semiconductor Devices , 1994, SIAM J. Appl. Math..

[6]  Ansgar Jüngel,et al.  A Positivity-Preserving Numerical Scheme for a Nonlinear Fourth Order Parabolic System , 2001, SIAM J. Numer. Anal..

[7]  Naoufel Ben Abdallah,et al.  A Hybrid Kinetic-Quantum Model for Stationary Electron Transport , 1998 .

[8]  Paul Kutler,et al.  Simulation of Ultra-Small Electronic Devices: The Classical-Quantum Transition Region , 1997 .

[9]  Andrea L. Lacaita,et al.  Quantum-corrected drift-diffusion models for transport in semiconductor devices , 2005 .

[10]  William R. Frensley,et al.  Boundary conditions for open quantum systems driven far from equilibrium , 1990 .

[11]  Pierre Degond,et al.  Quantum Energy-Transport and Drift-Diffusion Models , 2005 .

[12]  Pierre Degond,et al.  Quantum Moment Hydrodynamics and the Entropy Principle , 2003 .

[13]  Zhou,et al.  Form of the quantum potential for use in hydrodynamic equations for semiconductor device modeling. , 1993, Physical review. B, Condensed matter.

[14]  Pierre Degond,et al.  A 1D coupled Schrödinger drift-diffusion model including collisions , 2005 .

[15]  Craig S. Lent,et al.  The quantum transmitting boundary method , 1990 .

[16]  Pierre Degond,et al.  Quantum Hydrodynamic models derived from the entropy principle , 2003 .

[17]  Bernardo Cockburn,et al.  Quantum hydrodynamic simulation of hysteresis in the resonant tunneling diode at 300 K , 1995, Journal of Computational Electronics.

[18]  Nicolas Vauchelet,et al.  Analysis of a Drift-Diffusion-Schrödinger–Poisson model , 2002 .

[19]  G. Iafrate,et al.  Quantum correction to the equation of state of an electron gas in a semiconductor. , 1989, Physical review. B, Condensed matter.

[20]  Pierre Degond,et al.  Coupling one-dimensional time-dependent classical and quantum transport models , 2002 .

[21]  Olivier Pinaud,et al.  Transient simulations of a resonant tunneling diode , 2002 .

[22]  Hans-Christoph Kaiser,et al.  A QUANTUM TRANSMITTING SCHRÖDINGER–POISSON SYSTEM , 2004 .

[23]  A. Wettstein Quantum effects in MOS devices , 2000 .