Project 5: Difference between revisions

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==Part I for both PHYS460 and PHYS660 students: Quantum tunneling of spinless wave packets==
==Part I for both PHYS460 and PHYS660 students: Quantum tunneling of spinless wave packets==
By numerically solving the time-dependent Schrödinger equation in one spatial dimension,
By numerically solving the time-dependent Schrödinger equation  


<math> -\frac{\hbar^2}{2m} \frac{\partial^2 \Psi}{\partial x^2} + V(x) \Psi(x) = i\hbar \frac{\partial \Psi}{\partial t} </math>
<math> -\frac{\hbar^2}{2m} \frac{\partial^2 \Psi}{\partial x^2} + V(x) \Psi(x) = i\hbar \frac{\partial \Psi}{\partial t} </math>


study reflection and transmission of a quantum wave packet from a barrier for which the potential energy is greater than the kinetic energy of the incident wave packet.
via the Crank-Nicholson algorithm for partial-differential equations in one spatial dimension, study reflection and transmission of a quantum wave packet from a barrier for which the potential energy is greater than the kinetic energy of the incident wave packet. For computer simulation the units should be chosen as <math> m=1 </math>  and <math> \hbar=1 </math>.
 
Take the incident wave packet to be of the form
 
<math> \Psi(x,t=0) = \frac{1}{(2 \pi)^{1/4} \sqrt{\sigma}} e^{-(x-x_0)^2/4\sigma^2}e^{ik_0(x-x_0)} </math>


==Part II for PHYS660 students only: Spin dynamics of spin-polarized wave packet in Rashba quantum wires==
==Part II for PHYS660 students only: Spin dynamics of spin-polarized wave packet in Rashba quantum wires==

Revision as of 19:45, 16 April 2012

Propagation of Quantum Wave Packets in One and Two Dimensions

Introduction

This project explores tunneling of quantum wave packets in one dimension through a single potential barrier or a double barrier structure where resonant tunneling can be observed at special energies. In quasi-one-dimensional wire with the spin-orbit coupling one can observe spin precession and spin decoherence studied in current research on spintronics [1].

Part I for both PHYS460 and PHYS660 students: Quantum tunneling of spinless wave packets

By numerically solving the time-dependent Schrödinger equation

via the Crank-Nicholson algorithm for partial-differential equations in one spatial dimension, study reflection and transmission of a quantum wave packet from a barrier for which the potential energy is greater than the kinetic energy of the incident wave packet. For computer simulation the units should be chosen as and .

Take the incident wave packet to be of the form

Part II for PHYS660 students only: Spin dynamics of spin-polarized wave packet in Rashba quantum wires

References

  • [1] D. D. Awschalom and M. E. Flatté, Challenges for semiconductor spintronics, Nature Physics 3, 153 (2007).
  • [2] B. K. Nikolić, L. P. Zarbo, and S. Welack, Transverse spin-orbit force in the spin Hall effect in ballistic quantum wires, Phys. Rev. B 72, 075335 (2005).[PDF]
  • [3] B. K. Nikolić, L. P. Zarbo, and S. Souma, Spin currents in semiconductor nanostructures: A nonequilibrium Green function approach, Chapter 24, page 814-866 in Volume I of The Oxford Handbook of Nanoscience and Technology: Frontiers and Advances, edited by A. V. Narlikar and Y. Y. Fu (Oxford University Press, Oxford, 2010); also available as arXiv:0907.4122.
  • [4] S. A. Crooker and D. L. Smith, Imaging spin flows in semiconductors subject to electric, magnetic, and strain fields, Phys. Rev. Lett. 94, 236601 (2005). [PDF]