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Case of Parabolic Potential Barrier

In the case of a parabolic potential barrier, the Schrodinger equation to be solved is given by [Pg.6]

It should be noted that the coefficients of the wave running to the right are taken to be -C and -C as in Equation (2.2). By using the asymptotic expressions of Weber functions and the above WKB solutions, the connection between the coefficients [Pg.7]

The coefficients and represent the incoming waves to the potential barrier and the coefficients C f, and C represent the outgoing waves from the barrier. The matrix 5 that connects these sets of coefficients has physical meaning of scattering matrix defined as [Pg.7]

This tunneling scattering matrix can be obtained easily from the above expression of M-matrix as [Pg.7]

The diagonal (off-diagonal) elements of this matrix represent tunneling (reflection) amplitudes. At T Vmax the parameter e is negative [e = - e ] [see Equation (2.17)] and the tunneling probability is given by [Pg.8]


For the case of parabolic potential barriers, the conductivity as a function of temperature is described by the simple expression /52/ ... [Pg.74]


See other pages where Case of Parabolic Potential Barrier is mentioned: [Pg.6]   


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