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Tunneling

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4<br />

Substituting, we can calculate the transmission coefficient T,<br />

T = S tr<br />

S in<br />

= v trψ * tr ψ tr<br />

v in ψ * in ψ in<br />

=<br />

T = F A<br />

k 1<br />

m F * e−ik 1x Fe<br />

ik 1 x<br />

k 1<br />

m A * e−ik 1 x Ae ik 1 x<br />

2<br />

.<br />

Using the relations obtained from matching the wavefunctions and first derivatives at the boundaries, the ratio of<br />

F/A may be determined. For this system, the transmission coefficient is<br />

€<br />

T = F A<br />

2<br />

,<br />

or T =<br />

1 +<br />

1<br />

sinh 2 .<br />

( k 2 L)<br />

4E ⎛⎛<br />

1 − E ⎞⎞<br />

⎜⎜ ⎟⎟<br />

V 0 ⎝⎝ V 0 ⎠⎠<br />

In this equation, the function sinh is the hyperbolic sine function. It is defined<br />

€<br />

sinhbx = ebx − e −bx<br />

.<br />

2<br />

Though not appearing in this expression, the hyperbolic cosine function, cosh, is defined in a similar fashion,<br />

€<br />

coshbx = ebx + e −bx<br />

.<br />

2<br />

For values of the energy less than V 0 , the transmission coefficient only gets large for energies close to the top of the<br />

barrier, as illustrated in Figure 5.<br />

€<br />

€<br />

0.020<br />

0.018<br />

T<br />

0.016<br />

0.014<br />

0.012<br />

0.010<br />

0.008<br />

0.006<br />

0.004<br />

0.002<br />

0.000<br />

0.0 0.2 0.4 0.6 0.8 1.0 1.2<br />

E/V 0<br />

Figure 5. Transmission coefficient for a particle tunneling through a finite barrier in one dimension.

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