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The Nature of the Cooper Pair - University of Liverpool

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Let us see what <strong>the</strong> wavefunction looks like.<br />

Ψ =<br />

�ω<br />

�D<br />

0<br />

1<br />

ε + ∆<br />

sin kr<br />

It is a function <strong>of</strong> r only, so it is spherically symmetric. It is a<br />

sum <strong>of</strong> many sine functions. <strong>The</strong> coefficient decreases with<br />

energy. When <strong>the</strong> energy ε goes from 0 to ∆, <strong>the</strong> coefficient<br />

decreases from 1/∆ to 1/(2∆).<br />

So we may suppose that <strong>the</strong> terms are only significant in <strong>the</strong><br />

energy range from 0 to ∆. As energy changes, k changes.<br />

When r is large enough, sin kr starts to go out <strong>of</strong> phase for<br />

different wavevectors k.<br />

Superconductivity 21

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