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Mathematical Methods for Physicists: A concise introduction - Site Map

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WAVE PACKETS AND GROUP VELOCITY<br />

If we further increase the absolute value of z, the function sin (z†=z runs alternately<br />

through maxima and minima, the function values of which are small compared<br />

with the principal maximum at z ˆ 0, and quickly converges to zero.<br />

There<strong>for</strong>e, we can conclude that superposition generates a wave packet whose<br />

amplitude is non-zero only in a ®nite region, and is described by sin (z†=z (see Fig.<br />

4.19).<br />

The modulating factor sin (z†=z of the amplitude assumes the maximum value 1<br />

as z ! 0. Recall that z ˆ k…x ! 0 t), thus <strong>for</strong> z ˆ 0, we have<br />

x ! 0 t ˆ 0;<br />

which means that the maximum of the amplitude is a plane propagating with<br />

velocity<br />

dx<br />

dt ˆ ! 0 ˆ d!<br />

dk ;<br />

0<br />

that is, ! 0 is the group velocity, the velocity of the whole wave packet.<br />

The concept of a wave packet also plays an important role in quantum<br />

mechanics. The idea of associating a wave-like property with the electron and<br />

other material particles was ®rst proposed by Louis Victor de Broglie (1892±1987)<br />

in 1925. His work was motivated by the mystery of the Bohr orbits. After<br />

Ruther<strong>for</strong>d's successful -particle scattering experiments, a planetary-type<br />

nuclear atom, with electrons orbiting around the nucleus, was in favor with<br />

most physicists. But, according to classical electromagnetic theory, a charge<br />

undergoing continuous centripetal acceleration emits electromagnetic radiation<br />

Figure 4.19.<br />

A wave packet.<br />

177

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