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Mathematical Methods for Physicists: A concise introduction - Site Map

Mathematical Methods for Physicists: A concise introduction - Site Map

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FOURIER SERIES AND INTEGRALS<br />

continuously and so the electron would lose energy continuously and it would<br />

spiral into the nucleus after just a fraction of a second. This does not occur.<br />

Furthermore, atoms do not radiate unless excited, and when radiation does<br />

occur its spectrum consists of discrete frequencies rather than the continuum of<br />

frequencies predicted by the classical electromagnetic theory. In 1913 Niels Bohr<br />

(1885±1962) proposed a theory which successfully explained the radiation spectra<br />

of the hydrogen atom. According to Bohr's postulates, an atom can exist in<br />

certain allowed stationary states without radiation. Only when an electron<br />

makes a transition between two allowed stationary states, does it emit or absorb<br />

radiation. The possible stationary states are those in which the angular momentum<br />

of the electron about the nucleus is quantized, that is, mvr ˆ np, where v is<br />

the speed of the electron in the nth orbit and r is its radius. Bohr didn't clearly<br />

describe this quantum condition. De Broglie attempted to explain it by ®tting a<br />

standing wave around the circumference of each orbit. Thus de Broglie proposed<br />

that n ˆ 2r, where is the wavelength associated with the nth orbit. Combining<br />

this with Bohr's quantum condition we immediately obtain<br />

ˆ h<br />

mv ˆ h<br />

p :<br />

De Broglie proposed that any material particle of total energy E and momentum p<br />

is accompanied by a wave whose wavelength is given by ˆ h=p and whose<br />

frequency is given by the Planck <strong>for</strong>mula ˆ E=h. Today we call these waves<br />

de Broglie waves or matter waves. The physical nature of these matter waves was<br />

not clearly described by de Broglie, we shall not ask what these matter waves are ±<br />

this is addressed in most textbooks on quantum mechanics. Let us ask just one<br />

question: what is the (phase) velocity of such a matter wave? If we denote this<br />

velocity by u, then<br />

u ˆ ˆ E<br />

p ˆ 1 q<br />

p 2 c 2 ‡ m 2 0<br />

p<br />

c4<br />

q<br />

ˆ c<br />

<br />

1 ‡…m 0 c=p† 2<br />

ˆ c2<br />

v<br />

!<br />

m<br />

p ˆ 0 v<br />

p<br />

;<br />

1 v 2 =c 2<br />

which shows that <strong>for</strong> a particle with m 0 > 0 the wave velocity u is always greater<br />

than c, the speed of light in a vacuum. Instead of individual waves, de Broglie<br />

suggested that we can think of particles inside a wave packet, synthesized from a<br />

number of individual waves of di€erent frequencies, with the entire packet traveling<br />

with the particle velocity v.<br />

De Broglie's matter wave idea is one of the cornerstones of quantum<br />

mechanics.<br />

178

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