Theory of Spontaneous-Emission Line Shape in an Ideal Cavity
Theory of Spontaneous-Emission Line Shape in an Ideal Cavity
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DOI:
10.1103/physrevlett.51.550
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发表时间:
1983-08
影响因子:
8.6
通讯作者:
J. Sánchez-Mondragón;N. Narozhny;J. Eberly
中科院分区:
文献类型:
--
作者:
J. Sánchez-Mondragón;N. Narozhny;J. Eberly
A single atom is an ideal" laboratory" in which to study the interactions of matter and radiation. The most fundamentally quantum mechanical of these intereactions is responsible for spontaneous emission. The nature of spontaneous radiation in free space is well known, but this is not the case if the radiating atom is enclosed in a cavity.'Recently Kleppner'has proposed a microwave cavity experiment very far from resonance. He has emphasized the possibility of greatly sup-pressing thespontaneous emission rate of a Bydberg atomwhose preferred (also microwave) transition frequency falls in a spectral region where the cavity mode density is much lower than the free-space density of states. Greatly de-creased natural linewidths are one expected con-sequence.It is not generally realized that a fully quantum mechanical theory of natural linewidth under idealized cavity conditions has never been given. We will mention below theprincipal reasons for this. In this Letter we present what, to the best of our knowledge, are the first fully quantum mechanical predictions about the spectrum of spontaneous emission into a lossless cavity, by an atom with an isolated transition frequency. The atomic transition frequency may be arbitrar-ily near to, or many linewidths away from, a single, similarly isolated, cavity resonance line. We show not only that quantum theory makes strikingly different predictions from the corre-sponding semiclassical (nonquantized electro-magnetic field) theory,