Abstract
In 1917, Einstein formulated a theory of spontaneous stimulated emission and absorption, based on purely phenomenological considerations [1.1]. His results paved the way for an understanding, in a qualitative way, of the basic ingredients of the atom-radiation interaction, and could be useful for describing the processes of absorption, light scattering by atoms, stimulated emission in a variety of laser and maser systems, etc. This happened after Planck found that the spectral distribution of blackbody radiation could be explained by quantizing the energy [1.2], and Einstein had explained the photoelectric effect [1.3] by postulating the existence of energy packets that were later called photons.
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Reference
A. Einstein, Phys.Z. 18, 121 (1917).
M. Planck, Verh. Deutsch. Phys. Ges. 2, 202 (1900).
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Further Reading
H. Haken, Light Vol 1 ( North-Holland, Amsterdam, 1981 ).
H. Haken, Light Vol 2 ( North-Holland, Amsterdam, 1985 ).
L. Mandel, E. Wolf, Optical Coherence and Quantum Optics ( Cambridge University Press, Cambridge, 1995 ).
P. Meystre, M. Sargent III, Elements of Quantum Optics (Springer, Berlin, Heidelberg, 1993 ).
M. Sargent III, M.O. Scully, W.L. Lamb, Laser Physics ( Addison Wesley, Reading, MA, 1974 ).
M.O. Scully, M.S. Zubairy, Quantum Optics ( Cambridge University Press, Cambridge, 1997 ).
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Orszag, M. (2000). Einstein’s Theory of Atom-Radiation Interaction. In: Quantum Optics. Advanced Texts in Physics. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-662-04114-7_1
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DOI: https://doi.org/10.1007/978-3-662-04114-7_1
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