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Statistics
                             5.2.4 Quasi Particles and Statistics
                             The question as to which statistics should be applied to what is answered
                             by quantum-mechanical considerations. All phenomena occurring in a
                             semiconductor obey quantum mechanics. Often we are not aware of this
                             fact, such as when we are dealing with a macroscopically-sized sample.
                             For special cases, such as on a very small length scale, at very low tem-
                             peratures, or in a coherent light field from a laser, the quantum nature of
                             phenomena is directly observable.  The lattice vibrational amplitudes
                             show discrete changes, the light intensity as well, and the electric current
                             is composed of single charge carriers.


                             This discrete nature of the phenomena is best described by so called
                             quasi-particles. These are nothing else than the single quanta by which
                             the amplitudes of the each observable quantity may increase or decrease
                             by. It is just by way of talking about quantum phenomena that we intro-
                             duce the term “phonon” for the quantum of a lattice vibration, “photon”
                             for the quantum of electromagnetic oscillation, and “electron” or “hole”
                             for quantum moving charged carrier.  The most mechanically intuitive
                             picture is perhaps that of a phonon, which is the coaction of all the indi-
                             vidual ions forming a crystal lattice.

                             In a similar manner as for a photon, we have to imagine an electron in the
                             conduction band of a semiconductor. The picture we obtain is the net
                             result of a composed excitation of the bare free-electron, together with
                             the crystal structure forming the conduction band and the other electrons
                             in the semi-conductor (and of course strictly-speaking many more
                             effects.) It is not the electron as a massive particle that makes it different
                             from a phonon. Rather, it is the kind of interacting subsystems that form
                             the resulting phenomenon. In this light the “-ons”, the quasi-particle fam-
                             ily members, lose their mystery and remain simple descriptions of a phe-
                             nomenon.







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