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Systems and Ensembles
                             systems as they are found in microsystem devices: photons, electrons and
                             holes, quasiparticles. We end the chapter with applications of the statisti-
                             cal results, and show how they characterize the particles and quasiparti-
                             cles that we encounter in describing the behavior of semiconductor-based
                             devices.


                             5.1.1 Microcanonical Ensemble
                             An isolated system   (see Figure 5.1a) in equilibrium, with a fixed num-
                                            A

                                                                a)
                               System      Environment               Microcanonical

                                 S              E                  S              E

                                     Exchange





                             b)                                c)
                                     Canonical                      Grand canonical

                                 S              E                  S              E

                                       Heat                      Heat, particles (mass), …
                Figure 5.1. Characterization of systems according to the way they interact with the envi-
                ronment.



                             ber  N   of components, which resides in a fixed volume  , assumes dif-
                                                                          V
                             ferent microscopic implementations in the small energy interval
                             E <  E <  E +  δE  . The index   counts the different implementations. A
                                                     i
                                  i
                             large number of identical such systems  A   is called a microcanonical
                             ensemble. An implementation   is characterized by its energy  E   and a
                                                      i
                                                                                 i
                             detailed description of the state of each of the  N   subsystems. We can
                             think of the   components as particles. Each particle   then has a given
                                                                        j
                                       N
                             vector momentum  p   and vector position  q  ; each vector in turn has
                                              j                   j
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