Page 178 - Semiconductor For Micro- and Nanotechnology An Introduction For Engineers
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Systems and Ensembles
                                   A
                             system  . This average energy is the first moment of the probability dis-
                             tribution  E =  Σ E P(  )  .  The factor  β  , which we can also write as
                                          i  i  i
                             β =  ( k T)  – 1  , is the inverse of the thermal energy. Here   is the temper-
                                                                          T
                                   B
                             ature and k   is the Boltzmann constant. Note that the sum in the denom-
                                      B
                             inator of (5.11) accounts for the normalization of P  . Equation (5.11) is
                                                                       i
                             called the canonical probability distribution.
                Average      If we write Z =  k ∑  exp  – (  βE )   for the denominator of (5.11), then the
                                                      k
                Energy       average energy is given by
                                                      ∂
                                                    1 Z     ∂ lnZ
                                               E =  – --------- =  – -----------  (5.12)
                                                    Z β      ∂ β
                                                      ∂
                                    Z
                Canonical    We call   the canonical partition function. Suppose that we know the
                Partition    total number of particles for a specific implementation   to be the sum
                                                                          k
                Function
                             N =  Σ n  , where n i   is the number of particles with energy E i   such that
                                   i i
                              k
                             E =  Σ n E i   holds. Then we may write the partition function as
                              k
                                   i i
                                Z =  ∑  exp  – (  βΣ n E[  i i  i k    i i  N k   (5.13)
                                                    ] ), with the constraint  Σ n =
                                     k
                                                                               k
                Average      The bracket Σ n E[  ]   denotes one specific implementation   of  E  .
                                          i i  i k                                   k
                Number of    This gives us direct access to the average number of particles n j   in a spe-
                Particles
                                     j
                             cific state  . For a canonical distribution this is given by
                                      ∑  n exp  – (  βΣ n E ] )
                                                 [
                                          j
                                                   i i
                                                       i k
                                                              1 ∂
                                                                         ∂
                                                                  Z
                                       k
                                 n =  --------------------------------------------------------- =  – --------------- =  – 1  lnZ  (5.14)
                                                                       ----------------
                                                                         ∂
                                                                ∂
                                   j                          βZ E     β E
                                       ∑  exp  – (  βΣ n E ] )     j        j
                                                [
                                                      i k
                                                  i i
                                        k
                Sum Over     The canonical partition function   is sometimes also called the sum over
                                                       Z
                States       states.  We have already seen that  Z   is a central term in statistical
                             mechanics, from which many other system properties may be derived.
                                                                                 A
                             Let us consider the energies of all realizations   that the system   may
                                                                   k
                             assume for a small energy interval  EE +,[  δE]  . In this case the probabil-
                                        A
                             ity of finding   with the energy   is given by the sum over all imple-
                                                        E
                             mentations k
                             Semiconductors for Micro and Nanosystem Technology    175
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