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grand_canonical_expectation_value [2013/10/13 15:14]
nikolaj
grand_canonical_expectation_value [2014/03/21 11:11] (current)
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 ===== Grand canonical expectation value === ===== Grand canonical expectation value ===
-==== Definition ​==== +==== Set ==== 
-| @#88DDEE: $ w $ ... grand canonical weight |+| @#55CCEE: context ​    | @#55CCEE: $ w $ ... grand canonical weight |
  
-| @#FFBB00: $\langle A\rangle:​=\sum_{N=0}^\infty w_N\cdot \langle A_N\rangle_N$ |+| @#FFBB00: definiendum ​| @#FFBB00: $\langle A\rangle:​=\sum_{N=0}^\infty w_N\cdot \langle A_N\rangle_N$ |
  
 The functional $\langle \cdot\rangle_N$ denotes the expectation in the canonical ensamble of particle number $N$. So the grand canonical expectation value $\langle \cdot\rangle$ takes sequences of observables to a real. The functional $\langle \cdot\rangle_N$ denotes the expectation in the canonical ensamble of particle number $N$. So the grand canonical expectation value $\langle \cdot\rangle$ takes sequences of observables to a real.
  
 ==== Discussion ==== ==== Discussion ====
-We adopt the names of observables in canonical ensamble for the grand canonical ensamble. For example, if the internal energy in the canonical ensamble is defined as $U=\langle H\rangle$, then the grand canonical expectation value of the energy is denoted by $U$ as well and if formed from the sequence of Hamiltonians $H_N$.+We adopt the names of observables in canonical ensamble for the grand canonical ensamble. For example, if the internal energy in the canonical ensamble is defined as $U=\langle H\rangle$, then the grand canonical expectation value of the energy is denoted by $U$ as well and if formed from the sequence of all the $N$-particle ​Hamiltonians $H_N$. 
 + 
 +We also extend functions $f$ of classical canonical observables to such sequences. I.e. if $A$ has $A_N$, then $f(A)$ has entries $f(A_N)$.
 ==== Parents ==== ==== Parents ====
-=== Requirements ​===+=== Context ​===
 [[Grand canonical weight]] [[Grand canonical weight]]
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