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advanced_tools:expectation_values [2017/05/12 14:24]
jakobadmin created
advanced_tools:expectation_values [2017/11/05 16:13] (current)
jakobadmin ↷ Page moved from advanced_notions:expectation_values to advanced_tools:expectation_values
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 function'​) function'​)
 $$ G(r)=\langle \psi(0) \psi(r)\rangle $$ $$ G(r)=\langle \psi(0) \psi(r)\rangle $$
-where the angular brackets ​$$ \langle \cdot \rangle$ denote a statistical average over the thermal fluctuations that characterize all equilibrium systems at nonzero temperature. (Also understood, when $\psi(r)$ is an operator, are the corresponding quantum-mechanical+where the angular brackets $ \langle \cdot \rangle$ denote a statistical average over the thermal fluctuations that characterize all equilibrium systems at nonzero temperature. (Also understood, when $\psi(r)$ is an operator, are the corresponding quantum-mechanical
 expectation values.) expectation values.)
 Physically, $G(r)$ is important since it provides a direct measure of the influence of Physically, $G(r)$ is important since it provides a direct measure of the influence of
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 $$ G(r) \approx D/​d^{d-2+\eta} $$ $$ G(r) \approx D/​d^{d-2+\eta} $$
 as $r \to \infty$ as $r \to \infty$
-which is characterized by the critical exponent ​(or critical index) $d - 2 + \eta$.+which is characterized by the [[advanced_notions:​critical_exponent]] ​(or critical index) $d - 2 + \eta$.
  
 <​cite>​Michael Fisher in Conceptual Foundations of Quantum Field Theory, Edited by Cao</​cite>​ <​cite>​Michael Fisher in Conceptual Foundations of Quantum Field Theory, Edited by Cao</​cite>​
advanced_tools/expectation_values.1494591855.txt.gz · Last modified: 2017/12/04 08:01 (external edit)