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advanced_notions:observable [2017/11/19 06:42]
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 <tabbox Researcher> ​ <tabbox Researcher> ​
  
-In the path integral approach to gauge theory, observables are gauge invariant functions on the space $A$ of a $G$-connections on $E$, where $G$ denotes the structure group and $E$ the fiber bundle. Therefore, an observable $f$ is a function on the space $A/G$, of connections modulo gauge transformations.+In the path integral approach to gauge theory, observables are gauge invariant functions on the space $\mathcal ​A$ of a $G$-connections on $E$, where $G$ denotes the structure group and $E$ the fiber bundle. Therefore, an observable $f$ is a function on the space $\mathcal ​A / \mathcal ​G$, of connections modulo gauge transformations.
  
-As a result, vacuum expectation values are no longer defined as integrals with Lebesgue measure $A$, but instead with a Lebesgue measure on $A/G$. We obtain this measure by pushing forward the Lebesgue measure on $A$ by the map $A \to A/G$ that sends each connection to its gauge equivalence class, and then A$ denotes a gauge equivalence class of connections in the integral.+As a result, vacuum expectation values are no longer defined as integrals with Lebesgue measure $ \mathcal ​A$, but instead with a Lebesgue measure on $ \mathcal ​A/ \mathcal ​G$. We obtain this measure by pushing forward the Lebesgue measure on $ \mathcal ​A$ by the map  \mathcal ​A \to \mathcal ​A/ \mathcal ​G$ that sends each connection to its gauge equivalence class, and then A$ denotes a gauge equivalence class of connections in the integral.
  
 The simplest example of an observable in gauge theory are Wilson loops. ​ The simplest example of an observable in gauge theory are Wilson loops. ​
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 +Take note that this procedure of modding out $\mathcal G$ from $\mathcal A$ is what leads to [[advanced_notions:​quantum_field_theory:​ghosts|Ghosts]]. To do this properly requires to make use of the [[advanced_tools:​gauge_symmetry:​brst|BRST]] formalism. ​
 (Source: Baez, Munian; Gauge Fields, Knots and Gravity, page 342) (Source: Baez, Munian; Gauge Fields, Knots and Gravity, page 342)
  
advanced_notions/observable.1511070136.txt.gz · Last modified: 2017/12/04 08:01 (external edit)