This shows you the differences between two versions of the page.
Next revision | Previous revision | ||
advanced_notions:observable [2017/11/19 06:42] jakobadmin created |
advanced_notions:observable [2018/01/02 14:13] (current) jakobadmin ↷ Links adapted because of a move operation |
||
---|---|---|---|
Line 17: | Line 17: | ||
<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. | ||
+ | |||
+ | 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) | ||