In theoretical physics, path-ordering is the procedure (or a meta-operator P {\displaystyle {\mathcal {P}}} ) that orders a product of operators according to the value of a chosen parameter:
P { O 1 ( σ 1 ) O 2 ( σ 2 ) ⋯ O N ( σ N ) } ≡ O p 1 ( σ p 1 ) O p 2 ( σ p 2 ) ⋯ O p N ( σ p N ) . {\displaystyle {\mathcal {P}}\left\{O_{1}(\sigma _{1})O_{2}(\sigma _{2})\cdots O_{N}(\sigma _{N})\right\}\equiv O_{p_{1}}(\sigma _{p_{1}})O_{p_{2}}(\sigma _{p_{2}})\cdots O_{p_{N}}(\sigma _{p_{N}}).}
Here p is a permutation that orders the parameters by value:
p : { 1 , 2 , … , N } → { 1 , 2 , … , N } {\displaystyle p:\{1,2,\dots ,N\}\to \{1,2,\dots ,N\}}
σ p 1 ≤ σ p 2 ≤ ⋯ ≤ σ p N . {\displaystyle \sigma _{p_{1}}\leq \sigma _{p_{2}}\leq \cdots \leq \sigma _{p_{N}}.}
For example:
P { O 1 ( 4 ) O 2 ( 2 ) O 3 ( 3 ) O 4 ( 1 ) } = O 4 ( 1 ) O 2 ( 2 ) O 3 ( 3 ) O 1 ( 4 ) . {\displaystyle {\mathcal {P}}\left\{O_{1}(4)O_{2}(2)O_{3}(3)O_{4}(1)\right\}=O_{4}(1)O_{2}(2)O_{3}(3)O_{1}(4).}
In many fields of physics, the most common type of path-ordering is time-ordering, which is discussed in detail below.
Examples If an operator is not simply expressed as a product, but as a function of another operator, we must first perform a Taylor expansion of this function. This is the case of the Wilson loop, which is defined as a path-ordered exponential to guarantee that the Wilson loop encodes the holonomy of the gauge connection. The parameter σ that determines the ordering is a parameter describing the contour, and because the contour is closed, the Wilson loop must be defined as a trace in order to be gauge-invariant.
Time ordering In quantum field theory it is useful to take the time-ordered product of operators. This operation is denoted by T {\displaystyle {\mathcal {T}}} . (Although T {\displaystyle {\mathcal {T}}} is often called the "time-ordering operator", strictly speaking it is neither an operator on states nor a superoperator on operators.) For two operators A(x) and B(y) that depend on spacetime locations x and y we define:
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