- published: 18 Jun 2014
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In physics, an operator is a function acting on the space of physical states. As a result of its application on a physical state, another physical state is obtained, very often along with some extra relevant information.
The simplest example of the utility of operators is the study of symmetry. Because of this, they are a very useful tool in classical mechanics. In quantum mechanics, on the other hand, they are an intrinsic part of the formulation of the theory.
Let us consider a classical mechanics system led by a certain Hamiltonian Failed to parse (Missing texvc executable; please see math/README to configure.): H(q,p) , function of the generalized coordinates Failed to parse (Missing texvc executable; please see math/README to configure.): q
this function to be invariant under the action of a certain group of transformations Failed to parse (Missing texvc executable; please see math/README to configure.): G , i.e., if Failed to parse (Missing texvc executable; please see math/README to configure.): S\in G, H(S(q,p))=H(q,p) . The elements of Failed to parse (Missing texvc executable; please see math/README to configure.): G
Operator may refer to: