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CCR algebra

In quantum field theory, if V is a real vector space equipped with a nonsingular real antisymmetric bilinear form (,) (i.e. a symplectic vector space), the unital
- -algebra
generated by elements of V subject to the relations :fg-gf=i(f,g) :f
- =f for any f, g in V is called the canonical commutation relations (CCR) algebra. The uniqueness of the representations of this algebra when V is finite dimensional is discussed in the Stone-von Neumann theorem. There is also a corresponding unital C
- -algebra
, often referred to as the Weyl form of the algebra, generated by eif subject to :e^e^=e^ :e^e^=e^e^e^ :(eif)
- =e-if for real numbers c1, c2. If V is equipped with a nonsingular real symmetric bilinear form (,) instead, the unital
- -algebra generated by the elements of V subject to the relations :fg+gf=(f,g) :f
- =f for any f, g in V is called the canonical anticommutation relations (CAR) algebra. If V is a real Z2-graded vector space equipped with a nonsingular antisymmetric bilinear superform (,) (i.e. (g,f)=-(-1)|f||g|(g,f) ) such that (f,g) is real if either f or g is an even element and imaginary if both of them are odd, the unital
- -algebra generated by the elements of V subject to the relations :fg-(-1)^gf=i(f,g) :f
- =f, g
- =g for any two pure elements f, g in V is the obvious super generalization which unifies CCRs with CARs.

See also


- canonical commutation relation
- Stone-von Neumann theorem
- Bose-Einstein statistics
- Fermi-Dirac statistics
- Heisenberg group
- Bogoliubov transformation Category:Quantum field theoryCategory:functional analysis

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