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CCR algebraIn 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
:
: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
:
:
:(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
:
: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
:
: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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