Heisenberg algebra

Standard Heisenberg algebra for QM

Consider QM in nD. The Lie algebra over β„‚ generated by the operators { βˆ’π‘–β„,Λ†π‘₯𝑖,ˆ𝑝𝑖}𝑛𝑖=1 under the commutator is an example of a β„€-graded Heisenberg algebra, with

𝔩0=βŸ¨βˆ’π‘–β„βŸ©π”©βˆ’π‘–=βŸ¨Λ†π‘₯π‘–βŸ©π”©π‘–=βŸ¨Λ†π‘π‘–βŸ©

for 1 ≀𝑖 ≀𝑛 and 𝔩±𝑖 =0 otherwise, yielding the commutation relations

[Λ†π‘₯𝑖,𝑖ℏ]=[ˆ𝑝𝑖,𝑖ℏ]=[Λ†π‘₯𝑖,Λ†π‘₯𝑗]=[ˆ𝑝𝑖,ˆ𝑝𝑗]=0[ˆ𝑝𝑖,Λ†π‘₯𝑗]=βˆ’π‘–β„π›Ώπ‘–π‘—

for 1 ≀𝑖,𝑗 ≀𝑛.

Canonical realization

The irreducible representation of the Heisenberg algebra given by the Heisenberg module 𝑀( βˆ’π‘–β„) gives the vector space β„‚[π‘₯𝑖]𝑛𝑖=1 of polynomials in indeterminates {π‘₯𝑖}𝑛𝑖=1 with

Λ†π‘₯𝑖𝑓=π‘₯𝑓ˆ𝑝𝑖𝑓=βˆ’π‘–β„πœ•πœ•π‘₯π‘“βˆ’π‘–β„π‘“=βˆ’π‘–β„π‘“

which concurs with the realization of QM in nD position-space.


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