Natural Heisenberg algebras
Normal ordered product
Let ๐ be a space carrying a representation of a natural Heisenberg algebra ห๐ฅ๐ for ๐ =โค or ๐ =โค +12,
and let ๐ยฑ denote the strictly positive and negative parts of ๐ respectively.
The normal ordered product is a procedure for obtaining well-defined operators from infinite expressions.12
Definition
In general, if for ๐ผ โ๐ฅ we have the formal sum of operators
๐ผ(๐ง)=โ๐โโค๐ผ(๐)๐งโ๐
where ๐ผ(๐) is a homogenous operator of degree ๐, we define #m/def/lie
๐ผ(๐ง)ยฑ=12๐ผ(0)[0โ๐]+โ๐โ๐ยฑ๐ผ(๐)๐งโ๐โน๐ผ(๐ง)=๐ผ(๐ง)++๐ผ(๐ง)โ
where we have used an Iverson bracket.
Then the normal ordered product is defined recursively for {๐ผ๐}๐๐=1 โ๐ฅ by
:๐ผ1(๐ง):=๐ผ1(๐ง):๐ผ1(๐ง)โฏ๐ผ๐(๐ง):=๐ผ๐(๐ง)โ:๐ผ1(๐ง)โฏ๐ผ๐โ1(๐ง):+:๐ผ1(๐ง)โฏ๐ผ๐โ1(๐ง):๐ผ๐(๐ง)+
which induces a map ๐โ๐ฅ โ(Endโก๐){๐ง}.
In particular
:๐ผ1(๐1)๐ผ2(๐2):={๐ผ1(๐1)๐ผ2(๐2)๐1โค๐2๐ผ2(๐2)๐ผ1(๐1)๐2โค๐1
and
:๐ผ(๐ง)๐:=๐โโ=0(๐โ)(๐(๐ง)โ)โ(๐(๐ง)+)๐โโ
For ๐ทโ1
Let ๐ทโ1 be the inverse degree operator on ๐ท((Endโก๐){๐ง}), so
๐ทโ1๐ผ(๐ง)=๐ทโ1๐ผ(๐ง)++๐ทโ1๐ผ(๐ง)โ:๐ทโ1๐ผ1(๐ง):=๐ทโ1๐ผ1(๐ง):๐ทโ1๐ผ1(๐ง)โฏ๐ทโ1๐ผ๐(๐ง):=๐ทโ1๐ผ๐(๐ง)โ:๐ทโ1๐ผ1(๐ง)โฏ๐ทโ1๐ผ๐โ1(๐ง):=+:๐ทโ1๐ผ1(๐ง)โฏ๐ทโ1๐ผ๐โ1(๐ง):๐ทโ1๐ผ๐(๐ง)+
and
:expโก๐ทโ1๐ผ(๐ง):=โ๐โโ0:(๐ทโ1๐ผ(๐ง))๐:๐!
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