Natural Heisenberg algebras

Normal ordered product

Let ๐‘‰ be a space carrying a representation of a natural Heisenberg algebra ห†๐”ฅ๐‘ for ๐‘ =โ„ค or ๐‘ =โ„ค +12, and let ๐‘ยฑ 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 ๐›ผ โˆˆ๐”ฅ we have the formal sum of operators

๐›ผ(๐‘ง)=โˆ‘๐‘›โˆˆโ„ค๐›ผ(๐‘›)๐‘งโˆ’๐‘›

where ๐›ผ(๐‘›) is a homogenous operator of degree ๐‘›, we define #m/def/lie

๐›ผ(๐‘ง)ยฑ=12๐›ผ(0)[0โˆˆ๐‘]+โˆ‘๐‘›โˆˆ๐‘ยฑ๐›ผ(๐‘›)๐‘งโˆ’๐‘›โŸน๐›ผ(๐‘ง)=๐›ผ(๐‘ง)++๐›ผ(๐‘ง)โˆ’

where we have used an Iverson bracket. Then the normal ordered product is defined recursively for {๐›ผ๐‘–}๐‘˜๐‘–=1 โІ๐”ฅ by

:๐›ผ1(๐‘ง):=๐›ผ1(๐‘ง):๐›ผ1(๐‘ง)โ‹ฏ๐›ผ๐‘˜(๐‘ง):=๐›ผ๐‘˜(๐‘ง)โˆ’:๐›ผ1(๐‘ง)โ‹ฏ๐›ผ๐‘˜โˆ’1(๐‘ง):+:๐›ผ1(๐‘ง)โ‹ฏ๐›ผ๐‘˜โˆ’1(๐‘ง):๐›ผ๐‘˜(๐‘ง)+

which induces a map ๐‘†โˆ™๐”ฅ โ†’(Endโก๐‘‰){๐‘ง}. In particular

:๐›ผ1(๐‘›1)๐›ผ2(๐‘›2):={๐›ผ1(๐‘›1)๐›ผ2(๐‘›2)๐‘›1โ‰ค๐‘›2๐›ผ2(๐‘›2)๐›ผ1(๐‘›1)๐‘›2โ‰ค๐‘›1

and

:๐›ผ(๐‘ง)๐‘˜:=๐‘˜โˆ‘โ„“=0(๐‘˜โ„“)(๐‘Ž(๐‘ง)โˆ’)โ„“(๐‘Ž(๐‘ง)+)๐‘˜โˆ’โ„“

For ๐ทโˆ’1

Let ๐ทโˆ’1 be the inverse degree operator on ๐ท((Endโก๐‘‰){๐‘ง}), so

๐ทโˆ’1๐›ผ(๐‘ง)=๐ทโˆ’1๐›ผ(๐‘ง)++๐ทโˆ’1๐›ผ(๐‘ง)โˆ’:๐ทโˆ’1๐›ผ1(๐‘ง):=๐ทโˆ’1๐›ผ1(๐‘ง):๐ทโˆ’1๐›ผ1(๐‘ง)โ‹ฏ๐ทโˆ’1๐›ผ๐‘˜(๐‘ง):=๐ทโˆ’1๐›ผ๐‘˜(๐‘ง)โˆ’:๐ทโˆ’1๐›ผ1(๐‘ง)โ‹ฏ๐ทโˆ’1๐›ผ๐‘˜โˆ’1(๐‘ง):=+:๐ทโˆ’1๐›ผ1(๐‘ง)โ‹ฏ๐ทโˆ’1๐›ผ๐‘˜โˆ’1(๐‘ง):๐ทโˆ’1๐›ผ๐‘˜(๐‘ง)+

and

:expโก๐ทโˆ’1๐›ผ(๐‘ง):=โˆ‘๐‘˜โˆˆโ„•0:(๐ทโˆ’1๐›ผ(๐‘ง))๐‘˜:๐‘˜!


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Footnotes

  1. 1988. Vertex operator algebras and the Monster, ยง3.3, p. 73โ€“76 โ†ฉ

  2. 1988. Vertex operator algebras and the Monster, ยง4.2, p. 89โ€“92 โ†ฉ