Natural Heisenberg algebras

Normal ordered product

Let 𝑉 be a space carrying a representation of a natural Heisenberg algebra Λ†π”₯𝑍 for 𝑍 =β„€ or 𝑍 =β„€ +12, and let 𝑍± denote the strictly positive and negative parts of 𝑍 respectively. The normal ordered product is a procedure for obtaining well-defined operators from infinite expressions.12

Definition

In general, if for 𝛼 ∈π”₯ we have the formal sum of operators

𝛼(𝑧)=βˆ‘π‘›βˆˆβ„€π›Ό(𝑛)π‘§βˆ’π‘›

where 𝛼(𝑛) is a ^homogenous operator of degree 𝑛, we define lie

𝛼(𝑧)Β±=12𝛼(0)[0βˆˆπ‘]+βˆ‘π‘›βˆˆπ‘Β±π›Ό(𝑛)π‘§βˆ’π‘›βŸΉπ›Ό(𝑧)=𝛼(𝑧)++𝛼(𝑧)βˆ’

where we have used an Iverson bracket. Then the normal ordered product is defined recursively for {𝛼𝑖}π‘˜π‘–=1 βŠ†π”₯ by

:𝛼1(𝑧):=𝛼1(𝑧):𝛼1(𝑧)β‹―π›Όπ‘˜(𝑧):=π›Όπ‘˜(𝑧)βˆ’:𝛼1(𝑧)β‹―π›Όπ‘˜βˆ’1(𝑧):+:𝛼1(𝑧)β‹―π›Όπ‘˜βˆ’1(𝑧):π›Όπ‘˜(𝑧)+

which induces a map π‘†βˆ™π”₯ β†’(End⁑𝑉){𝑧}. In particular

:𝛼1(𝑛1)𝛼2(𝑛2):={𝛼1(𝑛1)𝛼2(𝑛2)𝑛1≀𝑛2𝛼2(𝑛2)𝛼1(𝑛1)𝑛2≀𝑛1

and

:𝛼(𝑧)π‘˜:=π‘˜βˆ‘β„“=0(π‘˜β„“)(π‘Ž(𝑧)βˆ’)β„“(π‘Ž(𝑧)+)π‘˜βˆ’β„“

For π·βˆ’1

Let π·βˆ’1 be the inverse degree operator on 𝐷((End⁑𝑉){𝑧}), so

π·βˆ’1𝛼(𝑧)=π·βˆ’1𝛼(𝑧)++π·βˆ’1𝛼(𝑧)βˆ’:π·βˆ’1𝛼1(𝑧):=π·βˆ’1𝛼1(𝑧):π·βˆ’1𝛼1(𝑧)β‹―π·βˆ’1π›Όπ‘˜(𝑧):=π·βˆ’1π›Όπ‘˜(𝑧)βˆ’:π·βˆ’1𝛼1(𝑧)β‹―π·βˆ’1π›Όπ‘˜βˆ’1(𝑧):=+:π·βˆ’1𝛼1(𝑧)β‹―π·βˆ’1π›Όπ‘˜βˆ’1(𝑧):π·βˆ’1π›Όπ‘˜(𝑧)+

and

:expβ‘π·βˆ’1𝛼(𝑧):=βˆ‘π‘˜βˆˆβ„•0:(π·βˆ’1𝛼(𝑧))π‘˜:π‘˜!


develop | en | SemBr

Footnotes

  1. 1988. Vertex operator algebras and the Monster, Β§3.3, p. 73–76 ↩

  2. 1988. Vertex operator algebras and the Monster, Β§4.2, p. 89–92 ↩