Formal sums over a Lie algebra

Formal series over an (un)twisted affine Lie algebra

Let ๐”ค be quadratic Lie algebra, ๐œ— โˆˆAutโก๐”ค be an involutive isometry, and หœ๐”ค and หœ๐”ค[๐œ—] be the associated extended untwisted affine Lie algebra and extended twisted affine Lie algebra respectively. Then to each ๐‘ฅ โˆˆ๐”ค, we associate the following formal series in หœ๐”ค[[๐‘ง,๐‘งโˆ’1]] and หœ๐”ค[๐œ—][[๐‘ง1/2,๐‘งโˆ’1/2]] respectively: #m/def/lie

๐‘ฅโ„ค(๐‘ง)=โˆ‘๐‘›โˆˆโ„ค(๐‘ฅโŠ—๐‘ก๐‘›)๐‘งโˆ’๐‘›โˆˆหœ๐”ค[[๐‘ง,๐‘งโˆ’1]]๐‘ฅโ„ค+1/2(๐‘ง)=โˆ‘๐‘›โˆˆโ„ค(๐‘ฅ(๐‘›)โŠ—๐‘ก๐‘›/2)๐‘งโˆ’๐‘›/2โˆˆหœ๐”ค[๐œ—][[๐‘ง1/2,๐‘งโˆ’1/2]]

and we will drop the subscripts when it is clear. In the latter

๐‘ฅโ†ฆ๐‘ฅ(๐‘–)=12(๐‘ฅ+(โˆ’1)๐‘–๐œ—๐‘ฅ)

denotes the appropriate projection into the ๐œ—-eigenspace decomposition ๐”ค =๐”ค(0) โŠ•๐”ค(1).1

Commutation relations

For ๐‘ฅ,๐‘ฆ โˆˆ๐”ค, we may recast the commutation relations of หœ๐”ค using the Formal delta and ๐ท operator as

[๐‘ฅ(๐‘ง1),๐‘ฅ(๐‘ง2)]=[๐‘ฅ,๐‘ฆ](๐‘ง2)๐›ฟ(๐‘ง1/๐‘ง2)โˆ’โŸจ๐‘ฅ,๐‘ฆโŸฉ(๐ท๐›ฟ)(๐‘ง1/๐‘ง2)๐‘[๐‘,๐‘ฅ(๐‘ง)]=0[๐‘‘,๐‘ฅ(๐‘ง)]=โˆ’๐ท๐‘ฅ(๐‘ง)[๐‘,๐‘‘]=0

and in หœ๐”ค[๐œ—] as

[๐‘ฅ(๐‘ง1),๐‘ฅ(๐‘ง2)]=12โˆ‘๐‘–โˆˆโ„ค2[๐œ—๐‘–๐‘ฅ,๐‘ฆ](๐‘ง2)๐›ฟ((โˆ’1)๐‘–๐‘ง1/21/๐‘ง1/22)โˆ’12โˆ‘๐‘–โˆˆโ„ค2โŸจ๐œ—๐‘–๐‘ฅ,๐‘ฆโŸฉ๐ท1๐›ฟ((โˆ’1)๐‘–)๐‘ง1/21/๐‘ง1/22)๐‘[๐‘,๐‘ฅ(๐‘ง)]=0[๐‘‘,๐‘ฅ(๐‘ง)]=โˆ’๐ท๐‘ฅ(๐‘ง)[๐‘,๐‘‘]=0


#state/develop | #lang/en | #SemBr

Footnotes

  1. 1988. Vertex operator algebras and the Monster, ยง2.3, pp. 58โ€“60 โ†ฉ