Affine Lie algebras of ๐”ฐ๐”ฉ2โก๐•‚

Twisted vertex operator representation of ๐”ฐ๐”ฉ2โก๐•‚ห†

Let ห†๐”ž1 =๐”ฐ๐”ฉ2โก๐•‚ห†[๐œŽ1] be the ๐œŽ1-twisted affine Lie algebra of ๐”ฐ๐”ฉ2โก๐•‚, and ๐‘‰ be the corresponding โ„ค +12-natural Heisenberg module on ๐”ฅ =๐•‚๐›ผ. Defining

๐›ผ(๐‘ง)ยฑ=โˆ‘๐‘›โˆˆยฑ(โ„•0+12)๐›ผ(๐‘›)๐‘งโˆ’๐‘›๐›ผ(๐‘ง)=โˆ‘๐‘›โˆˆโ„ค+12๐›ผ(๐‘›)๐‘งโˆ’๐‘›=๐›ผ(๐‘ง)++๐›ผ(๐‘ง)โˆ’๐ธยฑ(๐›ผ,๐‘ง)=eโˆ’๐ทโˆ’1๐›ผ(๐‘ง)ยฑ

we construct the twisted vertex operator

๐‘‹โ„ค+12(๐›ผ,๐‘ง)=๐ธโˆ’(โˆ’๐›ผ,๐‘ง)๐ธ+(โˆ’๐›ผ,๐‘ง)2โŸจ๐›ผ,๐›ผโŸฉ=:e๐ทโˆ’1๐›ผ(๐‘ง):2โˆ’โŸจ๐›ผ,๐›ผโŸฉ

where the second expression used the Normal ordered product. Skipping over a lot of detail1, the representation of หœ๐”ฅ[ โˆ’1] on ๐‘‰ extends to precisely two irreducible representations

๐œ‹ยฑ:หœ๐”ž1โ†’Endโก๐‘‰๐‘ฅ๐›ผ1(๐‘ง)โ†ฆ๐‘‹(๐›ผ1,๐‘ง)


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Footnotes

  1. 1988. Vertex operator algebras and the Monster, ยง3, pp. 61ff. โ†ฉ