sl_2

Affine Lie algebras of 𝔰𝔩2⁑𝕂

Let π”ž = sl_2 with its Chevalley basis and let πœŽπ‘– be the suggestively named1 involutive isometries of π”ž defined by lie

𝜎1:𝛼1β†¦βˆ’π›Ό1𝜎2:𝛼1β†¦βˆ’π›Ό1𝜎3:𝛼1↦𝛼1π‘₯±𝛼1↦π‘₯βˆ“π›Ό1π‘₯±𝛼1β†¦βˆ’π‘₯βˆ“π›Ό1π‘₯±𝛼1β†¦βˆ’π‘₯±𝛼

and let 𝜎0 =1. Furthermore we let

π‘₯+𝛼1=π‘₯𝛼1+π‘₯βˆ’π›Ό1=π‘₯𝛼1+π‘₯𝜎1𝛼1=π‘₯𝛼1βˆ’π‘₯𝜎2𝛼1π‘₯βˆ’π›Ό1=π‘₯𝛼1βˆ’π‘₯βˆ’π›Ό1=π‘₯𝛼1βˆ’π‘₯𝜎1𝛼1=π‘₯𝛼1+π‘₯𝜎2𝛼1

We consider the untwisted or twisted affine Lie algebra Λ†π”žπ‘– =Λ†π”ž[πœŽπ‘–]2 which have bases

Λ†π”ž0=βŸ¨π‘,𝛼1βŠ—π‘‘π‘š,π‘₯±𝛼1βŠ—π‘‘π‘š:π‘šβˆˆβ„€βŸ©Λ†π”ž1=βŸ¨π‘,𝛼1βŠ—π‘‘π‘š+1/2,π‘₯+𝛼1βŠ—π‘‘π‘š,π‘₯βˆ’π›Ό1βŠ—π‘‘π‘š+1/2:π‘šβˆˆβ„€βŸ©Λ†π”ž2=βŸ¨π‘,𝛼1βŠ—π‘‘π‘š+1/2,π‘₯+𝛼1βŠ—π‘‘π‘š+1/2,π‘₯βˆ’π›Ό1βŠ—π‘‘π‘š:π‘šβˆˆβ„€βŸ©Λ†π”ž3=βŸ¨π‘,𝛼1βŠ—π‘‘π‘š,π‘₯±𝛼1βŠ—π‘‘π‘š+1/2:π‘šβˆˆβ„€βŸ©

The 1-dimensional subalgebra π”₯ =𝕂𝛼 β‰€π”ž generates the natural Heisenberg algebras

Λ†π”₯β„€=π•‚π‘βŠ•β¨π‘›βˆˆβ„€βˆ–{0}𝛼1βŠ—π‘‘π‘›β‰€Λœπ”₯β‰€Λ†π”ž0,Λ†π”ž3Λ†π”₯β„€+12=π•‚π‘βŠ•β¨π‘›βˆˆβ„€+12𝛼1βŠ—π‘‘π‘›β‰€Λœπ”₯[βˆ’1]β‰€Λ†π”ž1,Λ†π”ž2

as Lie subalgebras and we have3

[𝑐,Λ†π”žπ‘–]=0[𝛼1βŠ—π‘‘π‘š,𝛼1βŠ—π‘‘π‘›]=2π‘šπ›Ώπ‘š+𝑛𝑐

Via formal series

Taking a formal series approach on Λ†π”žπ‘–, the exact characterization varies with 𝑖.

Representations


develop | en | SemBr

Footnotes

  1. For 𝕂 =β„‚, we can conjugate by Pauli matrices πœŽπ‘– for the same result. ↩

  2. FLM use πœ—1 =𝜎3 and πœ—2 =𝜎1 ↩

  3. 1988. Vertex operator algebras and the Monster, Β§3.1, pp. 62–67 ↩