Affine Lie algebras of π° π© 2 β‘ π
Let
and let
We consider the untwisted or twisted affine Lie algebra
The 1-dimensional subalgebra
as Lie subalgebras and we have3
Isomorphism of extended Lie algebras
and Λ π are isomorphic (but not as graded Lie algebras) under Λ π [ π 3 ] π β¦ π π β¦ π β 1 4 πΌ 1 πΌ 1 β π‘ π β¦ πΌ 1 β π‘ π + 1 2 πΏ π π π₯ Β± πΌ 1 β¦ π₯ Β± πΌ 1 β π‘ π Β± 1 / 2 There also exist grade-preserving isomorphisms between
for Λ π [ π π ] . π = 1 , 2 , 3
Via formal series
Taking a formal series approach on
For
\hat{\mathfrak{a}}_{0}In
we define the formal sums Λ π 0 [ [ π§ , π§ β 1 ] ] π₯ Β± πΌ 1 ( π§ ) = β π β β€ ( π₯ Β± πΌ 1 β π‘ π ) π§ β π πΌ 1 ( π§ ) = β π β β€ ( πΌ 1 β π‘ π ) π§ β π the commutation relations are more conveniently expressed as
[ πΌ 1 β π‘ π , π₯ Β± πΌ 1 ( π§ ) ] = Β± 2 π§ π π₯ Β± πΌ 1 ( π§ ) = β¨ πΌ 1 , Β± πΌ 1 β© π§ π π₯ Β± πΌ 1 ( π§ ) [ π₯ Β± πΌ 1 ( π§ 1 ) , π₯ Β± πΌ ( π§ 2 ) ] = 0 [ π₯ πΌ 1 ( π§ 1 ) , π₯ β πΌ 1 ( π§ 2 ) ] = ( πΌ 1 ( π§ 2 ) β π π· 1 ) πΏ ( π§ 1 / π§ 2 ) [ π , π₯ Β± πΌ 1 ( π§ ) ] = β π· π₯ Β± πΌ 1 ( π§ ) [ π , πΌ 1 ( π§ ) ] = β π· πΌ 1 ( π§ ) where
. π β β€
For
\hat{\mathfrak{a}}_{3}In
we define the formal sums Λ π 3 [ [ π§ 1 / 2 , π§ β 1 / 2 ] ] π₯ Β± πΌ 1 ( π§ ) = β π β β€ + 1 2 ( π₯ Β± πΌ 1 β π‘ π ) π§ β π πΌ 1 ( π§ ) = β π β β€ ( πΌ 1 β π‘ π ) π§ β π the commutation relations are more conveniently expressed as
[ πΌ 1 β π‘ π , π₯ Β± πΌ 1 ( π§ ) ] = Β± 2 π§ π π₯ Β± πΌ 1 ( π§ ) = β¨ πΌ 1 , Β± πΌ 1 β© π§ π π₯ Β± πΌ 1 ( π§ ) [ π₯ Β± πΌ 1 ( π§ 1 ) , π₯ Β± πΌ ( π§ 2 ) ] = 0 [ π₯ πΌ 1 ( π§ 1 ) , π₯ β πΌ 1 ( π§ 2 ) ] = ( πΌ 1 ( π§ 2 ) β π π· 1 ) [ ( π§ 1 / π§ 2 ) 1 / 2 πΏ ( π§ 1 / π§ 2 ) ] [ π , π₯ Β± πΌ 1 ( π§ ) ] = β π· π₯ Β± πΌ 1 ( π§ ) [ π , πΌ 1 ( π§ ) ] = β π· πΌ 1 ( π§ )
For
\hat{\mathfrak{a}}_{1}In
we define the formal sums Λ π 1 [ [ π§ 1 / 2 , π§ β 1 / 2 ] ] π₯ Β± πΌ 1 ( π§ ) = 1 2 β π β β€ ( π₯ + πΌ 1 β π‘ π ) π§ β π Β± 1 2 β π β β€ + 1 2 ( π₯ β πΌ 1 β π‘ π ) π§ β π πΌ 1 ( π§ ) = β π β β€ + 1 2 ( πΌ 1 β π‘ π ) π§ β π the commutation relations are more conveniently expressed as
[ πΌ 1 β π‘ π , π₯ Β± πΌ 1 ( π§ ) ] = Β± 2 π§ π π₯ Β± πΌ 1 ( π§ ) = β¨ πΌ 1 , Β± πΌ 1 β© π§ π π₯ Β± πΌ 1 ( π§ ) [ π₯ πΌ 1 ( π§ ) , π₯ β πΌ 1 ( π§ 2 ) ] = 1 2 ( πΌ 1 ( π§ 2 ) β π π· 1 ) πΏ ( π§ 1 / 2 1 / π§ 1 / 2 2 ) and we also have
π₯ β πΌ 1 ( π§ ) = l i m π§ 1 / 2 β β π§ 1 / 2 π₯ πΌ 1 ( π§ )
Representations
Footnotes
-
For
, we can conjugate by Pauli matricesπ = β for the same result. β©π π -
FLM use
andπ 1 = π 3 β©π 2 = π 1 -
1988. Vertex operator algebras and the Monster, Β§3.1, pp. 62β67 β©