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- (g,K)-module
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- Harish-Chandra module
In mathematics, more specifically in the representation theory of reductive Lie groups, a
(
g
,
K
)
{\displaystyle ({\mathfrak {g}},K)}
-module is an algebraic object, first introduced by Harish-Chandra, used to deal with continuous infinite-dimensional representations using algebraic techniques. Harish-Chandra showed that the study of irreducible unitary representations of a real reductive Lie group, G, could be reduced to the study of irreducible
(
g
,
K
)
{\displaystyle ({\mathfrak {g}},K)}
-modules, where
g
{\displaystyle {\mathfrak {g}}}
is the Lie algebra of G and K is a maximal compact subgroup of G.
Definition
Let G be a real Lie group. Let
g
{\displaystyle {\mathfrak {g}}}
be its Lie algebra, and K a maximal compact subgroup with Lie algebra
k
{\displaystyle {\mathfrak {k}}}
. A
(
g
,
K
)
{\displaystyle ({\mathfrak {g}},K)}
-module is defined as follows: it is a vector space V that is both a Lie algebra representation of
g
{\displaystyle {\mathfrak {g}}}
and a group representation of K (without regard to the topology of K) satisfying the following three conditions
1. for any v ∈ V, k ∈ K, and X ∈
g
{\displaystyle {\mathfrak {g}}}
k
⋅
(
X
⋅
v
)
=
(
Ad
(
k
)
X
)
⋅
(
k
⋅
v
)
{\displaystyle k\cdot (X\cdot v)=(\operatorname {Ad} (k)X)\cdot (k\cdot v)}
2. for any v ∈ V, Kv spans a finite-dimensional subspace of V on which the action of K is continuous
3. for any v ∈ V and Y ∈
k
{\displaystyle {\mathfrak {k}}}
(
d
d
t
exp
(
t
Y
)
⋅
v
)
|
t
=
0
=
Y
⋅
v
.
{\displaystyle \left.\left({\frac {d}{dt}}\exp(tY)\cdot v\right)\right|_{t=0}=Y\cdot v.}
In the above, the dot,
⋅
{\displaystyle \cdot }
, denotes both the action of
g
{\displaystyle {\mathfrak {g}}}
on V and that of K. The notation Ad(k) denotes the adjoint action of G on
g
{\displaystyle {\mathfrak {g}}}
, and Kv is the set of vectors
k
⋅
v
{\displaystyle k\cdot v}
as k varies over all of K.
The first condition can be understood as follows: if G is the general linear group GL(n, R), then
g
{\displaystyle {\mathfrak {g}}}
is the algebra of all n by n matrices, and the adjoint action of k on X is kXk−1; condition 1 can then be read as
k
X
v
=
k
X
k
−
1
k
v
=
(
k
X
k
−
1
)
k
v
.
{\displaystyle kXv=kXk^{-1}kv=\left(kXk^{-1}\right)kv.}
In other words, it is a compatibility requirement among the actions of K on V,
g
{\displaystyle {\mathfrak {g}}}
on V, and K on
g
{\displaystyle {\mathfrak {g}}}
. The third condition is also a compatibility condition, this time between the action of
k
{\displaystyle {\mathfrak {k}}}
on V viewed as a sub-Lie algebra of
g
{\displaystyle {\mathfrak {g}}}
and its action viewed as the differential of the action of K on V.
Notes
References
Doran, Robert S.; Varadarajan, V. S., eds. (2000), The mathematical legacy of Harish-Chandra, Proceedings of Symposia in Pure Mathematics, vol. 68, AMS, ISBN 978-0-8218-1197-9, MR 1767886
Wallach, Nolan R. (1988), Real reductive groups I, Pure and Applied Mathematics, vol. 132, Academic Press, ISBN 978-0-12-732960-4, MR 0929683