In mathematics , the Cartan projection is an aid in the theory of Lie groups and Lie algebras .
definition
Let it be a semi-simple Lie group with Lie algebra and a Cartan subalgebra . For a root system, let the positive Weyl chamber and .
G
{\ displaystyle G}
G
{\ displaystyle {\ mathfrak {g}}}
a
⊂
G
{\ displaystyle {\ mathfrak {a}} \ subset {\ mathfrak {g}}}
Σ
{\ displaystyle \ Sigma}
a
+
⊂
a
{\ displaystyle {\ mathfrak {a}} ^ {+} \ subset {\ mathfrak {a}}}
A.
+
=
exp
(
a
+
)
{\ displaystyle A ^ {+} = \ exp ({\ mathfrak {a}} ^ {+})}
Then there is a unique maximally compact subgroup with
K
⊂
G
{\ displaystyle K \ subset G}
G
=
K
A.
+
K
{\ displaystyle G = KA ^ {+} K}
and a clear picture
μ
:
G
→
A.
+
{\ displaystyle \ mu \ colon G \ to A ^ {+}}
,
so that each can be unambiguously decomposed as having (from dependent) .
G
∈
G
{\ displaystyle g \ in G}
G
=
k
1
μ
(
G
)
k
2
{\ displaystyle g = k_ {1} \ mu (g) k_ {2}}
G
{\ displaystyle g}
k
1
,
k
2
∈
K
{\ displaystyle k_ {1}, k_ {2} \ in K}
The image is called the Cartan projection . It applies .
μ
:
G
→
A.
+
{\ displaystyle \ mu \ colon G \ to A ^ {+}}
μ
(
G
)
=
K
G
K
∩
A.
+
{\ displaystyle \ mu (g) = KgK \ cap A ^ {+}}
example
Be it
G
=
S.
L.
(
n
,
R.
)
,
K
=
S.
O
(
n
)
,
A.
+
=
{
diag
(
σ
1
,
...
,
σ
n
)
∈
G
:
σ
1
≥
...
≥
σ
n
>
0
}
{\ displaystyle G = SL (n, \ mathbb {R}), K = SO (n), A ^ {+} = \ left \ {\ operatorname {diag} (\ sigma _ {1}, \ ldots, \ sigma _ {n}) \ in G: \ sigma _ {1} \ geq \ ldots \ geq \ sigma _ {n}> 0 \ right \}}
.
Then the Cartan projection is given by
μ
(
G
)
=
diag
(
σ
1
(
G
)
,
...
,
σ
n
(
G
)
)
{\ displaystyle \ mu (g) = \ operatorname {diag} (\ sigma _ {1} (g), \ ldots, \ sigma _ {n} (g))}
,
where is the -th eigenvalue of .
σ
i
(
G
)
2
{\ displaystyle \ sigma _ {i} (g) ^ {2}}
i
{\ displaystyle i}
G
t
G
{\ displaystyle g ^ {t} g}
Jordan projection
Another continuous projection can be defined by the Jordan decomposition ; it overhangs with the Cartan projection
λ
:
G
→
a
¯
+
{\ displaystyle \ lambda \ colon G \ to {\ overline {\ mathfrak {a}}} ^ {+}}
λ
(
G
)
=
lim
n
→
∞
e
x
p
-
1
(
μ
(
G
n
)
)
n
{\ displaystyle \ lambda (g) = \ lim _ {n \ to \ infty} {\ frac {exp ^ {- 1} (\ mu (g ^ {n}))} {n}}}
together. In the case one obtains the figure
G
=
S.
L.
(
n
,
R.
)
{\ displaystyle G = SL (n, \ mathbb {R})}
λ
(
G
)
=
(
log
∣
λ
1
(
G
)
∣
,
log
∣
λ
2
(
G
)
∣
,
...
,
log
∣
λ
n
(
G
)
∣
)
{\ displaystyle \ lambda (g) = (\ log \ mid \ lambda _ {1} (g) \ mid, \ log \ mid \ lambda _ {2} (g) \ mid, \ ldots, \ log \ mid \ lambda _ {n} (g) \ mid)}
,
whereby the eigenvalues (possibly with repetitions) are in ascending order.
λ
1
(
G
)
,
...
,
λ
n
(
G
)
{\ displaystyle \ lambda _ {1} (g), \ ldots, \ lambda _ {n} (g)}
literature
Helgason, Sigurdur: Differential geometry, Lie groups, and symmetric spaces. Corrected reprint of the 1978 original. Graduate Studies in Mathematics, 34th American Mathematical Society, Providence, RI, 2001. ISBN 0-8218-2848-7 (Chapter 9)
Benoist, Yves: Actions propres sur les espaces homogènes réductifs. (Chapter 3) pdf
Web links
Individual evidence
^ Benoist: Propriétés asymptotiques des groupes linéaires , GAFA 7 (1997), 1-47
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