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Draft in progress for: G-structure on a manifold
G
{\displaystyle G}
dim
(
M
)
{\displaystyle \operatorname {dim} (M)}
G
{\displaystyle G}
-structure
Torsion-free
Integrable
Comments
GL
(
n
,
R
)
{\displaystyle \operatorname {GL} (n,\mathbb {R} )}
n
{\displaystyle n}
—
Every n -manifold trivally possesses an integrable
GL
(
n
,
R
)
{\displaystyle \operatorname {GL} (n,\mathbb {R} )}
structure: the frame bundle itself
GL
+
(
n
,
R
)
{\displaystyle \operatorname {GL} ^{+}(n,\mathbb {R} )}
n
{\displaystyle n}
An orientation
Possible only if the manifold is orientable.
SL
(
n
,
R
)
{\displaystyle \operatorname {SL} (n,\mathbb {R} )}
n
{\displaystyle n}
A volume form
Possible only if the manifold is orientable.
{
e
}
{\displaystyle \{e\}}
n
{\displaystyle n}
A parallelization
An affine parallelization
A topological obstruction exists in this case. A parallelization is torsion-free if and only if the given global frame is a holonomic (commuting) frame.
O
(
n
)
{\displaystyle \operatorname {O} (n)}
n
{\displaystyle n}
A Riemannian metric
A flat Riemannian metric
Always possible, since
O
(
n
)
{\displaystyle \operatorname {O} (n)}
is a deformation retract of
GL
(
n
,
R
)
{\displaystyle \operatorname {GL} (n,\mathbb {R} )}
. The existence of the Levi-Civita connection means that every
O
(
n
)
{\displaystyle \operatorname {O} (n)}
-structure is torsion-free.
O
(
p
,
q
)
{\displaystyle \operatorname {O} (p,q)}
p
+
q
{\displaystyle p+q}
A pseudo-Riemannian metric
A flat pseudo-Riemannian metric
There is a topological obstruction in this case.
Sp
(
2
n
,
R
)
{\displaystyle \operatorname {Sp} (2n,\mathbb {R} )}
2
n
{\displaystyle 2n}
A non-degenerate 2-form
A symplectic form
The torsion of a
Sp
(
2
n
,
R
)
{\displaystyle \operatorname {Sp} (2n,\mathbb {R} )}
-structure
ω
{\displaystyle \omega }
is essentially the exterior derivative
d
ω
{\displaystyle d\omega }
, so the structure is torsion-free iff
ω
{\displaystyle \omega }
is closed . Darboux's theorem says that every torsion-free
Sp
(
2
n
,
R
)
{\displaystyle \operatorname {Sp} (2n,\mathbb {R} )}
-structure is integrable.
GL
(
n
,
C
)
{\displaystyle \operatorname {GL} (n,\mathbb {C} )}
2
n
{\displaystyle 2n}
An almost complex structure
A complex structure
The torsion of a
GL
(
n
,
C
)
{\displaystyle \operatorname {GL} (n,\mathbb {C} )}
-structure
J
{\displaystyle J}
given by the Nijenhuis tensor
N
J
{\displaystyle N_{J}}
. The Newlander–Nirenberg theorem states that every torsion-free
GL
(
n
,
C
)
{\displaystyle \operatorname {GL} (n,\mathbb {C} )}
-structure is integrable.
U
(
n
)
{\displaystyle \operatorname {U} (n)}
2
n
{\displaystyle 2n}
A Hermitian metric
A Kähler metric
A flat Kähler metric
U
(
n
)
=
GL
(
n
,
C
)
∩
Sp
(
2
n
,
R
)
∩
O
(
2
n
)
{\displaystyle \operatorname {U} (n)=\operatorname {GL} (n,\mathbb {C} )\cap \operatorname {Sp} (2n,\mathbb {R} )\cap \operatorname {O} (2n)}
, so this is a compatible combination of a complex, a symplectic, and an orthogonal structure.
GL
(
n
,
H
)
⋅
H
×
{\displaystyle \operatorname {GL} (n,\mathbb {H} )\cdot \mathbb {H} ^{\times }}
4
n
{\displaystyle 4n}
An almost quaternionic structure
A quaternionic structure
Unlike the complex case, there is no guarantee of integrability for (torsion-free) quaternionic manifolds. There exist counterexamples.
GL
(
n
,
H
)
{\displaystyle \operatorname {GL} (n,\mathbb {H} )}
4
n
{\displaystyle 4n}
A hypercomplex structure
Sp
(
n
)
⋅
Sp
(
1
)
{\displaystyle \operatorname {Sp} (n)\cdot \operatorname {Sp} (1)}
4
n
{\displaystyle 4n}
A quaternion-Hermitian metric
A quaternionic Kähler metric
Sp
(
n
)
{\displaystyle \operatorname {Sp} (n)}
4
n
{\displaystyle 4n}
A hyperkähler metric