Coframe
In mathematics, a coframe or coframe field on a smooth manifold M {\displaystyle M} is a system of one-forms or covectors which form a basis of the cotangent bundle at every point. In the exterior algebra of M {\displaystyle M} , one has a natural map from v k : ⨁ k T ∗ M → ⋀ k T ∗ M {\displaystyle v_{k}:\bigoplus ^{k}T^{*}M\to \bigwedge ^{k}T^{*}M} , given by v k : ( ρ 1 , … , ρ k ) ↦ ρ 1 ∧ … ∧ ρ k {\displaystyle v_{k}:(\rho _{1},\ldots ,\rho _{k})\mapsto \rho _{1}\wedge \ldots \wedge \rho _{k}} . If M {\displaystyle M} is n {\displaystyle n} dimensional, a coframe is given by a section σ {\displaystyle \sigma } of ⨁ n T ∗ M {\displaystyle \bigoplus ^{n}T^{*}M} such that v n ∘ σ ≠ 0 {\displaystyle v_{n}\circ \sigma \neq 0} . The inverse image under v n {\displaystyle v_{n}} of the complement of the zero section of ⋀ n T ∗ M {\displaystyle \bigwedge ^{n}T^{*}M} forms a G L ( n ) {\displaystyle GL(n)} principal bundle over M {\displaystyle M} , which is called the coframe bundle.
In mathematics, a coframe or coframe field on a smooth manifold
M
{\displaystyle M}
is a system of one-forms or covectors which form a basis of the cotangent bundle at every point. In the exterior algebra of
M
{\displaystyle M}
, one has a natural map from
v
k
:
⨁
k
T
∗
M
→
⋀
k
T
∗
M
{\displaystyle v_{k}:\bigoplus ^{k}T^{*}M\to \bigwedge ^{k}T^{*}M}
, given by
v
k
:
(
ρ
1
,
…
,
ρ
k
)
↦
ρ
1
∧
…
∧
ρ
k
{\displaystyle v_{k}:(\rho _{1},\ldots ,\rho _{k})\mapsto \rho _{1}\wedge \ldots \wedge \rho _{k}}
. If
M
{\displaystyle M}
is
n
{\displaystyle n}
dimensional, a coframe is given by a section
σ
{\displaystyle \sigma }
of
⨁
n
T
∗
M
{\displaystyle \bigoplus ^{n}T^{*}M}
such that
v
n
∘
σ
≠
0
{\displaystyle v_{n}\circ \sigma \neq 0}
. The inverse image under
v
n
{\displaystyle v_{n}}
of the complement of the zero section of
⋀
n
T
∗
M
{\displaystyle \bigwedge ^{n}T^{*}M}
forms a
G
L
(
n
)
{\displaystyle GL(n)}
principal bundle over
M
{\displaystyle M}
, which is called the coframe bundle.
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- Frame fields in general relativity
- Moving frame
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