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In [[mathematics]], the '''Frölicher–Nijenhuis bracket''' is an extension of the [[Lie bracket of vector fields|Lie bracket]] of [[vector fields]] to [[vector-valued differential form]]s on a [[differentiable manifold]].  It is useful in the study of [[connection (mathematics)|connections]], notably the [[Ehresmann connection]], as well as in the more general study of [[projection (linear algebra)|projections]] in the [[tangent bundle]].
It was introduced by  [[Alfred Frölicher]] and [[Albert Nijenhuis]] (1956) and is related to the work of [[Jan Arnoldus Schouten|Schouten]] (1940).
 
It is related to but not the same as the [[Nijenhuis–Richardson bracket]] and the [[Schouten–Nijenhuis bracket]].
 
==Definition==
Let Ω*(''M'') be the [[sheaf (mathematics)|sheaf]] of [[exterior algebra]]s of [[differential form]]s on a [[smooth manifold]] ''M''. This is a [[graded algebra]] in which forms are graded by degree:
:<math>\Omega^*(M) = \bigoplus_{k=0}^\infty \Omega^k(M).</math>
A [[graded derivation]] of degree ℓ is a mapping
:<math>D:\Omega^*(M)\to\Omega^{*+l}(M)</math>
which is linear with respect to constants and satisfies
:<math>D(\alpha\wedge\beta) = D(\alpha)\wedge\beta + (-1)^{\ell\deg(\alpha)}\alpha\wedge D(\beta).</math>
Thus, in particular, the [[interior product]] with a vector defines a graded derivation of degree ℓ&nbsp;=&nbsp;&minus;1, whereas the [[exterior derivative]] is a graded derivation of degree ℓ&nbsp;=&nbsp;1.
 
The vector space of all derivations of degree ℓ is denoted by Der<sub>ℓ</sub>Ω*(''M''). The direct sum of these spaces is a [[graded vector space]] whose homogeneous components consist of all graded derivations of a given degree; it is denoted
:<math>\mathrm{Der}\, \Omega^*(M) = \bigoplus_{k=-\infty}^\infty \mathrm{Der}_k\, \Omega^*(M).</math>
This forms a [[graded Lie algebra]] under the anticommutator of derivations defined on homogeneous derivations ''D''<sub>1</sub> and ''D''<sub>2</sub> of degrees ''d''<sub>1</sub> and ''d''<sub>2</sub>, respectively, by
:<math>[D_1,D_2] = D_1\circ D_2 - (-1)^{d_1d_2}D_2\circ D_1.</math>
 
Any [[vector-valued differential form]] ''K'' in Ω<sup>''k''</sup>(''M'',&nbsp;T''M'') with values in the [[tangent bundle]] of ''M'' defines a graded derivation of degree ''k''&nbsp;&minus;&nbsp;1, denote by ''i''<sub>''K''</sub>, and called the insertion operator. For ω&nbsp;∈&nbsp;Ω<sup>ℓ</sup>(''M''),
:<math>i_K\,\omega(X_1,\dots,X_{k+\ell-1})=\frac{1}{k!(\ell-1)!}\sum_{\sigma\in{S}_{k+\ell-1}}\textrm{sign}\,\sigma \cdot
\omega(K(X_{\sigma(1)},\dots,X_{\sigma(k)}),X_{\sigma(k+1)},\dots,X_{\sigma(k+\ell-1)})
</math>
The [[Lie derivative#Nijenhuis–Lie derivative|Nijenhuis–Lie derivative]] along ''K''&nbsp;∈&nbsp;Ω<sup>k</sup>(''M'',&nbsp;T''M'') is defined by
:<math>\mathcal{L}_K = [d,i_K] =d\,{\circ}\,  i_K-(-1)^{k-1}i_K{\circ}\, d</math>
where ''d'' is the exterior derivative and ''i''<sub>K</sub> is the insertion operator.
 
The Frölicher–Nijenhuis bracket is defined to be the unique vector-valued differential form
 
:<math>[\cdot, \cdot] : \Omega^k(M,\mathrm{T}M) \times \Omega^\ell(M,\mathrm{T}M) \to \Omega^{k+\ell}(M,\mathrm{T}M) : (K, L) \mapsto [K, L]</math>
such that
 
:<math>\mathcal{L}_{[K, L]} = [\mathcal{L}_K, \mathcal{L}_L].</math>
 
If ''k''&nbsp;=&nbsp;0, so that ''K''&nbsp;∈&nbsp;Ω<sup>0</sup>(''M'',&nbsp;T''M'')
is a vector field, the usual homotopy formula for the Lie derivative is recovered
:<math>\mathcal{L}_K = [d,i_K] =d \,{\circ}\, i_K+i_K \,{\circ}\, d.</math>
An explicit formula for the Frölicher–Nijenhuis bracket of <math>\phi\otimes X</math> and <math>\psi\otimes Y</math> (for forms φ and ψ and vector fields ''X'' and ''Y'') is given by
:<math>\left.\right.[\phi \otimes X,\psi \otimes Y] = \phi\wedge\psi\otimes [X,Y] + \phi\wedge\mathcal{L}_X \psi\otimes Y - \mathcal{L}_Y \phi\wedge\psi \otimes  X +(-1)^{\deg(\phi)}(d\phi \wedge i_X(\psi)\otimes Y +i_Y(\phi) \wedge d\psi \otimes X).</math>
 
==Derivations of the ring of forms==
 
Every derivation of Ω<sup>*</sup>(''M'') can be written as
:<math>i_L + \mathcal{L}_K</math>
for unique elements ''K'' and ''L'' of  Ω<sup>*</sup>(''M'', T''M''). The Lie bracket of these derivations is given as follows.
*The derivations of the form <math>\mathcal{L}_K</math> form the Lie superalgebra of all derivations commuting with ''d''. The bracket is given by
::<math>[\mathcal{L}_{K_1},\mathcal{L}_{K_2}]= \mathcal{L}_{[K_1,K_2]}</math>
:where the bracket on the right is the Frölicher–Nijenhuis bracket. In particular the Frölicher–Nijenhuis bracket defines a [[graded Lie algebra]] structure on <math>\Omega(M,\mathrm{T}M)</math>, which extends the [[Lie bracket of vector fields|Lie bracket]] of [[vector field]]s.
*The derivations of the form <math>i_L</math> form the Lie superalgebra of all derivations vanishing on functions Ω<sup>0</sup>(''M''). The bracket is given by
::<math>[i_{L_1},i_{L_2}]= i_{[L_1,L_2]^\and}</math>
:where the bracket on the right is the  [[Nijenhuis–Richardson bracket]].
*The bracket of derivations of different types is given by
::<math>[\mathcal{L}_{K}, i_L]= i_{[K,L]} - (-1)^{kl}\mathcal{L}_{i_LK}</math>
: for ''K'' in &Omega;<sup>k</sup>(''M'', T''M''), ''L'' in &Omega;<sup>l+1</sup>(''M'', T''M'').
 
==Applications==
The [[Nijenhuis tensor]] of an [[almost complex structure]] ''J'', is the Frölicher–Nijenhuis bracket of ''J'' with itself. An almost complex structure is a complex structure if and only if the Nijenhuis tensor is zero.
 
With the Frölicher–Nijenhuis bracket it is possible to define the [[curvature]] and [[cocurvature]] of a vector-valued 1-form which is a [[projection (mathematics)|projection]]. This generalizes the concept of the curvature of a [[Connection (mathematics)|connection]].
 
There is a common generalization of the Schouten–Nijenhuis bracket and the Frölicher–Nijenhuis bracket; for details see the article on the [[Schouten–Nijenhuis bracket]].
 
==References==
*{{citation
| last1 = Frölicher | first1 = A.
| last2 = Nijenhuis | first2 = A. | author2-link = Albert Nijenhuis
| journal = [[Indagationes Mathematicae]]
| pages = 338–360
| title = Theory of vector valued differential forms. Part I.
| volume = 18
| year = 1956}}.
*{{citation
| last1 = Frölicher | first1 = A.
| last2 = Nijenhuis | first2 = A. | author2-link = Albert Nijenhuis
| journal = Communicationes Mathematicae Helveticae
| pages = 227–248
| title = Invariance of vector form operations under mappings
| volume = 34
| year = 1960}}.
*{{springer|id=F/f120230|author=P. W. Michor|title=Frölicher–Nijenhuis bracket}}
*{{citation
| last = Schouten | first = J. A. | author-link = Jan Arnoldus Schouten
| journal = [[Indagationes Mathematicae]]
| pages = 449–452
| title = Über Differentialkonkomitanten zweier kontravarianten Grössen
| volume = 2
| year = 1940}}.
 
{{DEFAULTSORT:Frolicher-Nijenhuis Bracket}}
[[Category:Bilinear operators]]
[[Category:Binary operations]]
[[Category:Differential geometry]]

Revision as of 03:10, 27 January 2014

In mathematics, the Frölicher–Nijenhuis bracket is an extension of the Lie bracket of vector fields to vector-valued differential forms on a differentiable manifold. It is useful in the study of connections, notably the Ehresmann connection, as well as in the more general study of projections in the tangent bundle. It was introduced by Alfred Frölicher and Albert Nijenhuis (1956) and is related to the work of Schouten (1940).

It is related to but not the same as the Nijenhuis–Richardson bracket and the Schouten–Nijenhuis bracket.

Definition

Let Ω*(M) be the sheaf of exterior algebras of differential forms on a smooth manifold M. This is a graded algebra in which forms are graded by degree:

Ω*(M)=k=0Ωk(M).

A graded derivation of degree ℓ is a mapping

D:Ω*(M)Ω*+l(M)

which is linear with respect to constants and satisfies

D(αβ)=D(α)β+(1)deg(α)αD(β).

Thus, in particular, the interior product with a vector defines a graded derivation of degree ℓ = −1, whereas the exterior derivative is a graded derivation of degree ℓ = 1.

The vector space of all derivations of degree ℓ is denoted by DerΩ*(M). The direct sum of these spaces is a graded vector space whose homogeneous components consist of all graded derivations of a given degree; it is denoted

DerΩ*(M)=k=DerkΩ*(M).

This forms a graded Lie algebra under the anticommutator of derivations defined on homogeneous derivations D1 and D2 of degrees d1 and d2, respectively, by

[D1,D2]=D1D2(1)d1d2D2D1.

Any vector-valued differential form K in Ωk(M, TM) with values in the tangent bundle of M defines a graded derivation of degree k − 1, denote by iK, and called the insertion operator. For ω ∈ Ω(M),

iKω(X1,,Xk+1)=1k!(1)!σSk+1signσω(K(Xσ(1),,Xσ(k)),Xσ(k+1),,Xσ(k+1))

The Nijenhuis–Lie derivative along K ∈ Ωk(M, TM) is defined by

K=[d,iK]=diK(1)k1iKd

where d is the exterior derivative and iK is the insertion operator.

The Frölicher–Nijenhuis bracket is defined to be the unique vector-valued differential form

[,]:Ωk(M,TM)×Ω(M,TM)Ωk+(M,TM):(K,L)[K,L]

such that

[K,L]=[K,L].

If k = 0, so that K ∈ Ω0(M, TM) is a vector field, the usual homotopy formula for the Lie derivative is recovered

K=[d,iK]=diK+iKd.

An explicit formula for the Frölicher–Nijenhuis bracket of ϕX and ψY (for forms φ and ψ and vector fields X and Y) is given by

[ϕX,ψY]=ϕψ[X,Y]+ϕXψYYϕψX+(1)deg(ϕ)(dϕiX(ψ)Y+iY(ϕ)dψX).

Derivations of the ring of forms

Every derivation of Ω*(M) can be written as

iL+K

for unique elements K and L of Ω*(M, TM). The Lie bracket of these derivations is given as follows.

  • The derivations of the form K form the Lie superalgebra of all derivations commuting with d. The bracket is given by
[K1,K2]=[K1,K2]
where the bracket on the right is the Frölicher–Nijenhuis bracket. In particular the Frölicher–Nijenhuis bracket defines a graded Lie algebra structure on Ω(M,TM), which extends the Lie bracket of vector fields.
  • The derivations of the form iL form the Lie superalgebra of all derivations vanishing on functions Ω0(M). The bracket is given by
[iL1,iL2]=i[L1,L2]
where the bracket on the right is the Nijenhuis–Richardson bracket.
  • The bracket of derivations of different types is given by
[K,iL]=i[K,L](1)kliLK
for K in Ωk(M, TM), L in Ωl+1(M, TM).

Applications

The Nijenhuis tensor of an almost complex structure J, is the Frölicher–Nijenhuis bracket of J with itself. An almost complex structure is a complex structure if and only if the Nijenhuis tensor is zero.

With the Frölicher–Nijenhuis bracket it is possible to define the curvature and cocurvature of a vector-valued 1-form which is a projection. This generalizes the concept of the curvature of a connection.

There is a common generalization of the Schouten–Nijenhuis bracket and the Frölicher–Nijenhuis bracket; for details see the article on the Schouten–Nijenhuis bracket.

References

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