Double centralizer theorem: Difference between revisions

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A '''Representation up to homotopy''' is a concept in [[differential geometry]] that generalizes the notion of [[representation of a Lie algebra]] to [[Lie algebroid]]s and nontrivial [[vector bundle]]s. It was introduced by Abad and Crainic.<ref>C.A. Abad, M. Crainic: ''Representations up to homotopy of Lie algebroids'', [http://arxiv.org/abs/0901.0319 arXiv:0901.0319]</ref>
 
As a motivation consider a regular Lie algebroid (''A'',''ρ'',[.,.]) (regular meaning that the anchor ''ρ'' has constant rank) where we have two natural ''A''-[[connection (mathematics)|connection]]s on ''g''(''A'')&nbsp;=&nbsp;ker&nbsp;''ρ'' and ''ν''(''A'')= ''TM''/im&nbsp;''ρ'' respectively:
:<math>\nabla\colon \Gamma(A)\times\Gamma(\mathfrak{g}(A))\to\Gamma(\mathfrak{g}(A)): \nabla_{\!\phi\,}\psi:=[\phi,\psi],</math>
:<math>\nabla\colon \Gamma(A)\times\Gamma(\nu(A))\to\Gamma(\nu(A)): \nabla_{\!\phi\,}\overline{X}:=\overline{[\rho(\phi),X]}.</math>
 
In the [[deformation theory]] of the Lie algebroid ''A'' there is a long exact sequence<ref>M.Crainic, I.Moerdijk: ''Deformations of Lie brackets: cohomological aspects''. J. Eur. Math. Soc., '''10''':1037–1059, (2008)</ref>
:<math>\dots\to H^n(A,\mathfrak{g}(A))\to H^n_{def}(A)\to H^{n-1}(A,\nu(A))\to H^{n-1}(A,\mathfrak{g}(A))\to\dots</math>
This suggests that the correct cohomology for the deformations (here denoted as ''H''<sub>def</sub>) comes from the direct sum of the two modules ''g''(''A'') and ''ν''(''A'') and should be called [[Adjoint representation of a Lie group|adjoint representation]].  Note however that in the more general case where ''ρ'' does not have constant rank we cannot easily define the representations ''g''(''A'') and ''ν''(''A''). Instead we should consider the 2-term [[complex]]{{disambiguation needed|date=June 2012}} ''A''→''TM'' and a representation on it.  This leads to the notion explained here.
 
== Definition ==
Let (''A'',''ρ'',[.,.]) be a Lie algebroid over a smooth manifold ''M'' and let Ω(''A'') denote its Lie algebroid complex.  Let further ''E'' be a ℤ-graded vector bundle over ''M'' and Ω(''A'',''E'')&nbsp;=&nbsp;Ω(''A'')&nbsp;⊗&nbsp;Γ(''E'') be its ℤ-graded ''A''-cochains with values in ''E''.  A representation up to homotopy of ''A'' on ''E'' is a differential operator ''D'' that maps
:<math>D\colon \Omega^\bullet(A,E)\to\Omega^{\bullet+1}(A,E),</math>
 
fulfills the Leibniz rule
:<math> D(\alpha\wedge\beta) = (D\alpha)\wedge\beta + (-1)^{|\alpha|}\alpha\wedge(D\beta),</math>
 
and squares to zero, i.e. ''D''<sup>2</sup>&nbsp;=&nbsp;0.
 
=== Homotopy operators ===
A representation up to homotopy as introduced above is equivalent to the following data
* a degree 1 operator ∂: ''E''&nbsp;→&nbsp;''E'' that squares to 0,
* an ''A''-connection ∇ on ''E'' compatible as <math>\nabla\circ\partial=\partial\circ\nabla</math>,
* an End(''E'')-valued ''A''-2-form ''ω''<sub>2</sub> of total degree 1, such that the curvature fulfills <math>\partial\omega_2+R_\nabla=0,</math>
* End(''E'')-valued ''A''-''p''-forms ''ω''<sub>''p''</sub> of total degree 1 that fulfill the homotopy relations….
 
The correspondence is characterized as
:<math> D = \partial +\nabla+\omega_2+\omega_3+\cdots. \,</math>
 
=== Homomorphisms ===
A homomorphism between representations up to homotopy (''E'',''D<sub>E</sub>'') and (''F'',''D<sub>F</sub>'') of the same Lie algebroid ''A'' is a degree 0 map Φ:Ω(''A'',''E'')&nbsp;→&nbsp;Ω(''A'',''F'') that commutes with the differentials, i.e.
:<math>D_E\circ\Phi = \Phi\circ D_E. \, </math>
 
An [[isomorphism]] is now an invertible homomorphism.
We denote '''Rep<sup>∞</sup>''' the category of equivalence classes of representations up to homotopy together with equivalence classes of homomorphisms.
 
In the sense of the above decomposition of ''D'' into a cochain map ∂, a connection ∇, and higher homotopies, we can also decompose the Φ as Φ<sub>0</sub> + Φ<sub>1</sub> + … with
 
:<math>\Phi_i\in\Omega^i(A,\mathrm{Hom}^{-i}(E,F))</math>
 
and then the compatibility condition reads
:<math> \partial\Phi_n +d_\nabla(\Phi_{n-1})+[\omega_2,\Phi_{n-2}]+\cdots+[\omega_n,\Phi_0] = 0.</math>
 
== Examples ==
Examples are usual representations of Lie algebroids or more specifically Lie algebras, i.e. modules.
 
Another example is given by a ''p''-form ''ω''<sub>''p''</sub> together with ''E''&nbsp;=&nbsp;M&nbsp;×&nbsp;ℝ[0]&nbsp;⊕&nbsp;ℝ[''p''] and the operator ''D''&nbsp;=&nbsp;∇&nbsp;+&nbsp;''ω''<sub>''p''</sub> where ∇ is the flat connection on the trivial bundle&nbsp;''M''&nbsp;×&nbsp;ℝ.
 
Given a representation up to homotopy as ''D''&nbsp;=&nbsp;∂&nbsp;+&nbsp;∇&nbsp;+&nbsp;''ω''<sub>2</sub>&nbsp;+&nbsp;… we can construct a new representation up to homotopy by conjugation, i.e.
: ''D'' = ∂ &minus; ∇ + ''ω''<sub>2</sub> &minus; ''ω''<sub>3</sub> + &minus;&hellip;.
 
=== Adjoint representation ===
Given a Lie algebroid (''A'',''ρ'',[.,.]) together with a connection ∇ on its vector bundle we can define two associated ''A''-connections as follows<ref>M.Crainic, R.L.Fernandes: ''Secondary characteristic classes of Lie algebroids''. In ''Quantum field theory and noncommutative geometry'', '''vol 662''' of Lecture Notes in Phys., pp. 157–176, Springer, Berlin, 2005.</ref>
:<math>\nabla^{bas}_{\!\phi\,}\psi := [\phi,\psi]+\nabla_{\!\rho(\psi)\,}\phi,</math>
:<math>\nabla^{bas}_{\!\phi\,}X := [\rho(\phi),X]+\rho(\nabla_{\!X\,}\phi).</math>
Moreover we can introduce the mixed curvature as
:<math>R^{bas}(\phi,\psi)(X):= \nabla_{\!X\,}[\phi,\psi]-[\nabla_{\!X\,}\phi,\psi]-[\phi,\nabla_{\!X\,}\psi] -\nabla_{\!\nabla^{bas}_{\!\psi\,}X\,}\phi +\nabla_{\!\nabla^{bas}_{\!\psi\,}X\,}\phi.</math>
This curvature measures the compatibility of the Lie bracket with the connection and is one of the two conditions of ''A'' together with ''TM'' forming a [[matched pair]] of Lie algebroids.
 
The first observation is that this term decorated with the anchor map ''ρ'', accordingly, expresses the curvature of both connections ∇<sup>bas</sup>.  Secondly we can match up all three ingredients to a representation up to homotopy as:
:<math>D = \rho +\nabla^{bas}+R^{bas}.</math>
 
Another observation is that the resulting representation up to homotopy is independent of the chosen connection ∇, basically because the difference between two ''A''-connections is an (''A''&nbsp;&minus;&nbsp;1&nbsp;-form with values in End(''E'').
 
== References ==
<!--- See [[Wikipedia:Footnotes]] on how to create references using <ref></ref> tags which will then appear here automatically -->
{{Reflist}}
 
<!--- Categories --->
 
[[Category:Representation theory of Lie algebras]]
[[Category:Differential geometry]]

Latest revision as of 03:36, 8 April 2014

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