User damienc - MathOverflowmost recent 30 from http://mathoverflow.net2013-05-26T04:58:44Zhttp://mathoverflow.net/feeds/user/7031http://www.creativecommons.org/licenses/by-nc/2.5/rdfhttp://mathoverflow.net/questions/127589/does-the-vanishing-of-the-poisson-bracket-on-s-mathfrakg-mathfrakg-ins/130091#130091Answer by DamienC for Does the vanishing of the Poisson bracket on $S(\mathfrak{g})^{\mathfrak{g}}$ inspire the disover of Duflo's isomorphism theorem?DamienC2013-05-08T16:10:41Z2013-05-11T09:10:31Z<blockquote>
<p>My question is: Does the vanishing of
the Poisson bracket plays an important
role in finding and proving Duflo's
isomorphism theorem? Or it is just an
literally first step?</p>
</blockquote>
<p>Let $A_0$ be a Poisson algebra and $A$ a deformation quantization of $A_0$ (assume we are in a context when it exists). </p>
<p>Assume you have a quantization map $Q:A_0\to A$, by which I mean a section of the classical limit map $A\to A/(\hbar)=A_0$. </p>
<p>Then for any two elements $a,b\in A_0$, <code>$[Q(a),Q(b)]=\hbar\{a,b\}+O(\hbar^2)$</code>. </p>
<p>Hence if you want to have $Q(ab)=Q(a)Q(b)$ you must at least assume that <code>$\{a,b\}=0$</code>. </p>
<p>My (non-)answer to your question is then: </p>
<blockquote>
<p>the vanishing of the Poisson bracket is a necessary requirement
if you want a statement of Duflo-type. It is just a first step. </p>
</blockquote>
<p>The actual history comes from the Harish-Chandra isomomorphism.
Duflo noticed that the original formula could be written for any Lie algebra, without any use of roots and similar stuff specific to the semi-simple case. </p>
http://mathoverflow.net/questions/119991/is-the-quantum-algebra-unique-up-to-isomorphism-in-deformation-quantization/120089#120089Answer by DamienC for Is the quantum algebra unique (up to isomorphism) in deformation quantization ? DamienC2013-01-28T08:38:33Z2013-01-28T08:38:33Z<p>Let me give a conjectural answer. </p>
<p>Point 1. $GRT$ acts non-trivially on poly-vector fields by $L_\infty$-isomorphisms (see T.Willwacher, M. Kontsevich’s graph complex and the Grothendieck-Teichm¨uller Lie algebra, arXiv:1009.1654 for an explicit description of this actions). </p>
<p>Point 2. I guess that $GRT$ actually acts non-trivially on the set of equivalence classes of Maurer-Cartan elements (I haven't checked this). </p>
<p>Point 3. composing Kontsevich's formality map with the action of GRT gives a negative answer to your question if Point 2 is correct. . </p>
<p>Point 4. concerning the symplectic case, the main reason why the classification map doesn't depend on any choice is because the quantization is unique. Let me explain further: the choices involved in the formality isomorphism appear in the local case. By itself, the globalization procedure does not require any additional choice. </p>
http://mathoverflow.net/questions/47885/trace-of-the-atiyah-class-equals-chern-class/115613#115613Answer by DamienC for trace of the atiyah class equals chern classDamienC2012-12-06T14:27:44Z2012-12-06T14:27:44Z<p>I might be wrong but it seems to me that the $p$-th Atiyah class does not have any reason to agree with the usual $p$-th Chern class unless the manifold under consideration is Kahler. </p>
<p>Namely, if $X$ is not Kahler then for a holomorphic vector bundle $E\to X$, $c_p(E)\in H^{2p}(X)$ and $at_p(E)\in H^{p}(X,\Omega^p_X)$ live in different spaces. </p>
<p>The point is that $c_p(E)$ can be defined as the class of $tr(R^p)$, where $R$ is the curvature of an hermitian connection on $E$, while $at_p(E)$ can be defined as the class of $tr(R_{1,1}^p)$, where $R_{1,1}$ is the $(1,1)$-part of the curvature of a $(1,0)$-connection on $E$. </p>
<p>The point is that if $X$ is Kahler then there exists an Hermitian $(1,0)$-connection with curvature being of type $(1,1)$. The relation between the Atiyah classes and the Chern classes can be made through the Hodge-to-de Rham spectral sequence. </p>
<hr>
<p>So, I think that the Chern classes you are talking about are not the usual (i.e. topological) ones, but the Chern classes in Hodge cohomology. Then they coincide with the Atiyah classes almost by definition (by the way, there is a <a href="http://archive.numdam.org/ARCHIVE/BSMF/BSMF_1958__86_/BSMF_1958__86__137_0/BSMF_1958__86__137_0.pdf" rel="nofollow">very nice paper of Grothendieck</a> on Chern classes in Hodge cohomology). </p>
http://mathoverflow.net/questions/31972/todd-class-and-baker-campbell-hausdorff-or-the-curious-number-12/115488#115488Answer by DamienC for Todd class and Baker-Campbell-Hausdorff, or the curious number $12$DamienC2012-12-05T10:05:26Z2012-12-05T10:05:26Z<p>The answer to your question is the following: given two non-commutative variables $x$ and $y$ one has
$$
log(e^xe^y)=x+e^{ad_x}\frac{ad_x}{e^{ad_x}-1}(y)+O(y^2)
$$</p>
<p>It is not the appearance of $12$ that is intriguing, but the appearance of the Todd series in algebraic geometry. It suggests that there is a group hidden somewhere... and this is indeed the case. This group is the derived loop space of your favorite algebraic variety $X$, and its tangent Lie algebra is the shifted tangent sheaf $T_X[-1]$, with Lie bracket given by the Atiyah class (the fact that the Atiyah class gives rize to a Lie structure was <a href="http://arxiv.org/abs/alg-geom/9704009" rel="nofollow">discovered by Kapranov</a>). </p>
<p>The universal enveloping algebra of this Lie algebra is the Hochschild complex of $X$. One then gets a nice dictionnary between the Lie side and the algebraic geometry side. E.g.: </p>
<ul>
<li><p>any object in the derived category of $X$ turns out to be a representation of this Lie algebra. </p></li>
<li><p>Poincare-Birkhoff-Witt is Hochschild-Kostant-Rosenberg. </p></li>
<li><p>the Duflo isomorphism is the Kontsevich-Caldararu isomorphism between the Harmonic and Hochschild structures. </p></li>
<li><p>there is also an relation between closed embeddings in algebraic geometry and inclusions of Lie algebras. </p></li>
<li><p>...</p></li>
</ul>
http://mathoverflow.net/questions/54430/video-lectures-of-mathematics-courses-available-online-for-free/115474#115474Answer by DamienC for Video lectures of mathematics courses available online for freeDamienC2012-12-05T07:18:37Z2012-12-05T07:18:37Z<p>The courses of the summer school <strong>Poisson 2012</strong> (that took place in Utrecht), as well as lectures of the conference that followed, are available online: <a href="http://www.youtube.com/user/poissonutrecht" rel="nofollow">http://www.youtube.com/user/poissonutrecht</a></p>
<p>The courses are: </p>
<ul>
<li><a href="http://www.youtube.com/watch?v=uYDi1NTJ930" rel="nofollow">Poisson and Symplectic Geometry of Moduli Spaces of Flat Connections</a>, by Anton Alekseev </li>
<li><a href="http://www.youtube.com/watch?v=oYSE7p9fRBE" rel="nofollow">Poisson Geometry</a>, by Rui Loja Fernandes </li>
<li><a href="http://www.youtube.com/watch?v=Yai8BIUfTuY" rel="nofollow">Lie Groupoids and Multiplicative Structures</a>, by Henrique Bursztyn </li>
<li><a href="http://www.youtube.com/watch?v=_uiNqQIOzK4" rel="nofollow">Cluster Algebras and Compatible Poisson Structures</a>, by Michael Gekhtman </li>
</ul>
http://mathoverflow.net/questions/114701/one-more-question-about-pbwOne more question about PBWDamienC2012-11-27T21:03:43Z2012-11-28T18:20:41Z
<p>Let $k$ be a commutative ring with unit and $L$ be a Lie $k$-algebra. </p>
<p>Let $U(L)$ be the universal enveloping $k$-algebra of $L$ (one can define it as a quotient of the tensor algebra, as it is explained <a href="http://mathoverflow.net/questions/61954/pbw-theorem-over-a-q-algebra-without-freeness-or-flatness" rel="nofollow">in this MO question</a>, or one can say that $U(-)$ is left adjoint to the forgetful functor sending an associative $k$-algebra to the Lie $k$-algebra obtained by taking the same underlying $k$-module and with Lie bracket being the commutator). </p>
<p>The associative $k$-algebra $U(L)$ is filtered as a $k$-algebra, and there is a canonical epimorphism $S(L)\to gr\big(U(L)\big)$. </p>
<p>If this epimorphism is an isomorphism, then we say that <em>$L$ has the PBW property</em>. </p>
<p>All the examples of Lie $k$-algebras not satisfying the PBW property I am aware of are constructed in the following way: one first finds an example of a Lie algebra for which the map $L\to U(L)$ (the unit of the adjunction) is not injective, and then it is quite clear that the PBW property can't hold. </p>
<p>My question is then: </p>
<blockquote>
<p>Is there any example of a Lie
$k$-algebra $L$ such that the map
$L\to U(L)$ is injective which does
not satisfy the PBW property ?</p>
</blockquote>
<p>Or is it that the PBW property is just equivalent to $L\to U(L)$ being injective (it would be great, but I have no idea why this would be true - EDIT: one might want to use that $L\to U(L)$ is injective to reduce to the cas when $k\supset\mathbb{Q}$)?</p>
http://mathoverflow.net/questions/99689/existence-of-dg-realization-for-6-functors/100570#100570Answer by DamienC for Existence of dg realization for 6 functorsDamienC2012-06-25T07:45:08Z2012-11-27T07:53:39Z<p>If I understand correctly your are looking for a dg enhancement of the six operation formalism. </p>
<p>There seem to be a paper that does something very close to it: Yifeng Liu and Weizhe Zheng, <em>Enhanced six operations and base change theorem for sheaves on Artin stacks</em> (available at <a href="http://math.columbia.edu/~liuyf/sixi.pdf" rel="nofollow">http://math.columbia.edu/~liuyf/sixi.pdf</a>). </p>
<p>They use the language of $(\infty,1)$-categories, but I think one can adapt it to dg-categories (assuming that one is working over a field of characteristic zero). </p>
<p>EDIT Nov. 27, 2012: the above preprint has been posted on the arXiv: <a href="http://arxiv.org/abs/1211.5948" rel="nofollow">http://arxiv.org/abs/1211.5948</a></p>
http://mathoverflow.net/questions/112069/a-fibrant-objects-structure-on-top/114412#114412Answer by DamienC for A fibrant-objects structure on TopDamienC2012-11-25T11:20:08Z2012-11-25T12:40:06Z<p>This might be a naive answer but here is a suggestion for the definition of $\pi_n$-fibrations: maps having the RLP with respect to the the map $\Delta^k\to\Delta^k\times I$ for any $k\leq n$. </p>
<p>In the limit you will get the "obvious" fibrant-object structure on $Top$ which comes from its usual model structure (recall that the full subcategory of fibrant objects in any model category is a category of fibrant objects.. and that all objects are fibrants in $Top$).</p>
http://mathoverflow.net/questions/110020/algebraic-proof-of-hodge-decomposition-theorem/110024#110024Answer by DamienC for algebraic proof of Hodge decomposition theoremDamienC2012-10-18T17:04:36Z2012-10-18T17:04:36Z<p>Deligne and Illusie proved the degeneration of Hodge to de Rahm (see e.g. <a href="http://math.bu.edu/people/potthars/writings/HdRSS.pdf" rel="nofollow">http://math.bu.edu/people/potthars/writings/HdRSS.pdf</a> for a brief review): </p>
<blockquote>
<p>Relevements modulo $p^2$ et
decomposition du complexe de De Rham,
Inv. Math. <strong>89</strong> (1987), 247-270.</p>
</blockquote>
<p>BUT the Deligne-Illusie approach does only says that the spectral suequence degenerates at $E_1$ (with $E_1$ terms being $H^q(X,\Omega^p_X)$). But is does not give an explicit isomorphism between $H^n(X)$ and $\oplus_{p+q=n}H^q(X,\Omega^p_X)$. </p>
<p>I heard about a work-in-progress by Dima Arinkin, Andrei Caldararu and Marton Hablicsek, where they have a new approach to Deligne-Illusie <em>via</em> derived geometry. It might be that there approach gives the Hodge decomposition (I actualy don't know if this is the case or not). </p>
http://mathoverflow.net/questions/109001/exact-dg-poisson-algebra/109122#109122Answer by DamienC for Exact DG Poisson algebraDamienC2012-10-08T07:51:27Z2012-10-08T17:32:24Z<p>It seems to me that there is a (quasi-)isomorphism between the de Rham algebra and the dg algebra of polyvector fields equipped with the differential $[\pi,-]$ (where $\pi$ is the Poisson structure corresponding to the symplectic form). </p>
<p>Through this isomorphism the equation $d\omega=0$ is sent to $[\pi,\pi]=0$, and the equation $\omega=d\lambda$ is sent to $\pi=[\pi,V]$, where $V$ is a vector field. </p>
<p>On the level of the Poisson algebra of functions it tells you that for any two functions $f,g$, we have (up to a sign)
<code>$$
\{f,g\}=V(\{f,g\})-\{V(f),g\}+\{f,V(g)\}
$$</code></p>
<p>Algebraically you can say that there is a derivation $V$ for the product such that the Poisson bracket is its own derived bracket w.r.t. $V$. </p>
http://mathoverflow.net/questions/63381/do-i-need-to-know-what-an-infinity-gerstenhaber-algebra-is-and-if-so-what-is-it/105937#105937Answer by DamienC for Do I need to know what an infinity-Gerstenhaber algebra is, and if so, what is it?DamienC2012-08-30T12:39:03Z2012-08-30T12:39:03Z<blockquote>
<p>Question 1: Does there necessarily
exist a resolution of S that computes
the derived $S\otimes_R$ and that is
Gerstenhaber in a compatible way?</p>
</blockquote>
<p>Yes. As pointed out in the comments, the category of dg Gerstenhaber algebra admits a model structure in which the weak equivalences are the quasi-isomorphisms, fibrations are degreewise surjections, and cobifrant obects are those dg Gerstenhaber algebras that are free as graded algerbas. </p>
<p>This actually wors with dg algebras over any given operad $\mathcal O$ (in place of Gerstenhaber). </p>
<p>This is proved in Hinich's paper (quoted by the nLab: <a href="http://ncatlab.org/nlab/show/model+structure+on+dg-algebras+over+an+operad" rel="nofollow">http://ncatlab.org/nlab/show/model+structure+on+dg-algebras+over+an+operad</a>). </p>
<p>Then there is also a natural model structure on the category of dg Gerstenhaber $R$-algebras (there is a more general statement about existence of a model structure on the category of objects under a given one $X$ in a model category $\mathcal C$). </p>
<p>So, the answer to the title of your question is that you don't "need" to know what a $G_\infty$-algebra is. </p>
<blockquote>
<p>Question 2 if the answer to 1 is YES: How do I construct it?</p>
</blockquote>
<p>Shortly, bar-cobar. You can have a look at <a href="http://www.institut.math.jussieu.fr/%257Eginot/papers/gerstenhaber.pdf" rel="nofollow">Homologie et model minimal des algèbres de Gerstenhaber</a> in order to see how it works in details. </p>
<p>Btw, the above paper also tells you what is the definition of a $G_\infty$-algebra. </p>
<blockquote>
<p>Question 2 if the answer to 1 is NO:
Certainly my homotopy equivalence $S\leftrightarrow\widetilde{S}$
allows me to move the Gerstenhaber
structure on $S$ to something on $\widetilde{S}$.
What structure on $\widetilde{S}$ does it move to?</p>
</blockquote>
<p>Even though the answer to Question 1 is YES, there is still something to say here.
There is on $\widetilde{S}$ a $G_\infty$-structure. This is "just" homotopy transfer formula (and the use of the explicit minimal model for the Gerstenhaber operad). </p>
<p>The homotopy transfer for algebras over operad $\mathcal O$, w.r.t. to a cofibrant resolution $\widetilde{\mathcal O}\to\mathcal O$ is proved in the appendix A.2 of <a href="http://arxiv.org/abs/0710.4510" rel="nofollow">my paper with Van den Bergh</a> (see also Theorem 10.3.6 in <a href="http://math.unice.fr/~brunov/Operads.pdf" rel="nofollow">Loday-Vallette's Algebraic Operads</a> for the Koszul case). </p>
http://mathoverflow.net/questions/105904/how-to-define-the-equivalence-of-maurer-cartan-elements-in-an-l-infty-algebr/105905#105905Answer by DamienC for How to define the equivalence of Maurer-Cartan elements in an $L_{\infty}$-algebra?DamienC2012-08-30T06:03:00Z2012-08-30T06:03:00Z<p>This is explained in Section 4.5.2 of "deformation quantization of poisson manifolds" by Kontsevich (http://arxiv.org/abs/q-alg/9709040). </p>
<p>The way you wrote the homotopy between two Maurer-Cartan elements is not enough : as it is explained in the above reference you also need a 1-parameter family of infinitesimal gauge equivalences. </p>
<p>A quick reformulation of Kontsevich definition is the following. An equivalence between two Maurer-Cartan elements $a$ and $b$ in $\mathfrak g$ is a Maurer-Cartan element $c$ in $DR([0,1])\otimes\mathfrak g$ such that $a=c(0)$ and $b=c(0)$. </p>
<p>Note that $DR(...)$ stands for the de Rham algebra of "...". </p>
http://mathoverflow.net/questions/105806/what-structure-on-the-second-order-cotangent-bundleWhat structure on the second order cotangent bundle ?DamienC2012-08-29T09:05:15Z2012-08-29T12:56:19Z
<p>It is well-known that the total space of the cotangent bundle $T^*X$ of a given smooth manifold $X$ admits a <a href="http://en.wikipedia.org/wiki/Symplectic_manifold" rel="nofollow">symplectic form</a> $\omega$. It is actually exact: $\omega=d\lambda$. The $1$-form $\lambda$ is called the <a href="http://en.wikipedia.org/wiki/Liouville_form" rel="nofollow">Liouville form</a> and can be defined in a quite tautological way: given an element $p=(x,\xi)\in T^*X$ (i.e. $x\in X$ and <code>$\xi\in T^*_xX$</code>) and a vector $v\in T_p(T^*X)$, we define <code>$\lambda_p(v):=\xi(\pi_*(v))$</code>, where <code>$\pi:T^*X\to X$</code> (and thus <code>$\pi_*(v)\in T_xX$</code>). </p>
<blockquote>
<p>Does the total space of the second order cotangent bundle $T^*_2X$ also admits a "natural" geometric structure ? It seems that there is similarly a tautological "second order form" on $T^*_2X$ (in place of the Liouville tautological $1$-form $\lambda$). But then I don't see any analog for $\omega$... </p>
</blockquote>
<p><strong>Recall that</strong> the second order cotangent bundle can be defined as the dual of the second order tangent bundle $T^2X$, which is the bundle of order $2$ differential operators on $X$ that vanish on constants. </p>
<p>In case you would be an algebraic geometer, the fiber of <code>$T^*_2X$</code> at a point $x$ ($X$ is now a smooth algebraic variety) is just <code>$I_x/I_x^3$</code> if $I_x$ is the maximal ideal corresponding to $x$ (w.r.t. to an affine open neighbourhood of it).</p>
http://mathoverflow.net/questions/30536/t-structures-and-higher-categories/105825#105825Answer by DamienC for t-structures and higher categories?DamienC2012-08-29T12:25:39Z2012-08-29T12:25:39Z<blockquote>
<p>So I'd like to ask: is there a higher
categorical analog of a t-structure?</p>
</blockquote>
<p>As Mike Skirvin pointed out in a comment, higher categorical analog of t-structures have been introduced by Lurie. A more up-to-date reference might be <a href="http://www.math.harvard.edu/~lurie/papers/HigherAlgebra.pdf" rel="nofollow">Higher Algebra</a> (<code>$\S$</code> 1.2.1). </p>
<blockquote>
<p>More generally, how does the higher categorical viewpoint help one understand the set of all (or maybe all "nice" in an appropriate sense) t-structures on a given trangulated category, provided it is the homotopy category of a stable (∞,1) category?</p>
</blockquote>
<p>I guess the answer can be found at the same place. There, Lurie says that "there is a bijective correspondence between $t$-localizations of $\mathcal C$ (a stable $\infty$-category) and $t$-structures on the triangulated category $h\mathcal C$. </p>
<p>The higher categorical point-of-view also seems to be useful to understand the yoga of derived functors in a more conceptual way. In Section 1.3 of the same reference (Higher Algebra) it is explained that if $\mathcal A$ is an abelian category with enough injectives, then its derived $\infty$-category $\mathcal D^-(\mathcal A)$ is stable, admits a $t$-structure, has homotopy category the standard derived category, and satisfies the following universal property: there is a canonical equivalence of abelian categories <code>$\mathcal A\to \mathcal D^-(\mathcal A)^\heartsuit$</code>, and if $\mathcal C$ is a stable $\infty$-category with a left-complete $t$-structure then any right exact functor $\mathcal A\to\mathcal C^\heartsuit$ extends (in an essentially unique way) to an exact functor $\mathcal D^-(\mathcal A)\to \mathcal C$. </p>
http://mathoverflow.net/questions/102730/the-differential-of-the-exponential-map-reductive-homogeneous-space/103192#103192Answer by DamienC for The differential of the exponential map: reductive homogeneous spaceDamienC2012-07-26T13:23:46Z2012-07-26T13:23:46Z<p>I think the formula will be essentially the same. </p>
<p>The formula you wrote is valid in general for the exponential map of analytic manifolds equipped with an analytic affine connection. It is stated and proved in <a href="http://www.mscand.dk/article.php?id=1601" rel="nofollow">this paper</a> by Helgason (see pages 6-7 of the linked .pdf): <em>Some remarks on the exponential mapping of an affine connection. Math. Scand. 9 (l961), l29-l46.</em></p>
<p>The existence of such connections on reductive homogeneous spaces, with an additional invariance property (that you might probably need at some point) is stated and proved in <em>K.Nomizu, Invariant affine connections on homogeneous spaces, Amer. J. Math. 76 (1954), 33-65</em>. </p>
http://mathoverflow.net/questions/102597/history-question-autobiography-of-mathematicians/102618#102618Answer by DamienC for History Question: AUTObiography of MathematiciansDamienC2012-07-19T05:54:34Z2012-07-19T10:11:57Z<p>Récoltes et semailles, by Alexander Grothendieck (available at the Grothendieck circle), might be considered as an autobiography. </p>
http://mathoverflow.net/questions/101619/what-is-the-definition-of-the-l-infty-part-of-a-g-infty-morphism/101656#101656Answer by DamienC for What is the definition of "the $L_\infty$ part of a $G_\infty$ morphism"?DamienC2012-07-08T12:45:08Z2012-07-08T12:45:08Z<p>A $G_\infty$-morphism $\phi$ is determined by structure maps $\phi^{k_1,\dots,k_n}$, $n\geq1$, $k_1,\dots,k_n\geq1$. </p>
<p>The $L_\infty$-part of $\phi$ is the $L_\infty$-morphism $\ell$ with structure maps $\ell^k=\phi^{\overbrace{1,\dots,1}^{k~times}}$. </p>
<p>In order to make this precise you might have to put (de)suspensions at the appropriate places.</p>
http://mathoverflow.net/questions/75588/why-bi-module-bi-bundle-etc/75591#75591Answer by DamienC for Why bi-module, bi-bundle, etc?DamienC2011-09-16T11:35:28Z2012-07-06T15:21:17Z<p>If you work with a single associative algebra $A$, then there is not so much sense to try to define a notion of $A$-tri-module. Namely, $A$-bimodules appear naturally as operadic $A$-modules. </p>
<hr>
<p>To give you a picture, an associative algebra $A$ is in particular an algebra over the colored operad given by intervals of the real line and their disjoint union inclusions (a-k-a <a href="http://math.northwestern.edu/~costello/factorization_public.html" rel="nofollow">prefactorization algebras</a> on the real line). </p>
<p>It has the property to be locally constant: the space associated to any interval is the same ($A$ itself). </p>
<p>Let me now relax a bit this locally constant property. Assume that you have such a (pre)factorization algebra over the real line such that it is locally constant outside the origin. Then you will get two associative algebras (one from $(0,+\infty)$ and the other from $(-\infty,0)$) together with a bunch of bimodules (One for each interval containing the origin). </p>
<p>There is nothing against the idea of having a factorization algebra on the graph consisting of three half-edges attached to a single vertex. Things like this might have appeared in $2d$ lattice models. </p>
http://mathoverflow.net/questions/92988/can-duflo-type-map-be-defined-for-invariant-differential-operators-in-a-way-co/100578#100578Answer by DamienC for Can Duflo type map be defined for invariant differential operators ? (In a way compatible with "Harish-Chandra" isomorphism defined by F. Knop)DamienC2012-06-25T09:35:50Z2012-06-25T09:35:50Z<p>Let $X=T^*M$, and apply Dolgushev's equivariant formality theorem (see <a href="http://arxiv.org/abs/math/0307212" rel="nofollow">http://arxiv.org/abs/math/0307212</a>) to get a $G$-equivariant $L_\infty$-quasi-isomorphism
$$
\mathcal U:T_{poly}X \longrightarrow D_{poly}X
$$</p>
<p>Let $\pi$ be the Poisson structure on $X$ which comes from the canonical symplectic form on $T^*M$. Then one gets a $G$-equiavriant quasi-isomorphism of complexes
$\mathcal U_\pi^1$ from the Poisson cochain complex of $(X,\pi)$ to the Hochschild cochain complex of $(\mathcal O_X,\star_\pi)$, where $\star_\pi$ is the star-product the quantizes $\pi$ through $\mathcal U$. </p>
<p>Moreover, one has a homotopy betwen the cup-product one both sides, and it is $G$-equivariant (compatibility with cup-products is sketched in the original paper of Kontsevich <a href="http://arxiv.org/abs/q-alg/9709040" rel="nofollow">http://arxiv.org/abs/q-alg/9709040</a>, is rigorously proved in <a href="http://arxiv.org/abs/math/0106205" rel="nofollow">http://arxiv.org/abs/math/0106205</a> by Manchon and Torossian, and the globalization is adressed in <a href="http://arxiv.org/abs/0805.3444" rel="nofollow">http://arxiv.org/abs/0805.3444</a> - in this last reference you will easily see that if you start with a $G$-invariant connection to perform globalization then your homotopy will be $G$-invariant too). </p>
<p><strong>Conclusion</strong>. taking $G$-invariants and restricting yourself to the degree zero part of cohomology (Poisson and Hochschil, respectively), you'll find that the Poisson center of $\mathcal O_X^G$ is isomorphic, <em>as an algebra</em>, to the center of the subalgebra of $G$-invariants elements in the quantization. </p>
<p><strong>Things I have been hiding under the carpet</strong>. 1. issues involving $\hbar$. In this case you have to prove that the quantization is actually convergent and can be specialized to $\hbar=1$. 2. You have to prove that the quantization really gives back differential operators... this is probably the more tricky part. </p>
http://mathoverflow.net/questions/98291/are-fully-extended-tqfts-generalized-cohomology-theories/98298#98298Answer by DamienC for Are fully extended TQFTs generalized cohomology theories?DamienC2012-05-29T18:54:33Z2012-06-18T12:14:04Z<p>A fully extended tqft is not quite a generalized homology theory... But almost. You can find a preliminary reference here (notes of a talk by Hiro Tannaka at the mit Talbot workshop):
<a href="http://math.mit.edu/conferences/talbot/2012/notes/14_Tanaka_FactorizationHomology(hiro).pdf" rel="nofollow">http://math.mit.edu/conferences/talbot/2012/notes/14_Tanaka_FactorizationHomology(hiro).pdf</a>
The precise statements you might be interested in are Theorems 2.16 and 2.20. </p>
<p>(side remark: the notes of the whole workshop are worth reading: <a href="http://math.mit.edu/conferences/talbot/2012/notes/talbot_2012_notes(claudia).pdf" rel="nofollow">http://math.mit.edu/conferences/talbot/2012/notes/talbot_2012_notes(claudia).pdf</a>). </p>
<p>EDIT : the work announced in the above talk is now partly available on John Francis' webpage: <a href="http://www.math.northwestern.edu/~jnkf/writ/" rel="nofollow">http://www.math.northwestern.edu/~jnkf/writ/</a> (see "Factorization homology of topological manifolds" and "Structured singular manifolds and factorization homology"). </p>
http://mathoverflow.net/questions/93140/associative-yang-baxter-on-ug/93197#93197Answer by DamienC for associative Yang-Baxter on U(g)DamienC2012-04-05T07:42:15Z2012-04-05T07:42:15Z<p>I don't know about full classification results for $U(\mathfrak{g})$ in general (this is probably out of reach), but there are a bunch of very interesting constructions (together with partial classification resultas) when $A=M_n(\textbf{k})$ and/or when $\mathfrak{g}$ is a semi-simple Lie algebra: </p>
<ul>
<li><p>in the work of Travis Schedler: see e.g. <a href="http://arxiv.org/abs/math/0212258" rel="nofollow">http://arxiv.org/abs/math/0212258</a> (this is very much in the spirit of Belavin-Drinfeld classification of solutions of the classical Yang-Baxter equation for a semi=simple $\mathfrak{g}$)</p></li>
<li><p>in the work of Igor Burban: see e.g. <a href="http://www.mi.uni-koeln.de/~burban/AYBEnewsemistable.pdf" rel="nofollow">http://www.mi.uni-koeln.de/~burban/AYBEnewsemistable.pdf</a> (imo, this is beautiful geometric approach). </p></li>
<li><p>in the original work of Alexander Polishchuk: <a href="http://arxiv.org/abs/math/0008156" rel="nofollow">http://arxiv.org/abs/math/0008156</a></p></li>
</ul>
http://mathoverflow.net/questions/92356/a-infty-basic-reference/92379#92379Answer by DamienC for $A_\infty$ basic referenceDamienC2012-03-27T14:02:02Z2012-03-27T14:02:02Z<p>I believe the thesis of Kenji Lefèvre-Hasegawa is a remarkable piece of work, and is very readable (references spotted by Samuel Tinguely are very good, but they are about $A_\infty$-algebras): </p>
<p><a href="http://www.math.jussieu.fr/~keller/lefevre/TheseFinale/tel-00007761.pdf" rel="nofollow">http://www.math.jussieu.fr/~keller/lefevre/TheseFinale/tel-00007761.pdf</a></p>
<p>Unfortunately it is in only available in French. </p>
http://mathoverflow.net/questions/86414/pbw-theorem-and-multigraded-lie-algebras/86613#86613Answer by DamienC for PBW-Theorem and multigraded Lie algebrasDamienC2012-01-25T10:37:42Z2012-01-25T10:37:42Z<p>As $\mathfrak{a}[0]$-modules we have:
<code>$$
U(\mathfrak{a}_+)[k]=\bigoplus_{\substack{l\geq1 \\ c_1r_1+\cdots+c_lr_l=k}}S^{c_1}(\mathfrak{a}_+[r_1])\otimes\cdots\otimes S^{c_l}(\mathfrak{a}_+[r_l])
$$</code></p>
<p>PS: I assume you work over a field of characteristic zero and I use the isomorphism of graded $\mathfrak a$-modules $S(\mathfrak a)\to U(\mathfrak a)$ given by the symmetrization map. </p>
http://mathoverflow.net/questions/17182/is-an-irreducible-holomorphic-symplectic-manifold-a-simple-lie-algebra/82486#82486Answer by DamienC for Is an irreducible holomorphic symplectic manifold a simple Lie algebra?DamienC2011-12-02T16:54:54Z2012-01-23T13:15:28Z<p>I believe this is a very interesting question, that I have been asking myself for quite a long time. </p>
<p>Nevertheless, I have been told by Prof. Beauville that even in the irreducible case one does not have that
$$
Ext_X(\mathcal O_X,\mathcal O_X)=Ext_X(T_X,T_X)
$$</p>
<p>Namely, consider $X$ being the Hilbert scheme of two points on a $K3$ surface. </p>
<p>Then $Ext_X(\mathcal O_X,\mathcal O_X)=\mathbb{C}\oplus\mathbb{C}[-2]\oplus\mathbb{C}[-4]$. </p>
<p>But <code>$Ext_X(T_X,T_X)=Ext_X(\mathcal O_X,(T^*_X)^{\otimes 2})$</code> contains $Ext_X(\mathcal O_X,\Omega^2_X)$, which is huge ($h^{2,2}=232$). </p>
<p>Anyway, I must say that this does not kill the question (this just tells we have to reformulate it). I hope to be able to write more about it soon. </p>
<p>EDIT: it seems that the answer to the question is NO. The point is that 232 is also the dimension of $H^1(X,S^3(T_X))$ ($X$ is again a $K3$), therefore $Ext_X^1(S^2(T_X),T_X)=RHom_X(\wedge^2(T_X[-1]),T_X[-1]))$ has dimension $\geq232$. </p>
http://mathoverflow.net/questions/85258/is-the-hochschild-chain-complex-c-a-a-a-b-infty-module-over-the-hochschi/85261#85261Answer by DamienC for Is the Hochschild chain complex $C_*(A, A)$ a $B_\infty$-module over the Hochschild cochain complex $C^*(A, A)$?DamienC2012-01-09T15:13:57Z2012-01-11T07:49:52Z<p>This is the subject of Section 2 in <a href="http://arxiv.org/abs/0805.3444" rel="nofollow">that paper</a> (sorry for self-promotion).
Chains actually have two $B_\infty$-module structures (over cochains). Those two module structures are moreover compatible (see Theorem 2.4 of the above paper for a precise statement). </p>
http://mathoverflow.net/questions/32889/a-few-questions-about-kontsevich-formality/81891#81891Answer by DamienC for A few questions about Kontsevich formalityDamienC2011-11-25T14:47:48Z2012-01-10T13:26:01Z<p>Hi Kevin, even if the question is answered I would like to add a few remarks. </p>
<p><strong>(0)</strong> the claim that </p>
<blockquote>
<p>this quasi-isomorphism $U$ is
compatible with the dg algebra
structures on $T$ and $D$</p>
</blockquote>
<p>is not exactly true. It is compatible only on tangent cohomology. </p>
<p><strong>(1)</strong> I agree with Daniel and James that there exists a $G_\infty$-quasi-isomorphism between $T$ and $D$ (this implies compatibility at the level of tangent cohomology, and is strictly stronger). But until recently this was not known if Kontsevich's $L_\infty$-quasi-isomorphism can be upgraded to a $G_\infty$-one. <a href="http://arxiv.org/abs/1109.3520" rel="nofollow">A recent paper of Willwacher</a> solves (in a positive way) this question (EDIT: Willwacher makes the comparison with Tamarkin's $G_\infty$-quasi-isomorphism in Section 10). </p>
<p><strong>(2)</strong> the proof for smooth affine varieties is essentially the same as the one for smooth differentiable manifolds. Both rely </p>
<ul>
<li><p>either on the exitence of a connection in the tangent bundle (see the papers of Dolgushev, e.g. <a href="http://arxiv.org/abs/math/0307212" rel="nofollow">this one</a>). </p></li>
<li><p>or (equivalently) on acyclicity of sheaves of sections of bundles (see e.g. my <a href="http://arxiv.org/abs/0708.2725" rel="nofollow">paper with Michel Van den Bergh</a>). </p></li>
</ul>
<p><strong>(3)</strong> references are </p>
<ul>
<li><p><a href="http://arxiv.org/abs/math/0310399" rel="nofollow">Yekutieli's paper</a> and <a href="http://arxiv.org/abs/math/0603200" rel="nofollow">Van den Bergh'sone</a> for smooth algebraic varieties. </p></li>
<li><p>my <a href="http://arxiv.org/abs/math/0504372" rel="nofollow">paper with Dolgushev and Halbout</a> for complex manifolds. </p></li>
<li><p>the <a href="http://arxiv.org/abs/0708.2725" rel="nofollow">above paper</a> with Van den Bergh for a uniform approach to smooth, complex and algebraic settings (using Lie algebroids). </p></li>
<li><p><a href="http://arxiv.org/abs/math/0605141" rel="nofollow">Dolgushev-Tamarkin-Tsygan paper</a> for the $G_\infty$ version (see also <a href="http://arxiv.org/abs/0710.4510" rel="nofollow">another paper with Van den Bergh</a>). </p></li>
</ul>
<blockquote>
<p>For a general smooth variety, though,
instead of taking the Hochschild
cochain complex of $A=\Gamma(X;\mathcal O_X)$,
presumably we should take the
Hochschild cochain complex of the
(dg?) derived category of $X$. Is this
correct?</p>
</blockquote>
<p>One could do this, but one instead works on the sheaf level. Consider $T$ and $D$ as sheaves and prove that they are $L_\infty$- (or $G_\infty$-)quasi-isomorphic as sheaves of DG Lie (or $G_\infty$)-algebras. </p>
<p><strong>(3+$\epsilon$)</strong> "Deformation quantization of Poisson manifolds, II" does not exist, but there is <a href="http://arxiv.org/abs/math/0106006" rel="nofollow">"Deformation quantization of algebraic varieties"</a> (quite sketchy). You might also be interested by the very inspiring paper <a href="http://arxiv.org/abs/math/9904055" rel="nofollow">"Operads and motives in deformation quantization"</a>. </p>
http://mathoverflow.net/questions/71315/tamarkin-tsygan-formalism/84962#84962Answer by DamienC for Tamarkin-Tsygan FormalismDamienC2012-01-05T14:20:03Z2012-01-05T14:43:44Z<p>Here is a sketch of topological description of a Tamarkin-Tsygan precalculus. </p>
<p>Consider the compactified configuration spaces $C_n$ and $D_{1,n}$ of $n$ points on $\mathbb{R}^2$ and $\mathbb{R}^2-{(0,0)}$, respectively. The collection $(C_n,D_{1,n})_n$ form a topological (colored) operad. </p>
<p><strong>Claim</strong>: the collection <code>$(H_{-\bullet}(C_n,\mathbb{Q}),H_{-\bullet}(D_{1,n},\mathbb{Q}))_n$</code> is the operad of Tamarkin-Tsygan precalculi. </p>
<p>It is well-known that <code>$(H_{-\bullet}(C_n,\mathbb{Q}))_n$</code> is the Gerstenhaber operad. Then the operations $L$ and $i$ are the two classes (of respective degrees $1$ and $0$) in <code>$H_{\bullet}(D_{1,1},\mathbb{Q})=H_{\bullet}(S^1,\mathbb{Q})$</code>. </p>
<p>The two compatibility conditions can be understood as identities in <code>$H_1(D_{1,2},\mathbb{Q})$</code>. </p>
<p>If you want to get the operator $d$ (i.e. get a calulus rather than a precalculus) you'll have to replace $D_{1,n}$ by its semi-direct product with $S^1$. </p>
<p>See also Section 11 (especially $\S 11.3$) of <a href="http://arxiv.org/abs/math/0606241" rel="nofollow">this paper by Kontsevich and Soibelman</a> for a similar point-of-view and its relation to a generalization of Deligne's conjecture. </p>
<hr>
<p>EDIT: there is also an algebraic motivation for the compatibility conditions, which is explained in <a href="http://arxiv.org/abs/math/0002116" rel="nofollow">the original paper of Tamarkin and Tsygan</a>. Namely, if $A$ is a Gerstenhaber algebra then $A[\epsilon]$, with $deg(\epsilon)=1$, is a Gerstenhaber algebra with modified product $a*b=a\cdot b+(-1)^{|a|}\epsilon[a,b]$. And if $(A,M)$ is a precalculus then $M$ becomes a Gerstenhaber module over $A[\epsilon]$ with
$$
(a+\epsilon b)*m=(-1)^{|a|}i_am\quad\textrm{and}\quad [a+\epsilon b,m]=L_am+i_bm
$$</p>
http://mathoverflow.net/questions/70881/duality-between-proper-homotopy-theory-and-strong-shape-theoryDuality between proper homotopy theory and strong shape theoryDamienC2011-07-21T08:09:05Z2011-12-13T17:13:57Z
<p>In the <a href="http://ncatlab.org/nlab/show/shape+theory" rel="nofollow">n-lab entry about shape theory</a> one can read that </p>
<blockquote>
<p>Strong Shape Theory [...] has, especially
in the approach pioneered by Edwards
and Hastings, strong links to proper
homotopy theory. The links are a form
of duality related to some of the more
geometric duality theorems of
classical cohomology.</p>
</blockquote>
<p>I would be interested in any reference where I can find a precise formulation of this duality. </p>
<p>EDIT: according to Gjergji Zaimi's answer the duality might be an improvement of Chapman's complement theorem. One can find it as Theorem 6.5.3 on page 230 of the book by Edwards and Hastings ("Cech and Steenrod Homotopy Theories with Applications to Geometric Topology"). Nevertheless, it seems to me that what was meant on the n-lab entry was more a cohomology type duality (like an instance of Verdier duality in the $(\infty,1)$-ctageorical context). Am I completely wrong?</p>
http://mathoverflow.net/questions/76913/is-the-nc-torus-a-quantum-group/83343#83343Answer by DamienC for Is the nc torus a quantum group?DamienC2011-12-13T15:13:06Z2011-12-13T15:13:06Z<p>Despite the negative result quoted by MTS, there have been some attempts to put a Hopf-like structure on the quantum torus. </p>
<p>One of these attemps, which seems orthogonal to the one mentioned by Pierre in his answer, is <em>via</em> <a href="http://arxiv.org/abs/math/0510421" rel="nofollow">Hopfish algebras</a>. To be short, Hopfish algebras (after Tang-Weinstein-Zhu) are unital algebras equipped a coproduct, a counit and an antipode that are morphisms in the Morita category (they are bimodules,rather than actual algebra morphisms). </p>
<p>The Hopfish structure on the quantum torus has been studied in details in <a href="http://arxiv.org/abs/math/0604405" rel="nofollow">this paper</a>. </p>
<p>To be complete, let me emphazise the following point (taken from the above paper): </p>
<blockquote>
<p>It is important to note that, although
the irrational rotation algebra may be
viewed as a deformation of the algebra
of functions on a 2-dimensional torus,
our hopfish structure is not a
deformation of the Hopf structure
associated with the group structure on
the torus. Rather, the classical limit
of our hopfish structure is a second
symplectic groupoid structure on
$T^∗\mathbb{T}^2$ (...), whose
quantization is the multiplication in
the irrational rotation algebra. We
thus seem to have a symplectic double
groupoid which does not arise from a
Poisson Lie group.</p>
</blockquote>
http://mathoverflow.net/questions/81209/galois-theory-for-polynomials-in-several-variablesGalois theory for polynomials in several variablesDamienC2011-11-17T23:11:34Z2011-12-04T13:37:46Z
<p>I feel a bit ashamed to ask the following question here. </p>
<blockquote>
<p>What is (actually, is there) Galois
theory for polynomials in
$n$-variables for $n\geq2$?</p>
</blockquote>
<p>I am preparing a large audience talk on Lie theory, and decided to start talking about symmetries and take Galois theory as a "baby" example. I know that Lie groups are somehow to differential equations what discrete groups are to algebraic equations. But I nevertheless would expect Lie (or algebraic) groups to appear naturally as higher dimensional analogs of Galois groups. </p>
<p>Namely, the Galois group $G_P$ of a polynomial $P(x)$ in one variable can be defined as the symmetry group of the equation $P(x)=0$ (very shortly, the subgroup of permutations of the solutions/roots that preserves any algebraic equation satisfied by them). </p>
<p>Then one of the great results of Galois theory is that $P(x)=0$ is solvable by radicals if and only if the group $G_P$ is solvable (meaning that its derived series reaches <code>$\{1\}$</code>). </p>
<p>I was wondering what is the analog of the story in higher dimension (i.e. for equations of the form $P(x_1,\dots,x_n)=0$. I would naively expect algebraic group to show up... </p>
<hr>
<p>I googled the main key words and found <a href="http://www.ucl.ac.uk/~ucahmki/sheffield.pdf" rel="nofollow">this presentation</a>: on the last slide it is written that </p>
<blockquote>
<p>the task at hand is to develop a
Galois theory of polynomials in two
variables</p>
</blockquote>
<p>This convinced me to anyway ask the question</p>
<hr>
<p><strong>EDIT: the first "idea" I had</strong></p>
<p>I first thought about the following strategy. Consider $P(x,y)=0$ as an polynomial equation in one variable $x$ with coefficients in the field $k(y)$ of rational functions in $y$, and consider its Galois group. But then we could do the opposite...what would happen?</p>
http://mathoverflow.net/questions/126705/sh-lie-algebra-cohomologyComment by DamienCDamienC2013-04-07T19:52:25Z2013-04-07T19:52:25Z@Jim Conant: higher sh Lie operations have arity in arbitrary positive degree, but they also have an inner cohomological degree which is precisely 1-arity. So that their total degree is still 1. http://mathoverflow.net/questions/124505/the-work-of-pierre-deligneComment by DamienCDamienC2013-03-14T14:26:19Z2013-03-14T14:26:19ZIs this question appropriate for mathoverflow? I personnally believe not: what kind of answer can one expect?http://mathoverflow.net/questions/124404/phd-in-operator-algebras-and-non-commutative-geometry/124410#124410Comment by DamienCDamienC2013-03-13T23:06:38Z2013-03-13T23:06:38ZBenameur is no longer in Metz. He is now in Montpellier. http://mathoverflow.net/questions/119991/is-the-quantum-algebra-unique-up-to-isomorphism-in-deformation-quantization/120089#120089Comment by DamienCDamienC2013-01-28T15:17:12Z2013-01-28T15:17:12Z@Adrien. I think that point 2 is not the content of Dolgushev's paper (though related to it). But your last sentence is correct (and THIS is the main point of 2.).
@Alexander 1. I was just saying that if you make the choice of a local universal formality morphism (i.e. given by weights associated to graphs) then the globalization is essentially unique.
@Alexander 2. this is not what I am saying BUT in the context of the class of a star-product, the Poisson structures you are looking at are of the form $\hbar\pi+\cdots$. wiht a given fixed $\pi$. If $\pi$ is ND then they are all equivalent.http://mathoverflow.net/questions/116137/the-bch-series-in-terms-of-lyndon-wordsComment by DamienCDamienC2012-12-12T08:23:46Z2012-12-12T08:23:46ZIs it really periodic or something more like a sturmian sequence? Namely, if one writes "A" whenever the even and odd guys coincide, and then "B" whenever they don't, then one gets a (semi-)infinite word in two letters "A" and "B". Is this sequence ultimately periodic or sturmian (the later meaning that it is of minimal complexity among non-periodic words)?http://mathoverflow.net/questions/31972/todd-class-and-baker-campbell-hausdorff-or-the-curious-number-12/115488#115488Comment by DamienCDamienC2012-12-05T20:07:55Z2012-12-05T20:07:55ZI actualy mean quasi-coherent sheaves (the action of $T_X[-1]$ on a given one $E$ is given by the Atiyah class of $E$). http://mathoverflow.net/questions/54430/video-lectures-of-mathematics-courses-available-online-for-free/54462#54462Comment by DamienCDamienC2012-12-05T09:28:08Z2012-12-05T09:28:08ZI added the (hyper)link. http://mathoverflow.net/questions/54430/video-lectures-of-mathematics-courses-available-online-for-free/94390#94390Comment by DamienCDamienC2012-12-05T09:22:03Z2012-12-05T09:22:03ZFor me it says "404 Not Found". http://mathoverflow.net/questions/54430/video-lectures-of-mathematics-courses-available-online-for-free/100559#100559Comment by DamienCDamienC2012-12-05T09:18:08Z2012-12-05T09:18:08ZWould you mind giving a link ? :-)http://mathoverflow.net/questions/115369/detadetb-detabcorrection-capelli-identities-factorzied-representatiComment by DamienCDamienC2012-12-04T08:54:05Z2012-12-04T08:54:05ZI would suggest to see if this is true even when you consider non-commutative variables $E_{ij}$ that are not necessarily of the form $a_ib_j$. http://mathoverflow.net/questions/115032/non-rigorous-reasoning-in-rigorous-mathematicsComment by DamienCDamienC2012-12-01T15:54:28Z2012-12-01T15:54:28ZWhy isn't it CW?http://mathoverflow.net/questions/114701/one-more-question-about-pbw/114781#114781Comment by DamienCDamienC2012-11-28T20:13:55Z2012-11-28T20:13:55ZThere is also has a relatively simple example in <a href="http://archive.numdam.org/ARCHIVE/ASNSP/ASNSP_1958_3_12_1-2/ASNSP_1958_3_12_1-2_1_0/ASNSP_1958_3_12_1-2_1_0.pdf" rel="nofollow">archive.numdam.org/ARCHIVE/ASNSP/…</a> (see also the discussion here: <a href="http://mathoverflow.net/questions/61954/" rel="nofollow">mathoverflow.net/questions/61954</a> ). http://mathoverflow.net/questions/114701/one-more-question-about-pbwComment by DamienCDamienC2012-11-28T07:52:15Z2012-11-28T07:52:15ZI know that PBW holds whenever $k\supset\mathbb{Q}$. About my EDIT, this was just a dummy suggestion for a strategy. I was thinking about something like: if $L\to U(L)$ is injective and if PBW holds for $L\otimes_k\mathbb{K}$ (for some $\mathbb{K}$) then PBW holds for $L$http://mathoverflow.net/questions/111433/symplectic-manifold-with-totally-geodesic-foliationComment by DamienCDamienC2012-11-04T14:39:00Z2012-11-04T14:39:00Z@helge. As paolo ghiggini and robert bryant said, if a poisson manifold is symplectic then its symplectic foliation consists of a single leaf. Therefore there is no example of a poisson manifold which is symplectic and have codimension 2 symplectic leaves.http://mathoverflow.net/questions/110613/for-which-calabi-yau-threefolds-is-syz-conjecture-known-to-holdComment by DamienCDamienC2012-10-25T04:52:00Z2012-10-25T04:52:00ZIt seems that the OP is asking for a list... shouldn't it be community wiki then ?