On (2)-relative cohomology of the Lie algebra of vector fields and differential operators |
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Abstract: | Abstract Let Vect(?) be the Lie algebra of smooth vector fields on ?. The space of symbols Pol(T*?) admits a non-trivial deformation (given by differential operators on weighted densities) as a Vect(?)-module that becomes trivial once the action is restricted to ![/></span>(2) ? Vect(?). The deformations of Pol(<i>T</i>*?), which become trivial once the action is restricted to <span class=](/na101/home/literatum/publisher/tandf/journals/content/tnmp20/2007/tnmp20.v014.i01/jnmp.2007.14.1.9/20130121/images/medium/tnmp_a_10595428_o_ilf0001.gif) ![/></span>(2) and such that the Vect(?)-action on them is expressed in terms of differential operators, are classified by the elements of the weight basis of <span class=](/na101/home/literatum/publisher/tandf/journals/content/tnmp20/2007/tnmp20.v014.i01/jnmp.2007.14.1.9/20130121/images/medium/tnmp_a_10595428_o_ilf0001.gif) ![/></span>, where <span class=](/na101/home/literatum/publisher/tandf/journals/content/tnmp20/2007/tnmp20.v014.i01/jnmp.2007.14.1.9/20130121/images/medium/tnmp_a_10595428_o_ilf0002.gif) ![/></span> denotes the differential cohomology (i.e., we consider only cochains that are given by differential operators) and where <i>D</i> <sub>λ,μ</sub> = Homdiff(<i>F</i> <sub>λ</sub>, <i>F</i> <sub>μ</sub>) is the space of differential operators acting on weighted densities. The main result of this paper is computation of this cohomology. In addition to relative cohomology, we exhibit 2-cocycles spanning <span class=](/na101/home/literatum/publisher/tandf/journals/content/tnmp20/2007/tnmp20.v014.i01/jnmp.2007.14.1.9/20130121/images/medium/tnmp_a_10595428_o_ilf0003.gif) ![/></span> and <span class=](/na101/home/literatum/publisher/tandf/journals/content/tnmp20/2007/tnmp20.v014.i01/jnmp.2007.14.1.9/20130121/images/medium/tnmp_a_10595428_o_ilf0004.gif) ![/></span>(2).</td>
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