
The space of linear differential operators on a smooth manifold $M$ has a natural one-parameter family of $Diff(M)$ (and $Vect(M)$)-module structures, defined by their action on the space of tensor-densities. It is shown that, in the case of second order differential operators, the $Vect(M)$-module structures are equivalent for any degree of tensor-densities except for three critical values: $\{0,{1\over 2},1\}$. Second order analogue of the Lie derivative appears as an intertwining operator between the spaces of second order differential operators on tensor-densities.
20 pages, CPT-preprint Marseille
High Energy Physics - Theory, Lie algebras of vector fields and related (super) algebras, Mathematics(all), critical values, High Energy Physics - Theory (hep-th), Applications of Lie groups to the sciences; explicit representations, second-order linear differential operators, FOS: Physical sciences, Lie algebra of vector fields, tensor
High Energy Physics - Theory, Lie algebras of vector fields and related (super) algebras, Mathematics(all), critical values, High Energy Physics - Theory (hep-th), Applications of Lie groups to the sciences; explicit representations, second-order linear differential operators, FOS: Physical sciences, Lie algebra of vector fields, tensor
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