Differential operators | Differential geometry

Invariant differential operator

In mathematics and theoretical physics, an invariant differential operator is a kind of mathematical map from some objects to an object of similar type. These objects are typically functions on , functions on a manifold, vector valued functions, vector fields, or, more generally, sections of a vector bundle. In an invariant differential operator , the term differential operator indicates that the value of the map depends only on and the derivatives of in . The word invariant indicates that the operator contains some symmetry. This means that there is a group with a group action on the functions (or other objects in question) and this action is preserved by the operator: Usually, the action of the group has the meaning of a change of coordinates (change of observer) and the invariance means that the operator has the same expression in all admissible coordinates. (Wikipedia).

Invariant differential operator
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Related pages

Differential operator | Poincaré group | Lie group | Differential form | Exterior derivative | Invariant (mathematics) | Derivative | Gradient | Group (mathematics) | Section (category theory) | Map (mathematics) | Connection (mathematics) | Parabolic geometry (differential geometry) | Representation (mathematics) | Laplace invariant | Mathematics | Conformal geometry | Function (mathematics) | Dirac operator | Sphere | Euclidean space | Vector bundle | Manifold | Projective geometry | Torsion tensor | Generalized Verma module | Homogeneous space | Symmetry in mathematics | Invariant factorization of LPDOs | Vector field | Pullback (differential geometry)