AbstractLet M be the flat Minkowski space. The solutions of the wave equation, the Dirac equations, the Maxwell equations, or more generally the mass 0, spin s equations are invariant under a multiplier representation Us, of the conformal group. We provide the space of distributions solutions of the mass 0, spin s equations with a Hilbert space structure Hs, such that the representation Us, will act unitarily on Hs. We prove that the mass 0 equations give intertwining operators between representations of principal series. We relate these representations to the Segal-Shale-Weil (or “ladder”) representation of U(2, 2)
This is the first in a series of papers devoted to an analogue of the metaplectic representation, na...
Considering spin degrees of freedom incorporated in the conformal generators, we introduce an intrin...
This paper is a continuation and elaboration of our brief notice quant-ph/0206044 (Nucl. Phys. B, 19...
AbstractIt is shown that there exist conformally covariant differential operators D2l,k of all even ...
AbstractIt is shown that there exist conformally covariant differential operators D2l,k of all even ...
Unitary irreducible representations of the homogeneous Lorentz group O(3, 1) belonging to the princi...
For the group O(p, q) we give a new construction of its minimal unitary represen-tation via Euclidea...
AbstractLet G be a real reductive Lie group and G/H a reductive homogeneous space. We consider Kosta...
First-order relativistic wave equations are considered whose irreducible matrix coefficients satisfy...
AbstractThis is the first in a series of papers devoted to an analogue of the metaplectic representa...
AbstractWe extend from themasslessto themassivecase the canonical conformal mapping of solutions of ...
Bound and scattering state Schr\"odinger functions of nonrelativistic quantum mechanics as represent...
Considering all representations S(Λ) of the proper Lorentz group which are equivalent to the di...
AbstractFor the group O(p,q) we give a new construction of its minimal unitary representation via Eu...
In a recent paper Dirac has shown that by passing from the ordinary Euclidean space to a four-dimens...
This is the first in a series of papers devoted to an analogue of the metaplectic representation, na...
Considering spin degrees of freedom incorporated in the conformal generators, we introduce an intrin...
This paper is a continuation and elaboration of our brief notice quant-ph/0206044 (Nucl. Phys. B, 19...
AbstractIt is shown that there exist conformally covariant differential operators D2l,k of all even ...
AbstractIt is shown that there exist conformally covariant differential operators D2l,k of all even ...
Unitary irreducible representations of the homogeneous Lorentz group O(3, 1) belonging to the princi...
For the group O(p, q) we give a new construction of its minimal unitary represen-tation via Euclidea...
AbstractLet G be a real reductive Lie group and G/H a reductive homogeneous space. We consider Kosta...
First-order relativistic wave equations are considered whose irreducible matrix coefficients satisfy...
AbstractThis is the first in a series of papers devoted to an analogue of the metaplectic representa...
AbstractWe extend from themasslessto themassivecase the canonical conformal mapping of solutions of ...
Bound and scattering state Schr\"odinger functions of nonrelativistic quantum mechanics as represent...
Considering all representations S(Λ) of the proper Lorentz group which are equivalent to the di...
AbstractFor the group O(p,q) we give a new construction of its minimal unitary representation via Eu...
In a recent paper Dirac has shown that by passing from the ordinary Euclidean space to a four-dimens...
This is the first in a series of papers devoted to an analogue of the metaplectic representation, na...
Considering spin degrees of freedom incorporated in the conformal generators, we introduce an intrin...
This paper is a continuation and elaboration of our brief notice quant-ph/0206044 (Nucl. Phys. B, 19...