The master analytic function and the Lorentz group. III. Coupling of continuous representations of O(2,1)
DOI10.1063/1.524100zbMath0415.22007OpenAlexW1969784213MaRDI QIDQ3050645
Debabrata Basu, S. Datta Majumdar
Publication date: 1979
Published in: Journal of Mathematical Physics (Search for Journal in Brave)
Full work available at URL: https://doi.org/10.1063/1.524100
Burchnall-Chaundy formulaClebsch-Gordan coefficientsLorentz groupprincipal seriescontinuous representationsSommerfeld-Watson transformationSturm-Liouville theory of differential equations
Applications of Lie groups to the sciences; explicit representations (22E70) Structure and representation of the Lorentz group (22E43)
Related Items (3)
Cites Work
- A general study of the Wigner coefficients of \(\mathrm{SU}(1,1)\)
- Irreducible unitary representations of the Lorentz group
- On the Kronecker Products of Irreducible Representations of the 2 × 2 Real Unimodular Group. I
- The Clebsch-Gordan problem and coefficients for the three-dimensional Lorentz group in a continuous basis. IV
- Some new identities of the Clebsch–Gordan coefficients and representation functions of SO(2,1) and SO(4)
- The master analytic function and the Lorentz group. I. Reduction of the representations of O(3,1) in O(2,1) basis
- The master analytic function and the Lorentz group. II. The Clebsch–Gordan problem for O(2,1)
- Note on the representation spaces of O(2,1)
- On non-compact groups. II. Representations of the 2+1 Lorentz group
- On the wigner coefficients of the three-dimensional Lorentz group
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