Modified non-Euclidean transformation on the \(\frac{\mathrm{SO}(2N+2)}{U(N+1)}\) Grassmannian and \(\mathrm{SO}(2N+1)\) random phase approximation for unified description of Bose and Fermi type collective excitations (Q2805563)
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scientific article; zbMATH DE number 6579764
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | Modified non-Euclidean transformation on the \(\frac{\mathrm{SO}(2N+2)}{U(N+1)}\) Grassmannian and \(\mathrm{SO}(2N+1)\) random phase approximation for unified description of Bose and Fermi type collective excitations |
scientific article; zbMATH DE number 6579764 |
Statements
12 May 2016
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Hartree-Bogoliubov formalism
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\(\mathrm{SO}(2N)\) and \(\mathrm{SO}(2N+1)\) Lie algebras
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TD Hartree-Bogoliubov equation
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\(\mathrm{SO}(2N+1)\) random phase approximation
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Modified non-Euclidean transformation on the \(\frac{\mathrm{SO}(2N+2)}{U(N+1)}\) Grassmannian and \(\mathrm{SO}(2N+1)\) random phase approximation for unified description of Bose and Fermi type collective excitations (English)
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