Pages that link to "Item:Q5247570"
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The following pages link to $\frac{{\rm SO}(2N)}{U(N)}$ Riccati–Hartree–Bogoliubov equation based on the <font>SO</font>(2N) Lie algebra of the fermion operators (Q5247570):
Displaying 6 items.
- Path integral on the coset space of the SO\((2N)\) group and the time-dependent Hartree-Bogoliubov equation. (Q2750384) (← links)
- Note on the new type of the SO\((2n+1)\) time-dependent Hartree-Bogoliubov equation. (Q2750481) (← links)
- An equation for the quasiparticle RPA based on the \(\text{SO}(2N+1)\) Lie algebra of the fermion operators. (Q2750574) (← links)
- 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) (← links)
- A new description of motion of the fermionic \(SO(2N+2)\) top in the classical limit under the quasi-anticommutation relation approximation (Q2919210) (← links)
- Mean-field theory based on the Jacobi hsp ≔ semidirect sum hN⋊sp(2N,R)C algebra of boson operators (Q5234064) (← links)
