The response of isovector and isoscalar pairing to generalized rotation in isospace is studied. Analytical expressions for non-selfconsistent solutions for different limiting cases of the model are derived. In particular, the connections between gauge relations among pairing gaps and the position of the isocranking axis are investigated in $N$=$Z$ nuclei. The two domains of collective and non-collective rotation in space are generalized to isospace. The amplitudes for pair-transfer of T=0 and T=1 pairs are also calculated. It is shown that the structure of the T=0 state in odd-odd nuclei prevents any enhancement of pairing transfer also in the presence of strong T=0 correlations. The energy differences of the T=0 and T=1 excitations in odd-...
Supersymmetric models with broken R-parity induced by lepton number violating terms provide a calcul...
We show that the degenerate positive-norm physical propagating fields of the open bosonic string can...
Some time ago Salmhofer demonstrated the equivalence of the strong coupling lattice Schwinger model ...
Two dimensional SU(N) Yang-Mills theory is known to be equivalent to a string theory, as found by Gr...
We extend a procedure for construction of the photon position operators with transverse eigenvectors...
Following our earlier investigations we examine the quantum-classical winding number transition in t...
We investigate particular models which can be N-fold supersymmetric at specific values of a paramete...
The shell model within the $2s1d0g_{7/2}0h_{11/2}$ shell is applied to calculate nuclear structure p...
We construct and study a matrix model that describes two dimensional string theory in the Euclidean ...
The microscopic quasiparticle-phonon model, MQPM, is used to study the energy spectra of the odd $Z=...
A general discussion and illustration is given of strength functions for rotational transitions in t...
We obtain an almost perfect monopole action numerically after abelianprojection in pure SU(3) lattic...
An SU(3) chiral Lagrangian for the lightest decuplet of baryons is constructed on a discrete lattice...
The two opposite concepts - multiphoton and effective photon - readily describing the photoelectric ...
The quantum hadrodynamics (QHD) model with minimal nucleon-meson couplings is generalized by introdu...
Supersymmetric models with broken R-parity induced by lepton number violating terms provide a calcul...
We show that the degenerate positive-norm physical propagating fields of the open bosonic string can...
Some time ago Salmhofer demonstrated the equivalence of the strong coupling lattice Schwinger model ...
Two dimensional SU(N) Yang-Mills theory is known to be equivalent to a string theory, as found by Gr...
We extend a procedure for construction of the photon position operators with transverse eigenvectors...
Following our earlier investigations we examine the quantum-classical winding number transition in t...
We investigate particular models which can be N-fold supersymmetric at specific values of a paramete...
The shell model within the $2s1d0g_{7/2}0h_{11/2}$ shell is applied to calculate nuclear structure p...
We construct and study a matrix model that describes two dimensional string theory in the Euclidean ...
The microscopic quasiparticle-phonon model, MQPM, is used to study the energy spectra of the odd $Z=...
A general discussion and illustration is given of strength functions for rotational transitions in t...
We obtain an almost perfect monopole action numerically after abelianprojection in pure SU(3) lattic...
An SU(3) chiral Lagrangian for the lightest decuplet of baryons is constructed on a discrete lattice...
The two opposite concepts - multiphoton and effective photon - readily describing the photoelectric ...
The quantum hadrodynamics (QHD) model with minimal nucleon-meson couplings is generalized by introdu...
Supersymmetric models with broken R-parity induced by lepton number violating terms provide a calcul...
We show that the degenerate positive-norm physical propagating fields of the open bosonic string can...
Some time ago Salmhofer demonstrated the equivalence of the strong coupling lattice Schwinger model ...