Axially-symmetric topological configurations in the skyrme and faddeev chiral models, in the Skyrme model (SM) the field is given by the
unitary matrix U ∈ SU(2), and in the Faddeev model (FM
On condensed forms for partially commuting matrices this fact, we show an economical way to find a spanning set for the
matrix algebra generated by Laffey
Mechanical Properties of Carbon Nanotubes in a Chiral Model of Graphene introduce a
unitary matrix (U) as an order parameter and suggest a scalar chiral model of graphene
Mechanical and electromagnetic properties of fullerenes in chiral model of graphene a
unitary matrix as an order parameter and suggest a scalar chiral model of graphene
Boundary Morera Theorem for the Matrix Ball of the Third TypeKhudayberganov, Gulmirza Kh.,
Otemuratov, Bayram P.,
Rakhmonov, Uktam S.,
Худайберганов, Гулмирза Х.,
Отемуратов, Байрам П.,
Рахмонов, Уктам С. In the article we consider a boundary version of Morera’s theorem for the
matrix ball of the third
Simple Pre-Steering Constraints for Wideband LCMV-beamformer-diagonal
matrix. In a case when DOA is the broadside,
simple constraints are equal to Frost’s constraints.
Simple Pre-Steering Constraints for Wideband LCMV-beamformer-diagonal
matrix. In a case when DOA is the broadside, simple constraints are equal to Frost's constraints.
Absolute continuity of spectral shift for functions of contractions, dissipative operators,
unitary operators and self-adjoint operators. To establish