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This soliton preserves two of the sixteen supersymmetries and hence corresponds to N = 1 space-time supersymmetry in (2 + 1) dimensions transverse to the seven dimensions where
Actually, we calculated the brackets on gl(4, C ); the trace of X now becomes a Casimir. If we use a more conventional notation for the matrix X, i.e. There are, however,
From its admitted symmetries or multipliers for conservation laws, one can determine whether or not a given system of differential equations can be linearized by an
The asymptotically leading term of quasinormal modes (QNMs) in the Schwarzschild background, ω n = − in/ 2, is obtained in two straightforward analytical ways for arbitrary spins..
Having no topological analogy with the regular orbits in the geomet- rically corresponding circular billiard, sliding orbits and vortices are well distinguished in the weakly
The aim of this paper is to study orthogonality relations for the discrete q -ultraspherical polyno- mials and their duals by means of operators of representations of the
The fermion- antifermion operators generate a unitary Lie algebra, whose representations are fixed by a first order Casimir operator (corresponding to baryon number or
The Gaussian unitary ensemble with additional symmetry of type ( 3 ) was proposed in the papers [ 1 , 3 ] as an approach to the weak disorder regime in the Anderson model.. In all
