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    Andrzej Borowiec

    ... The organizing committee Andrzej Borowiec Wojciech Cegla Bernard Jancewicz Witold Karwowski ... HLS Supersymmetry Scheme I. Bandos and J. Lukierski 195 On the Implementation of Supersymmetry D. Buchholz 211 On Generalized Quantum... more
    ... The organizing committee Andrzej Borowiec Wojciech Cegla Bernard Jancewicz Witold Karwowski ... HLS Supersymmetry Scheme I. Bandos and J. Lukierski 195 On the Implementation of Supersymmetry D. Buchholz 211 On Generalized Quantum Statistics W. Marcinek 221 q ...
    ... (36a) SSJ (v+) = −e−σv+ , (36b) SSJ (v−) = −v− eσ + ξhv+eσ − 1 2 ξ v+ eσ eσ + 1 . (36c) 6 Page 8. Supplementing with ǫSJ (v±) = ǫSJ (h) = 0 we obtain the complete set of formulae describing the super-Jordanian deformation Uξ(osp(1|2))... more
    ... (36a) SSJ (v+) = −e−σv+ , (36b) SSJ (v−) = −v− eσ + ξhv+eσ − 1 2 ξ v+ eσ eσ + 1 . (36c) 6 Page 8. Supplementing with ǫSJ (v±) = ǫSJ (h) = 0 we obtain the complete set of formulae describing the super-Jordanian deformation Uξ(osp(1|2)) as non-cocommutative Hopf algebra. ...
    ABSTRACT We briefly analyze some general questions concerning the twist deformation of the Heisenberg double. We reconsider Heisenberg doubles based on quantized Poincaré (Hopf) algebras as illustrative examples. KeywordsHopf... more
    ABSTRACT We briefly analyze some general questions concerning the twist deformation of the Heisenberg double. We reconsider Heisenberg doubles based on quantized Poincaré (Hopf) algebras as illustrative examples. KeywordsHopf algebra–quantum deformation–smash product–Heisenberg double–quantum Poincaré
    ABSTRACT A method is proposed that is appropriate for resolving the Hamiltonian constraint and which leads to a reparametrization-invariant reduced theory specified by a well-defined nonzero local Hamiltonian. This method is based on... more
    ABSTRACT A method is proposed that is appropriate for resolving the Hamiltonian constraint and which leads to a reparametrization-invariant reduced theory specified by a well-defined nonzero local Hamiltonian. This method is based on introducing a global (dependent only on time) conformal variable. The physical and geometric meaning of the variables in the reduced action functional is investigated. It is shown that, within the theory, the method of small perturbations is self-consistent. It is demonstrated that, in the theory of gravity, there are no wavelike excitations that make a negative contribution to the Hamiltonian. From an analysis of the reduced classical theory in the linear approximation, it follows that, at the first instants from the birth of the Universe, the extremely rigid equation of state appeared to be the effective equation of the state of gravity matter.

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