456 research outputs found

    O QUE D. W. WINNICOTT DIRIA A D. HUME? SOBRE A IDENTIDADE PESSOAL/ WHAT WOULD D. W. WINNICOTT SAY TO D. HUME? AN ANALYSIS OF PERSONAL IDENTITY

    Get PDF
    Apresentaremos neste texto a tese de David Hume sobre a identidade pessoal tal como é apresentada no Tratado da natureza humana, de sua autoria. No apêndice da obra, Hume apresenta dúvidas sobre a tese que defendeu, apontando uma série de problemas que não se resolvem em sua teoria. Mas o tratamento desses problemas e uma possível resposta a Hume podem ser encontrados em D. W. Winnicott

    Quantum entanglement of bound particles under free center of mass dispersion

    Full text link
    On the basis of the full analytical solution of the overall unitary dynamics, the time evolution of entanglement is studied in a simple bipartite model system evolving unitarily from a pure initial state. The system consists of two particles in one spacial dimension bound by harmonic forces and having its free center of mass initially localized in space in a minimum uncertainty wave packet. The existence of such initial states in which the bound particles are not entangled is pointed out. The entanglement of the two particles is shown to be independent of the wavepacket mean momentum, and to increase monotonically in a time scale distinct from that of the spreading of the center of mass wavepacket.Comment: 17 pages, 5 figure

    Violation of the Ikeda sum rule and the self-consistency in the renormalized quasiparticle random phase approximation and the nuclear double-beta decay

    Full text link
    The effect of the inclusion of ground state correlations into the QRPA equation of motion for the two-neutrino double beta (ββ2ν\beta\beta_{2\nu}) decay is carefully analyzed. The resulting model, called renormalized QRPA (RQRPA), does not collapse near the physical value of the nuclear force strength in the particle-particle channel, as happens with the ordinary QRPA. Still, the ββ2ν\beta\beta_{2\nu} transition amplitude is only slightly less sensitive on this parameter in the RQRPA than that in the plain QRPA. It is argued that this fact reveals once more that the characteristic behaviour of the ββ2ν\beta\beta_{2\nu} transition amplitude within the QRPA is not an artifact of the model, but a consequence of the partial restoration of the spin-isospin SU(4)SU(4) symmetry. It is shown that the price paid for bypassing the collapse in the RQRPA is the violation of the Ikeda sum rule.Comment: 16 pages, latex, 3 postscript figure

    Self Consistent and Renormalized particle-particle RPA in a Schematic Model

    Get PDF
    The dynamical effects of ground state correlations for excitation energies and transition strengths near the superfluid phase transition are studied in the soluble two level pairing model, in the context of the particle-particle self consistent Random Phase Approximation (SCRPA). Exact results are well reproduced across the transition region, beyond the collapse of the standard particle-particle Random Phase Approximation. The effects of two-body correlation in the SCRPA are displayed explicitly.Comment: 11 pages, revtex, 3ps figures, to appear in Phys. Rev.

    Population Dynamics in the Penna Model

    Full text link
    We build upon the recent steady-state Penna model solution, Phys.Rev.Lett. 89, 288103 (2002), to study the population dynamics within the Penna model. We show, that any perturbation to the population can be broken into a collection of modes each of which decay exponentially with its respective time constant. The long time behaviour of population is therefore likely to be dominated by the modes with the largest time constants. We confirm our analytical approach with simulation data.Comment: 6 figure

    Time Evolution of tunneling and decoherence: soluble model

    Get PDF
    Decoherence effects associated to the damping of a tunneling two-level system are shown to dominate the tunneling probability at short times in strong coupling regimes in the context of a soluble model. A general decomposition of tunneling rates in dissipative and unitary parts is implemented. Master equation treatments fail to describe the model system correctly when more than a single relaxation time is involved
    corecore