66,327 research outputs found

    Improvement of Uncertainty Relations for Mixed States

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    We study a possible improvement of uncertainty relations. The Heisenberg uncertainty relation employs commutator of a pair of conjugate observables to set the limit of quantum measurement of the observables. The Schroedinger uncertainty relation improves the Heisenberg uncertainty relation by adding the correlation in terms of anti-commutator. However both relations are insensitive whether the state used is pure or mixed. We improve the uncertainty relations by introducing additional terms which measure the mixtureness of the state. For the momentum and position operators as conjugate observables and for the thermal state of quantum harmonic oscillator, it turns out that the equalities in the improved uncertainty relations hold

    Radial transonic shock solutions of Euler-Poisson system in convergent nozzles

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    Given constant data of density ρ0\rho_0, velocity βˆ’u0er-u_0{\bf e}_r, pressure p0p_0 and electric force βˆ’E0er-E_0{\bf e}_r for supersonic flow at the entrance, and constant pressure pexp_{\rm ex} for subsonic flow at the exit, we prove that Euler-Poisson system admits a unique transonic shock solution in a two dimensional convergent nozzle, provided that u0>0u_0>0, E0>0E_0>0, and that E0E_0 is sufficiently large depending on (ρ0,u0,p0)(\rho_0, u_0, p_0) and the length of the nozzle

    Scaling of Coulomb pseudo-potential in s-wave narrow-band superconductors

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    The Coulomb pseudo-potential ΞΌβˆ—\mu^* is extracted by fitting the numerically calculated transition temperature TcT_c of the Eliashberg-Nambu equation which is extended to incorporate the narrow-band effects, that is, the vertex correction and the frequency dependence of the screened Coulomb interaction. It is shown that even for narrow-band superconductors, where the fermi energy Ο΅F \epsilon_F is comparable with the phonon frequency Ο‰ph \omega_{ph}, the Coulomb pseudo-potential is a pertinent parameter, and is still given by ΞΌβˆ—=ΞΌ/[1+ΞΌln⁑(Ο΅F/Ο‰ph)]\mu^* = \mu/[1+\mu \ln(\epsilon_F/\omega_{ph})] , provided Ο‰ph\omega_{ph} is appropriately scaled.Comment: 5 pages, 3 figures, accepted for publication by Phys. Rev.
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