998 research outputs found

    Shock Theory of a Bubbly Liquid in a Deformable Tube

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    Shock propagation through a bubbly liquid filled in a deformable cylindrical tube is considered. Quasi-one-dimensional bubbly flow equations that include fluid-structure interaction are formulated, and the steady shock relations are derived. Experiments are conducted in which a free-falling steel projectile impacts the top of an air/water mixture in a polycarbonate tube, and stress waves in the tube material are measured. The experimental data indicate that the linear theory cannot properly predict the propagation speeds of shock waves in mixture-filled tubes; the shock theory is found to more accurately estimate the measured wave speeds

    Electron Mass Enhancement due to Anharmonic Local Phonons

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    In order to understand how electron effective mass is enhanced by anharmonic local oscillation of an atom in a cage composed of other atoms, i.e., {\it rattling}, we analyze anharmonic Holstein model by using a Green's function method. Due to the evaluation of an electron mass enhancement factor ZZ, we find that ZZ becomes maximum when zero-point energy is comparable with potential height at which the amplitude of oscillation is rapidly enlarged. Cooperation of such quantum and rattling effects is considered to be a key issue to explain the electron mass enhancement in electron-rattling systems.Comment: 3 pages, 3 figures, to appear in J. Phys. Soc. Jpn. Suppl. (Proceedings for International Conference on Heavy Electrons

    Shock propagation through a bubbly liquid in a deformable tube

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    Shock propagation through a bubbly liquid contained in a deformable tube is considered. Quasi-one-dimensional mixture-averaged flow equations that include fluid–structure interaction are formulated. The steady shock relations are derived and the nonlinear effect due to the gas-phase compressibility is examined. Experiments are conducted in which a free-falling steel projectile impacts the top of an air/water mixture in a polycarbonate tube, and stress waves in the tube material and pressure on the tube wall are measured. The experimental data indicate that the linear theory is incapable of properly predicting the propagation speeds of finite-amplitude waves in a mixture-filled tube; the shock theory is found to more accurately estimate the measured wave speeds

    Realization of Strong Coupling Fixed Point in Multilevel Kondo Models

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    Impurity four- and six-level Kondo model, in which an ion is tunneling among four- and six-stable points and interacting with surrounding conduction electrons, are investigated by using the perturbative and numerical renormalization group methods. It is shown that purely orbital Kondo effects occur at low temperatures in these systems which are direct generalizations of the Kondo effect in the so-called two-level system. This result offers a good explanation for the enhanced and magnetically robust Sommerfeld coefficient observed in SmOs_4Sb_12 and some other filled-skutterudites.Comment: 3 pages, 3 figures, for proceedings of ASR-WYP-2005. To be published in Journal of Physical Society Japan supplemen

    Universality in heavy-fermion systems with general degeneracy

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    We discuss the relation between the T^{2}-coefficient of electrical resistivity AA and the T-linear specific-heat coefficient γ\gamma for heavy-fermion systems with general NN, where NN is the degeneracy of quasi-particles. A set of experimental data reveals that the Kadowaki-Woods relation; A/γ2=1105μΩ(Kmol/mJ)2A/\gamma^{2} = 1*10^{-5} {\mu\Omega}(K mol/mJ)^{2}, collapses remarkably for large-N systems, although this relation has been regarded to be commonly applicable to the Fermi-liquids. Instead, based on the Fermi-liquid theory we propose a new relation; A~/γ~2=1×105\tilde{A}/\tilde{\gamma}^2=1\times10^{-5} with A~=A/(1/2)N(N1)\tilde{A} = A/(1/2)N(N-1) and γ~=γ/(1/2)N(N1)\tilde{\gamma} = \gamma/(1/2)N(N-1). This new relation exhibits an excellent agreement with the data for whole the range of degenerate heavy-fermions.Comment: 2 figures, to appear in Phys. Rev. Let
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