23,354 research outputs found

    Theory of quasiballistic transport through nanocrystalline silicon dots

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    A model to describe the underlying physics of high-energy electron emission from a porous silicon diode is presented. The model is based on an atomistic tight-binding method combined with semiclassical Monte Carlo simulation. It well reproduces essential features of experimental findings. An initial acceleration region is shown to play a crucial role in generating quasiballistic electron emission

    Magnetic strong coupling in a spin-photon system and transition to classical regime

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    We study the energy level structure of the Tavis-Cumming model applied to an ensemble of independent magnetic spins s=1/2s=1/2 coupled to a variable number of photons. Rabi splittings are calculated and their distribution is analyzed as a functin of photon number nmaxn_{\rm max} and spin system size NN. A sharp transition in the distribution of the Rabi frequency is found at nmax≈Nn_{\rm max}\approx N. The width of the Rabi frequency spectrum diverges as N\sqrt{N} at this point. For increased number of photons nmax>Nn_{\rm max}>N, the Rabi frequencies converge to a value proportional to nmax\sqrt{n_{\rm max}}. This behavior is interpreted as analogous to the classical spin resonance mechanism where the photon is treated as a classical field and one resonance peak is expected. We also present experimental data demonstrating cooperative, magnetic strong coupling between a spin system and photons, measured at room temperature. This points towards quantum computing implementation with magnetic spins, using cavity quantum-electrodynamics techniques.Comment: Received 8 April 2010; revised manuscript received 17 June 2010; published 14 July 201

    Scaling properties of the relaxation time near the mean-field spinodal

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    We study the relaxation processes of the infinitely long-range interaction model (the Husimi-Temperley model) near the spinodal point. We propose a unified finite-size scaling function near the spinodal point, including the metastable region, the spinodal point, and the unstable region. We explicitly adopt the Glauber dynamics, derive a master equation for the probability distribution of the total magnetization, and perform the so-called van Kampen Omega expansion (an expansion in terms of the inverse of the systems size), which leads to a Fokker-Planck equation. We analyze the scaling properties of the Fokker-Planck equation and confirm the obtained scaling plot by direct numerical solution of the original master equation, and by kinetic Monte Carlo simulation of the stochastic decay process.Comment: 9 pages, 3 figure

    Light Scalar Mesons as Manifestation of Spontaneously Broken Chiral Symmetry

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    Attention is paid to the production mechanisms of light scalars that reveal their nature. We reveal the chiral shielding of the \sigma(600) meson. We show that the kaon loop mechanism of the \phi radiative decays, ratified by experiment, points to the four-quark nature of light scalars. We show also that the light scalars are produced in the two photon collisions via four-quark transitions in contrast to the classic P wave tensor q\bar q mesons that are produced via two-quark transitions γγ→qqˉ\gamma\gamma\to q\bar q. The history of spontaneous breaking of symmetry in quantum physics is discussed in Appendix.Comment: Talk at The International Bogolyubov Conference "Problems of Theoretical and Mathematical Physics" devoted to the 100th anniversary of N.N.Bogolyubov's birth that was held from August 21 to August 22,2009 in Moscow at the Russian Academy of Sciences (RAS) and from August 23 to August 27, 2009 in Dubna at the Joint Institute for Nuclear Research (JINR

    Multi-Orbital Molecular Compound (TTM-TTP)I_3: Effective Model and Fragment Decomposition

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    The electronic structure of the molecular compound (TTM-TTP)I_3, which exhibits a peculiar intra-molecular charge ordering, has been studied using multi-configuration ab initio calculations. First we derive an effective Hubbard-type model based on the molecular orbitals (MOs) of TTM-TTP; we set up a two-orbital Hamiltonian for the two MOs near the Fermi energy and determine its full parameters: the transfer integrals, the Coulomb and exchange interactions. The tight-binding band structure obtained from these transfer integrals is consistent with the result of the direct band calculation based on density functional theory. Then, by decomposing the frontier MOs into two parts, i.e., fragments, we find that the stacked TTM-TTP molecules can be described by a two-leg ladder model, while the inter-fragment Coulomb energies are scaled to the inverse of their distances. This result indicates that the fragment picture that we proposed earlier [M.-L. Bonnet et al.: J. Chem. Phys. 132 (2010) 214705] successfully describes the low-energy properties of this compound.Comment: 5 pages, 4 figures, published versio

    Lightest scalar and tensor resonances in γγ→ππ\gamma\gamma\to\pi\pi after the Belle experiment

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    New high statistics Belle data on the γγ→π+π−\gamma\gamma\to\pi^+\pi^- reaction cross section measured in the range of pion-pair invariant masses s\sqrt{s} between 0.8 GeV and 1.5 GeV are analyzed to clarify the current situation around the σ(600)\sigma(600), f0(980)f_0(980), and f2(1270)f_2(1270) resonances in γγ\gamma\gamma collisions. The present analysis shows that the direct coupling constants of the σ(600)\sigma(600) and f0(980)f_0(980) resonances to γγ\gamma\gamma are small, and the σ(600)→γγ\sigma(600)\to\gamma\gamma and f0(980)→γγf_0(980)\to\gamma\gamma decays are four-quark transitions caused by the π+π−\pi^+\pi^- and K+K−K^+K^- loop mechanisms, respectively. The chiral shielding of the σ(600)\sigma(600) resonance takes place in the reactions γγ→ππ\gamma\gamma\to\pi\pi as well as in ππ\pi\pi scattering. Some results of a simultaneous description of the γγ→π+π−\gamma\gamma\to\pi^+\pi^- and γγ→π0π0\gamma\gamma\to\pi^0\pi^0 Belle data are also presented. In particular, the following tentative estimate of the f2(1270)→γγf_2(1270)\to\gamma\gamma decay width is obtained: Γf2→γγ(mf22)≈3.68\Gamma_{f_2\to\gamma\gamma}(m^2_{f_2})\approx 3.68 keV.Comment: 14 pages, 5 figures. Fitted for the publication in Physical Review
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