2,779 research outputs found

    Vortex pinning in high-Tc materials via randomly oriented columnar defects, created by GeV proton-induced fission fragments

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    Extensive work has shown that irradiation with 0.8 GeV protons can produce randomly oriented columnar defects (CD's) in a large number of HTS materials, specifically those cuprates containing Hg, Tl, Pb, Bi, and similar heavy elements. Absorbing the incident proton causes the nucleus of these species to fission, and the recoiling fission fragments create amorphous tracks, i.e., CD's. The superconductive transition temperature Tc decreases linearly with proton fluence and we analyze how the rate depends on the family of superconductors. In a study of Tl-2212 materials, adding defects decreases the equilibrium magnetization Meq(H) significantly in magnitude and changes its field dependence; this result is modeled in terms of vortex pinning. Analysis of the irreversible magnetization and its time dependence shows marked increases in the persistent current density and effective pinning energy, and leads to an estimate for the elementary attempt time for vortex hopping, tau ~ 4x10^(-9) s.Comment: Submitted to Physica C; presentation at ISS-2001. PDF file only, 13 pp. tota

    Functional changes in motor endplates of the target muscle after amputation of the C7 nerve root

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    There are limited data on structural and functional changes in motor endplates and muscle fibers in the target muscle following amputation of the 7th cervical nerve root, a transplantation-related procedure in surgical treatment in the case of avulsions of the brachial plexus roots. We examined functional changes in these structures using stimulated singlefiber electromyography (sSF-EMG) in an animal model. Unilateral amputation of the 7th cervical nerve root was performed in 36 male rats, and the m. triceps brachii muscle was tested by sSF-EMG at different time points. We observed significant differences in the jitter (mean consecutive difference, MCD, of the latencies between adjacent muscle fibers) at postamputation weeks 1, 2, 4, and 6. The post-operation fiber density (FD) values within the zone of effective stimulation also gradually increased. At post-amputation weeks 8 and 12, the jitter values returned to normal levels, whereas FD values continued to rise. Our results indicate that the post-amputation compensatory processes in the target muscles of the 7th cervical nerve root are completed at 9-12 weeks after amputation.Дані щодо структурних та функціональних змін у моторних кінцевих пластинках та м’язових волокнах м’яза-цілі після ампутації сьомого шийного нервового корінця (процедури в рамках трансплантаційного хірургічного лікування наслідків відриву корінців брахіального сплетіння) поки що обмежені. Ми досліджували функціональні зміни в згаданих структурах, використовуючи методику стимуляційної „одноволоконної” електроміографії в умовах експериментальної моделі на тваринах. Унілатеральну ампутацію сьомого цервікального нервового корінця було виконано на 36 щурах-самцях, і триголові м’язи плеча тестувалися за допомогою згаданої ЕМГ-методики в різні часові інтервали. Ми виявили істотні відмінності середніх варіацій („дрижання”, jitter, різниць між послідовними величинами) латентних періодів, характерних для прилеглих одне до одного м’язових волокон, у перший, другий, четвертий та шостий тижні після операційного періоду. В цей час щільність волокон у зоні ефективної стимуляції також поступово зростала. На восьмий–12-й тижні післяопераційного періоду значення варіацій („дрижання”) поверталися до нормальних, тоді як значення щільності активованих волокон продовжували зростати. Наші результати свідчать про те, що післяампутаційні компенсаторні процеси в м’язах-цілях волокон нервового корінця С7 завершуються через дев’ять–12 тижнів після ампутації останнього

    Tunneling spectra of submicron Bi2_2Sr2_2CaCu2_2O8+δ_{8+\delta} intrinsic Josephson junctions: evolution from superconducting gap to pseudogap

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    Tunneling spectra of near optimally doped, submicron Bi2_2Sr2_2CaCu2_2O8+δ_{8+\delta} intrinsic Josephson junctions are presented, and examined in the region where the superconducting gap evolves into pseudogap. The spectra are analyzed using a self-energy model, proposed by Norman {\it et al.}, in which both quasiparticle scattering rate Γ\Gamma and pair decay rate ΓΔ\Gamma_{\Delta} are considered. The density of states derived from the model has the familiar Dynes' form with a simple replacement of Γ\Gamma by γ+\gamma_+ = (Γ\Gamma + ΓΔ\Gamma_{\Delta})/2. The γ+\gamma_+ parameter obtained from fitting the experimental spectra shows a roughly linear temperature dependence, which puts a strong constraint on the relation between Γ\Gamma and ΓΔ\Gamma_{\Delta}. We discuss and compare the Fermi arc behavior in the pseudogap phase from the tunneling and angle-resolved photoemission spectroscopy experiments. Our results indicate an excellent agreement between the two experiments, which is in favor of the precursor pairing view of the pseudogap.Comment: 7 pages, 6 figure

    The littlest Higgs model and Higgs boson associated production with top quark pair at high energy linear e+ee^{+}e^{-} collider

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    In the parameter space allowed by the electroweak precision measurement data, we consider the contributions of the new particles predicted by the littlest Higgs(LHLH) model to the Higgs boson associated production with top quark pair in the future high energy linear e+ee^{+}e^{-} collider(ILCILC). We find that the contributions mainly come from the new gauge bosons ZHZ_{H} and BHB_{H}. For reasonable values of the free parameters, the absolute value of the relative correction parameter δσ/σSM\delta\sigma/\sigma^{SM} can be significanly large, which might be observed in the future ILCILC experiment with S=800GeV\sqrt{S}=800GeV.Comment: latex files, 13 pages, 3 figure

    Fermion Condensation Quantum Phase Transition versus Conventional Quantum Phase Transitions

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    The main features of fermion condensation quantum phase transition (FCQPT), which are distinctive in several aspects from that of conventional quantum phase transition (CQPT), are considered. We show that in contrast to CQPT, whose physics in quantum critical region is dominated by thermal and quantum fluctuations and characterized by the absence of quasiparticles, the physics of a Fermi system near FCQPT or undergone FCQPT is controlled by the system of quasiparticles resembling the Landau quasiparticles. Contrary to the Landau quasiparticles, the effective mass of these quasiparticles strongly depends on the temperature, magnetic fields, density, etc. This system of quasiparticles having general properties determines the universal behavior of the Fermi system in question. As a result, the universal behavior persists up to relatively high temperatures comparatively to the case when such a behavior is determined by CQPT. We analyze striking recent measurements of specific heat, charge and heat transport used to study the nature of magnetic field-induced QCP in heavy-fermion metal CeCoIn5_5 and show that the observed facts are in good agreement with our scenario based on FCQPT and certainly seem to rule out the critical fluctuations related with CQPT. Our general consideration suggests that FCQPT and the emergence of novel quasiparticles near and behind FCQPT and resembling the Landau quasiparticles are distinctive features intrinsic to strongly correlated substances.Comment: 10 pages, Revtex, new references and facts are adde

    Harmonic maps from degenerating Riemann surfaces

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    We study harmonic maps from degenerating Riemann surfaces with uniformly bounded energy and show the so-called generalized energy identity. We find conditions that are both necessary and sufficient for the compactness in W1,2W^{1,2} and C0C^{0} modulo bubbles of sequences of such maps.Comment: 27 page

    Analysis of the vertexes ΞQΞQV\Xi_Q^*\Xi'_Q V, ΣQΣQV\Sigma_Q^*\Sigma_Q V and radiative decays ΞQΞQγ\Xi_Q^*\to \Xi'_Q \gamma, ΣQΣQγ\Sigma_Q^*\to \Sigma_Q \gamma

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    In this article, we study the vertexes ΞQΞQV\Xi_Q^*\Xi'_Q V and ΣQΣQV\Sigma_Q^* \Sigma_Q V with the light-cone QCD sum rules, then assume the vector meson dominance of the intermediate ϕ(1020)\phi(1020), ρ(770)\rho(770) and ω(782)\omega(782), and calculate the radiative decays ΞQΞQγ\Xi_Q^*\to \Xi'_Q \gamma and ΣQΣQγ\Sigma_Q^*\to \Sigma_Q \gamma.Comment: 28 pages, 4 tables, revised versio
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