14,469 research outputs found

    String completion of an SU(3)cSU(3)LU(1)X\mathrm{SU(3)_c \otimes SU(3)_L \otimes U(1)_X} electroweak model

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    The extended electroweak SU(3)cSU(3)LU(1)X\mathrm{SU(3)_c \otimes SU(3)_L \otimes U(1)_X} symmetry framework "explaining" the number of fermion families is revisited. While 331331-based schemes can not easily be unified within the conventional field theory sense, we show how to do it within an approach based on D-branes and (un)oriented open strings, on Calabi-Yau singularities. We show how the theory can be UV-completed in a quiver setup, free of gauge and string anomalies. Lepton and baryon numbers are perturbatively conserved, so neutrinos are Dirac-type, and their lightness results from a novel TeV scale seesaw mechanism. Dynamical violation of baryon number by exotic instantons could induce neutron-antineutron oscillations, with proton decay and other dangerous R-parity violating processes strictly forbidden.Comment: 12 pages, 2 figures, published versio

    Irreversibility line and low-field grain-boundary pinning in electron-doped superconducting thin films

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    AC magnetic susceptibilities of electron-doped Pr_{1.85}Ce_{0.15}CuO_4 (PCCO) and Sm_{1.85}Ce_{0.15}CuO_4 (SCCO) granular thin films have been measured as a function of temperature and magnetic-field strength. Depending on the level of homogeneity of our films, two different types of the irreversibility line (IL) defined as the intergrain-loss peak temperature in the imaginary part of susceptibility have been found. The obtained results are described via the critical-state model taking into account the low-field grain-boundary pinning. The extracted pinning-force densities in more granular SCCO films turn out to be four times larger than their counterparts in less granular PCCO films

    Coalescence Rate of Supermassive Black Hole Binaries Derived from Cosmological Simulations: Detection Rates for LISA and ET

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    The coalescence history of massive black holes has been derived from cosmological simulations, in which the evolution of those objects and that of the host galaxies are followed in a consistent way. The present study indicates that supermassive black holes having masses greater than 109M\sim 10^{9} M_{\odot} underwent up to 500 merger events along their history. The derived coalescence rate per comoving volume and per mass interval permitted to obtain an estimate of the expected detection rate distribution of gravitational wave signals ("ring-down") along frequencies accessible by the planned interferometers either in space (LISA) or in the ground (Einstein). For LISA, in its original configuration, a total detection rate of about 15yr115 yr^{-1} is predicted for events having a signal-to-noise ratio equal to 10, expected to occur mainly in the frequency range 49mHz4-9 mHz. For the Einstein gravitational wave telescope, one event each 14 months down to one event each 4 years is expected with a signal-to-noise ratio of 5, occurring mainly in the frequency interval 1020Hz10-20 Hz. The detection of these gravitational signals and their distribution in frequency would be in the future an important tool able to discriminate among different scenarios explaining the origin of supermassive black holes.Comment: 18 pages, 7 figures, to appear in the IJMP

    Possible manifestation of spin fluctuations in the temperature behavior of resistivity in Sm_{1.85}Ce_{0.15}CuO_4 thin films

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    A pronounced step-like (kink) behavior in the temperature dependence of resistivity ρ(T)\rho (T) is observed in the optimally-doped Sm1.85Ce0.15CuO4Sm_{1.85}Ce_{0.15}CuO_4 thin films around Tsf=87KT_{sf}=87K and attributed to manifestation of strong spin fluctuations induced by Sm3+Sm^{3+} moments with the energy ωsf=kBTsf7meV\hbar \omega_{sf}=k_BT_{sf}\simeq 7meV. In addition to fluctuation induced contribution ρsf(T)\rho_{sf}(T) due to thermal broadening effects (of the width ωsf\omega_{sf}), the experimental data are found to be well fitted accounting for residual (zero-temperature) ρres\rho_{res}, electron-phonon ρeph(T)=AT\rho _{e-ph}(T)=AT and electron-electron ρee(T)=BT2\rho_{e-e}(T)=BT^2 contributions. The best fits produced ωp=2.1meV\omega_p=2.1meV, τ01=9.5×1014s1\tau_0^{-1}=9.5\times 10^{-14}s^{-1}, λ=1.2\lambda =1.2, and EF=0.2eVE_F=0.2eV for estimates of the plasmon frequency, the impurity scattering rate, electron-phonon coupling constant, and the Fermi energy, respectively.Comment: 6 pages (REVTEX4), 2 EPS figures; accepted for publication in JETP Letter
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