3,724 research outputs found

    Analytical investigation of magnetic field distributions around superconducting strips on ferromagnetic substrates

    Full text link
    The complex-field approach is developed to derive analytical expressions of the magnetic field distributions around superconducting strips on ferromagnetic substrates (SC/FM strips). We consider the ferromagnetic substrates as ideal soft magnets with an infinite magnetic permeability, neglecting the ferromagnetic hysteresis. On the basis of the critical state model for a superconducting strip, the ac susceptibility χ1+iχ1\chi_1'+i\chi_1'' of a SC/FM strip exposed to a perpendicular ac magnetic field is theoretically investigated, and the results are compared with those for superconducting strips on nonmagnetic substrates (SC/NM strips). The real part χ1\chi_1' for H0/jcds0H_0/j_cd_s\to 0 (where H0H_0 is the amplitude of the ac magnetic field, jcj_c is the critical current density, and dsd_s is the thickness of the superconducting strip) of a SC/FM strip is 3/4 of that of a SC/NM strip. The imaginary part χ1\chi_1'' (or ac loss QQ) for H0/jcds<0.14H_0/j_cd_s<0.14 of a SC/FM strip is larger than that of a SC/NM strip, even when the ferromagnetic hysteresis is neglected, and this enhancement of χ1\chi_1'' (or QQ) is due to the edge effect of the ferromagnetic substrate.Comment: 8 pages, 6 figures, submitted to Phys. Rev.

    Quantum Monte Carlo simulation of S=1/2 Heisenberg model with four spin interaction

    Get PDF
    25th International Conference on Low Temperature Physics (LT25)The spin S = 1/2 Heisenberg model with four-spin interaction on the square lattice is studied by using quantum Monte Carlo method. When the four-spin interaction is dominant, the system has a VBS ground state. In this case, we find a finite-temperature second-order phase transition to the VBS state. The universality class of the transition is investigated. We estimate the critical exponents ν and η from the finite size scaling analysis and find ν = 0.68(1) and η = 0.55(2)
    corecore