1,054 research outputs found

    Possible Pairing Symmetry of Three-dimensional Superconductor UPt3_3 -- Analysis Based on a Microscopic Calculation --

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    Stimulated by the anomalous superconducting properties of UPt3_3, we investigate the pairing symmetry and the transition temperature in the two-dimensional(2D) and three-dimensional(3D) hexagonal Hubbard model. We solve the Eliashberg equation using the third order perturbation theory with respect to the on-site repulsion UU. As results of the 2D calculation, we obtain distinct two types of stable spin-triplet pairing states. One is the ff-wave(B1_1) pairing around n=1.2n = 1.2 and in a small UU region, which is caused by the ferromagnetic fluctuation. Then, the other is the pxp_x(or pyp_y)-wave(E1_1) pairing in large UU region far from the half-filling (n=1n = 1) which is caused by the vertex corrections only. However, we find that the former ff-wave pairing is destroyed by introduced 3D dispersion. This is because the 3D dispersion breaks the favorable structures for the ff-wave pairing such as the van Hove singularities and the small pocket structures. Thus, we conclude that the ferromagnetic fluctuation mediated spin-triplet state can not explain the superconductivity of UPt3_3. We also study the case of the pairing symmetry with a polar gap. This pzp_z-wave(A1_1) is stabilized by the large hopping integral along c-axis tzt_z. It is nearly degenerate with the suppressed pxp_x(or pyp_y)-wave(E1_1) in the best fitting parameter region to UPt3_3 (1.3≤tz≤1.51.3 \le t_z \le 1.5). These two p-wave pairing states exist in the region far from the half-filling, in which the vertex correction terms play crucial roles like the case in Sr2_2RuO4_4.Comment: 15 pages, 12 figure

    Antiferromagnetism and Superconductivity in UPt_3

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    The short ranged antiferromagnetism recently seen in UPt_3 is proved incompatible with two dimensional (2D) order parameter models that take the antiferromagnetism as a symmetry breaking field. To adjust to the local moment direction, the order parameter twists over very long length scales as per the Imry-Ma argument. A variational solution to the Ginzburg-Landau equations is used to study the nature of the short ranged order. Although there are still two transitions, the lower one is of first order -- in contradiction to experiments. It is shown that the latent heat predicted by the 2D models at the lower transition is too large not to have been seen. A simple periodic model is numerically studied to show that the lower transition can not be a crossover either.Comment: To appear in Journal of Physics: Condensed Matter. 9 pages, 2 figure

    A single chain analysis of doped quasi one dimensional spin 1 compounds: paramagnetic versus spin 1/2 doping

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    We present a numerical study of single chain models of doped spin 1 compounds. We use low energy effective one-dimensional models for both the cases of paramagnetic and spin-1/2 doping. In the case of paramagnetic doping, the effective model is equivalent to the bond disordered spin-1/2 chain model recently analyzed by means of real space renormalization group by Hyman and Yang. By means of exact diagonalizations in the XX limit, we confirm the stability of the Haldane phase for weak disorder. Above a critical amount of disorder, the effective model flows to the so called random singlet fixed point. In the case of spin-1/2 doping, we argue that the Haldane phase should be destabilized even for weak disorder. This picture is not in contradiction with existing experimental data. We also discuss the possible occurrence of (unobserved) antiferromagnetically ordered phases.Comment: 13 pages, 7 included figure

    Identification of Non-unitary triplet pairing in a heavy Fermion superconductor UPt_3

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    A NMR experiment recently done by Tou et al. on a heavy Fermion superconductor UPt3_3 is interpreted in terms of a non-unitary spin-triplet pairing state which we have been advocating. The proposed state successfully explains various aspects of the seemingly complicated Knight shift behaviors probed for major orientations, including a remarkable d-vector rotation under weak fields. This entitles UPt3_3 as the first example that a charged many body system forms a spin-triplet odd-par ity pairing at low temperatures and demonstrates unambiguously that the putative spin-orbit coupling in UPt3_3 is weak.Comment: 4 pages, 2 eps figures, to be published in J. Phys. Soc. Jpn. 67 (1998) No.

    Quasiparticle localization in superconductors with spin-orbit scattering

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    We develop a theory of quasiparticle localization in superconductors in situations without spin rotation invariance. We discuss the existence, and properties of superconducting phases with localized/delocalized quasiparticle excitations in such systems in various dimensionalities. Implications for a variety of experimental systems, and to the properties of random Ising models in two dimensions, are briefly discussed.Comment: 10 page

    Transport and the Order Parameter of Superconducting UPt3

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    We calculate the ultrasonic absorption and the thermal conductivity in the superconducting state of UPt3_{3} as functions of temperature and direction of propagation and polarization. Two leading candidates for the superconducting order parameter are considered: the E1gE_{1g} and E2uE_{2u} representations. Both can fit the data except for the ultrasonic absorption in the AA phase. To do that, it is necessary to suppose that the system has only a single domain, and that must be chosen as the most favorable one. However, the E2uE_{2u} theory requires fine-tuning of parameters to fit the low temperature thermal conductivity. Thus, transport data favor the E1gE_{1g} theory. Measurements of the thermal conductivity as a function of pressure at low temperature could help to further distinguish the two theories.Comment: 7 pages, 4 figure
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