6,132 research outputs found

    Symmetry Reduction and Boundary Modes for Fe-Chains on an s-wave Superconductor

    Full text link
    We investigate the superconducting phase diagram and boundary modes for a quasi-1D system formed by three Fe-Chains on an s-wave superconductor, motivated by the recent Princeton experiment. The l⃗⋅s⃗\vec l\cdot\vec s onsite spin-orbit term, inter-chain diagonal hopping couplings, and magnetic disorders in the Fe-chains are shown to be crucial for the superconducting phases, which can be topologically trivial or nontrivial in different parameter regimes. For the topological regime a single Majorana and multiple Andreew bound modes are obtained in the ends of the chain, while for the trivial phase only low-energy Andreev bound states survive. Nontrivial symmetry reduction mechanism induced by the l⃗⋅s⃗\vec l\cdot\vec s term, diagonal hopping couplings, and magnetic disorder is uncovered to interpret the present results. Our study also implies that the zero-bias peak observed in the recent experiment may or may not reflect the Majorana zero modes in the end of the Fe-chains.Comment: 5 pages, 4 figures; some minor errors are correcte

    Reducing the Tension Between the BICEP2 and the Planck Measurements: A Complete Exploration of the Parameter Space

    Get PDF
    A large inflationary tensor-to-scalar ratio r0.002=0.20βˆ’0.05+0.07r_\mathrm{0.002} = 0.20^{+0.07}_{-0.05} is reported by the BICEP2 team based on their B-mode polarization detection, which is outside of the 95%95\% confidence level of the Planck best fit model. We explore several possible ways to reduce the tension between the two by considering a model in which Ξ±s\alpha_\mathrm{s}, ntn_\mathrm{t}, nsn_\mathrm{s} and the neutrino parameters NeffN_\mathrm{eff} and Ξ£mΞ½\Sigma m_\mathrm{\nu} are set as free parameters. Using the Markov Chain Monte Carlo (MCMC) technique to survey the complete parameter space with and without the BICEP2 data, we find that the resulting constraints on r0.002r_\mathrm{0.002} are consistent with each other and the apparent tension seems to be relaxed. Further detailed investigations on those fittings suggest that NeffN_\mathrm{eff} probably plays the most important role in reducing the tension. We also find that the results obtained from fitting without adopting the consistency relation do not deviate much from the consistency relation. With available Planck, WMAP, BICEP2 and BAO datasets all together, we obtain r0.002=0.14βˆ’0.11+0.05r_{0.002} = 0.14_{-0.11}^{+0.05}, nt=0.35βˆ’0.47+0.28n_\mathrm{t} = 0.35_{-0.47}^{+0.28}, ns=0.98βˆ’0.02+0.02n_\mathrm{s}=0.98_{-0.02}^{+0.02}, and Ξ±s=βˆ’0.0086βˆ’0.0189+0.0148\alpha_\mathrm{s}=-0.0086_{-0.0189}^{+0.0148}; if the consistency relation is adopted, we get r0.002=0.22βˆ’0.06+0.05r_{0.002} = 0.22_{-0.06}^{+0.05}.Comment: 8 pages, 4 figures, submitted to PL
    • …
    corecore