9,117 research outputs found

    Plasma chemistry and organic synthesis

    Get PDF
    The characteristic features of chemical reactions using low temperature plasmas are described and differentiated from those seen in other reaction systems. A number of examples of applications of plasma chemistry to synthetic reactions are mentioned. The production of amino acids by discharge reactions in hydrocarbon-ammonia-water systems is discussed, and its implications for the origins of life are mentioned

    Reentrant topological transitions in a quantum wire/superconductor system with quasiperiodic lattice modulation

    Get PDF
    We study the condition for a topological superconductor (TS) phase with end Majorana fermions to appear when a quasiperiodic lattice modulation is applied to a one-dimensional quantum wire with strong spin-orbit interaction situated under a magnetic field and in proximity to a superconductor. By density-matrix renormalization group analysis, we find that multiple topological phases with Majorana end modes are realized in finite ranges of the filling factor, showing a sequence of reentrant transitions as the chemical potential is tuned. The locations of these phases reflect the structure of bands in the non-interacting case, which exhibits a distinct self-similar structure. The stability of the TS in the presence of an on-site interaction or a harmonic trap potential is also discussed.Comment: 5 pages, 4 figures, v4: minor corrections; published in Phys. Rev. B Rapid Communicatio

    Density-Matrix Renormalization Group Study of Trapped Imbalanced Fermi Condensates

    Full text link
    The density-matrix renormalization group is employed to investigate a harmonically-trapped imbalanced Fermi condensate based on a one-dimensional attractive Hubbard model. The obtained density profile shows a flattened population difference of spin-up and spin-down components at the center of the trap, and exhibits phase separation between the condensate and unpaired majority atoms for a certain range of the interaction and population imabalance PP. The two-particle density matrix reveals that the sign of the order parameter changes periodically, demonstrating the realization of the Fulde-Ferrell-Larkin-Ovchinnikov phase. The minority spin atoms contribute to the quasi-condensate up to at least P0.8P \simeq 0.8. Possible experimental situations to test our predictions are discussed.Comment: 4 pages, 3 figures; added references; accepted for publication in Phys. Rev. Let

    Poisson Brackets, Strings and Membranes

    Full text link
    We construct Poisson brackets at boundaries of open strings and membranes with constant background fields which are compatible with their boundary conditions. The boundary conditions are treated as primary constraints which give infinitely many secondary constraints. We show explicitly that we need only two (the primary one and one of the secondary ones) constraints to determine Poisson brackets of strings. We apply this to membranes by using canonical transformations.Comment: 9 pages, references and a note are added, title and abstract is changed, the section 3 is improved, the version to appear in EPJ

    Reentrant topological transitions with Majorana end states in 1D superconductors by lattice modulation

    Get PDF
    The possibility to observe and manipulate Majorana fermions as end states of one-dimensional topological superconductors has been actively discussed recently. In a quantum wire with strong spin-orbit coupling placed in proximity to a bulk superconductor, a topological superconductor has been expected to be realized when the band energy is split by the application of a magnetic field. When a periodic lattice modulation is applied multiple topological superconductor phases appear in the phase diagram. Some of them occur for higher filling factors compared to the case without the modulation. We study the effects of phase jumps and argue that the topologically nontrivial state of the whole system is retained even if they are present. We also study the effect of the spatial modulation in the hopping parameter.Comment: 10 pages, 9 figures, submitted to Phys. Rev.

    A minimal model of many body localization

    Full text link
    We present a fully analytical description of a many body localization (MBL) transition in a microscopically defined model. Its Hamiltonian is the sum of one- and two-body operators, where both contributions obey a maximum-entropy principle and have no symmetries except hermiticity (not even particle number conservation). These two criteria paraphrase that our system is a variant of the Sachdev-Ye-Kitaev (SYK) model. We will demonstrate how this simple `zero-dimensional' system displays numerous features seen in more complex realizations of MBL. Specifically, it shows a transition between an ergodic and a localized phase, and non-trivial wave function statistics indicating the presence of `non-ergodic extended states'. We check our analytical description of these phenomena by parameter free comparison to high performance numerics for systems of up to N=15N=15 fermions. In this way, our study becomes a testbed for concepts of high-dimensional quantum localization, previously applied to synthetic systems such as Cayley trees or random regular graphs. We believe that this is the first many body system for which an effective theory is derived and solved from first principles. The hope is that the novel analytical concepts developed in this study may become a stepping stone for the description of MBL in more complex systems.Comment: 21 pages, 8 figures, introduction rewritten, changed titl

    K^*(BG) rings for groups G=G38,...,G41G=G_{38},...,G_{41} of order 32

    Full text link
    B. Schuster \cite{SCH1} proved that the modmod 2 Morava KK-theory K(s)(BG)K(s)^*(BG) is evenly generated for all groups GG of order 32. For the four groups GG with the numbers 38, 39, 40 and 41 in the Hall-Senior list \cite{H}, the ring K(2)(BG)K(2)^*(BG) has been shown to be generated as a K(2)K(2)^*-module by transferred Euler classes. In this paper, we show this for arbitrary ss and compute the ring structure of K(s)(BG)K(s)^*(BG). Namely, we show that K(s)(BG)K(s)^*(BG) is the quotient of a polynomial ring in 6 variables over K(s)(pt)K(s)^*(pt) by an ideal for which we list explicit generators.Comment: 23 page
    corecore