38 research outputs found

    Superconductivity by long-range color magnetic interaction in high-density quark matter

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    We argue that in quark matter at high densities, the color magnetic field remains unscreened and leads to the phenomenon of color superconductivity. Using the renormalization group near the Fermi surface, we find that the long-range nature of the magnetic interaction changes the asymptotic behavior of the gap Δ\Delta at large chemical potential ÎŒ\mu qualitatively. We find Δ∌Όg−5exp⁥(−3π221g)\Delta\sim\mu g^{-5}\exp(-{3\pi^2\over\sqrt{2}}{1\over g}), where gg is the small gauge coupling. We discuss the possibility of breaking rotational symmetry by the formation of a condensate with nonzero angular momentum, as well as interesting parallels to some condensed matter systems with long-range forces.Comment: 14 pages, REVTEX, uses eps

    The Crystallography of Color Superconductivity

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    We develop the Ginzburg-Landau approach to comparing different possible crystal structures for the crystalline color superconducting phase of QCD, the QCD incarnation of the Larkin-Ovchinnikov-Fulde-Ferrell phase. In this phase, quarks of different flavor with differing Fermi momenta form Cooper pairs with nonzero total momentum, yielding a condensate that varies in space like a sum of plane waves. We work at zero temperature, as is relevant for compact star physics. The Ginzburg-Landau approach predicts a strong first-order phase transition (as a function of the chemical potential difference between quarks) and for this reason is not under quantitative control. Nevertheless, by organizing the comparison between different possible arrangements of plane waves (i.e. different crystal structures) it provides considerable qualitative insight into what makes a crystal structure favorable. Together, the qualitative insights and the quantitative, but not controlled, calculations make a compelling case that the favored pairing pattern yields a condensate which is a sum of eight plane waves forming a face-centered cubic structure. They also predict that the phase is quite robust, with gaps comparable in magnitude to the BCS gap that would form if the Fermi momenta were degenerate. These predictions may be tested in ultracold gases made of fermionic atoms. In a QCD context, our results lay the foundation for a calculation of vortex pinning in a crystalline color superconductor, and thus for the analysis of pulsar glitches that may originate within the core of a compact star.Comment: 41 pages, 13 figures, 1 tabl

    Infection by the castrating parasitic nematode <i>Sphaerularia bombi </i>changes gene expression in <i>Bombus terrestris </i>bumblebee queens

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    Parasitism can result in dramatic changes in host phenotype, which are themselves underpinned by genes and their expression. Understanding how hosts respond at the molecular level to parasites can therefore reveal the molecular architecture of an altered host phenotype. The entomoparasitic nematode Sphaerularia bombi is a parasite of bumblebee (Bombus) hosts where it induces complex behavioural changes and host castration. To examine this interaction at the molecular level, we performed genome-wide transcriptional profiling using RNA-Seq of S. bombi-infected Bombus terrestris queens at two critical time-points: during and just after overwintering diapause. We found that infection by S. bombi affects the transcription of genes underlying host biological processes associated with energy usage, translation, and circadian rhythm. We also found that the parasite affects the expression of immune genes, including members of the Toll signaling pathway providing evidence for a novel interaction between the parasite and the host immune response. Taken together, our results identify host biological processes and genes affected by an entomoparasitic nematode providing the first steps towards a molecular understanding of this ecologically important host-parasite interaction

    Comments on the Quark Content of the Scalar Meson f0(1370)f_0(1370)

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    Based on the measurements of (Ds+,D+)→f0(1370)π+(D_s^+,D^+)\to f_0(1370)\pi^+ we determine, in a model independent way, the allowed ssˉs\bar s content in the scalar meson f0(1370)f_0(1370). We find that, on the one hand, if this isoscalar resonance is a pure nnˉn\bar n state [ nnˉ≡(uuˉ+ddˉ)/2]n\bar n\equiv(u\bar u+d\bar d)/\sqrt{2} ], a very large WW-annihilation term will be needed to accommodate Ds+→f0(1370)π+D_s^+\to f_0(1370)\pi^+. On the other hand, the ssˉs\bar s component of f0(1370)f_0(1370) should be small enough to avoid excessive Ds+→f0(1370)π+D_s^+\to f_0(1370)\pi^+ induced from the external WW-emission. Measurement of f0(1370)f_0(1370) production in the decay Ds+→K+K−π+D_s^+\to K^+K^-\pi^+ will be useful to test the above picture. For the decay D0→f0(1370)Kˉ0D^0\to f_0(1370)\bar K^0 which is kinematically barely or even not allowed, depending on the mass of f0(1370)f_0(1370), we find that the finite width effect of f0(1370)f_0(1370) plays a crucial role on the resonant three-body decay D0→f0(1370)Kˉ0→π+π−Kˉ0D^0\to f_0(1370)\bar K^0\to\pi^+\pi^-\bar K^0.Comment: 12 pages, 2 figure

    Scalar Particles in Lattice QCD

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    We report a project to study scalar particles by lattice QCD simulations. After a brief introduction of the current situation of lattice study of the sigma meson, we describe our numerical simulations of scalar mesons, σ\sigma and Îș\kappa. We observe a low sigma mass, mπ<mσ≀mρm_\pi<m_\sigma\le m_\rho, for which the disconnected diagram plays an important role. For the kappa meson, we obtain higher mass than the experimental value, i.e., mÎș∌2mK∗m_\kappa\sim 2m_{K^*}.Comment: 4 figures, to be published in Proceedings of `International Symposium on Hadron Spectroscopy, Chiral Symmetry and Relativistic Description of Bound Systems' (in a series of KEK proceedings

    Low Energy Theory for 2 flavors at High Density QCD

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    We construct the effective Lagrangian describing the low energy excitations for Quantum Chromodynamics with two flavors at high density. The non-linear realization framework is employed to properly construct the low energy effective theory. The light degrees of freedom, as required by 't Hooft anomaly conditions, contain massless fermions which we properly include in the effective Lagrangian. We also provide a discussion of the linearly realized Lagrangian.Comment: 17 pages, RevTeX format, references added. To appear in Phys. Rev.

    Magnetic catalysis and anisotropic confinement in QCD

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    The expressions for dynamical masses of quarks in the chiral limit in QCD in a strong magnetic field are obtained. A low energy effective action for the corresponding Nambu-Goldstone bosons is derived and the values of their decay constants as well as the velocities are calculated. The existence of a threshold value of the number of colors NcthrN^{thr}_c, dividing the theories with essentially different dynamics, is established. For the number of colors Ncâ‰ȘNcthrN_c \ll N^{thr}_c, an anisotropic dynamics of confinement with the confinement scale much less than ΛQCD\Lambda_{QCD} and a rich spectrum of light glueballs is realized. For NcN_c of order NcthrN^{thr}_c or larger, a conventional confinement dynamics takes place. It is found that the threshold value NcthrN^{thr}_c grows rapidly with the magnetic field [Ncthr≳100N^{thr}_c \gtrsim 100 for ∣eB∣≳(1GeV)2|eB| \gtrsim (1{GeV})^2]. In contrast to QCD with a nonzero baryon density, there are no principal obstacles for checking these results and predictions in lattice computer simulations.Comment: 10 pages, 1 figure. REVTeX. Minor correction. To appear in Phys. Rev.

    Emergence of Skyrme crystal in Gross-Neveu and 't Hooft models at finite density

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    We study two-dimensional, large NN field theoretic models (Gross-Neveu model, 't Hooft model) at finite baryon density near the chiral limit. The same mechanism which leads to massless baryons in these models induces a breakdown of translational invariance at any finite density. In the chiral limit baryonic matter is characterized by a spatially varying chiral angle with a wave number depending only on the density. For small bare quark masses a sine-Gordon kink chain is obtained which may be regarded as simplest realization of the Skyrme crystal for nuclear matter. Characteristic differences between confining and non-confining models are pointed out.Comment: 27 pages, 11 figures, added reference, corrected sig

    Baryon number violation, baryogenesis and defects with extra dimensions

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    In generic models for grand unified theories(GUT), various types of baryon number violating processes are expected when quarks and leptons propagate in the background of GUT strings. On the other hand, in models with large extra dimensions, the baryon number violation in the background of a string is not trivial because it must depend on the mechanism of the proton stabilization. In this paper we argue that cosmic strings in models with extra dimensions can enhance the baryon number violation to a phenomenologically interesting level, if the proton decay is suppressed by the mechanism of localized wavefunctions. We also make some comments on baryogenesis mediated by cosmological defects. We show at least two scenarios will be successful in this direction. One is the scenario of leptogenesis where the required lepton number conversion is mediated by cosmic strings, and the other is the baryogenesis from the decaying cosmological domain wall. Both scenarios are new and have not been discussed in the past.Comment: 20pages, latex2e, comments and references added, to appear in PR
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