134,760 research outputs found

    The Carnegie-Irvine Galaxy Survey. V. Statistical study of bars and buckled bars

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    Simulations have shown that bars are subject to a vertical buckling instability that transforms thin bars into boxy or peanut-shaped structures, but the physical conditions necessary for buckling to occur are not fully understood. We use the large sample of local disk galaxies in the Carnegie-Irvine Galaxy Survey to examine the incidence of bars and buckled bars across the Hubble sequence. Depending on the disk inclination angle (ii), a buckled bar reveals itself as either a boxy/peanut-shaped bulge (at high ii) or as a barlens structure (at low ii). We visually identify bars, boxy/peanut-shaped bulges, and barlenses, and examine the dependence of bar and buckled bar fractions on host galaxy properties, including Hubble type, stellar mass, color, and gas mass fraction. We find that the barred and unbarred disks show similar distributions in these physical parameters. The bar fraction is higher (70\%--80\%) in late-type disks with low stellar mass (Māˆ—<1010.5ā€‰MāŠ™M_{*} < 10^{10.5}\, M_{\odot}) and high gas mass ratio. In contrast, the buckled bar fraction increases to 80\% toward massive and early-type disks (Māˆ—>1010.5ā€‰MāŠ™M_{*} > 10^{10.5}\, M_{\odot}), and decreases with higher gas mass ratio. These results suggest that bars are more difficult to grow in massive disks that are dynamically hotter than low-mass disks. However, once a bar forms, it can easily buckle in the massive disks, where a deeper potential can sustain the vertical resonant orbits. We also find a probable buckling bar candidate (ESO 506āˆ’-G004) that could provide further clues to understand the timescale of the buckling process.Comment: 9 pages, 7 figures, 2 tables. Accepted for publication in The Astrophysical Journa

    On several families of elliptic curves with arbitrary large Selmer groups

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    In this paper, we calculate the Ļ•(Ļ•^)āˆ’ \phi (\hat{\phi})-Selmer groups S^{(\phi)} (E / \Q) and S^{(\hat{\varphi})} (E^{\prime} / \Q) of elliptic curves y2=x(x+ĻµpD)(x+ĻµqD) y^{2} = x (x + \epsilon p D) (x + \epsilon q D) via descent theory (see [S, Chapter X]), in particular, we obtain that the Selmer groups of several families of such elliptic curves can be arbitrary large.Comment: 22 page

    Magnetic field splitting of the spin-resonance in CeCoIn5

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    Neutron scattering in strong magnetic fields is used to show the spin-resonance in superconducting CeCoIn5 (Tc=2.3 K) is a doublet. The underdamped resonance (\hbar \Gamma=0.069 \pm 0.019 meV) Zeeman splits into two modes at E_{\pm}=\hbar \Omega_{0}\pm g\mu_{B} \mu_{0}H with g=0.96 \pm 0.05. A linear extrapolation of the lower peak reaches zero energy at 11.2 \pm 0.5 T, near the critical field for the incommensurate "Q-phase" indicating that the Q-phase is a bose condensate of spin excitons.Comment: 5 pages, 4 figure
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