21,078 research outputs found

    CP violating effects in the decay Z -> mu^+mu^-gamma induced by ZZgamma and Zgammagamma couplings

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    We analyze possible CP-violating effects induced in the ZZ decay with hard photon radiation by γZZ\gamma ZZ and γγZ\gamma\gamma Z anomalous vertices. We estimate the sensibility of future linear collider experiments on these couplings coming from CP-odd asymmetries associated to angular correlations of the three particle final state in e+e−→Z→μ+μ−γe^+e^- \to Z \to \mu^+\mu^-\gamma. We find that a linear collider with an integrated luminosity of 500 fb−1fb^{-1} and s=0.05\sqrt{s} = 0.05 TeV can place the bound ∣h1γ,Z∣<0.92|h_1^{\gamma,Z}| < 0.92 at the 90% confidence level for these couplings.Comment: Added references, 2 graphics 5 pages, LaTeX; typos added, 4 graphics remove

    Semiclassical ordering in the large-N pyrochlore antiferromagnet

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    We study the semiclassical limit of the Sp(N)Sp(N) generalization of the pyrochlore lattice Heisenberg antiferromagnet by expanding about the N→∞N \to \infty saddlepoint in powers of a generalized inverse spin. To leading order, we write down an effective Hamiltonian as a series in loops on the lattice. Using this as a formula for calculating the energy of any classical ground state, we perform Monte-Carlo simulations and find a unique collinear ground state. This state is not a ground state of linear spin-wave theory, and can therefore not be a physical (N=1) semiclassical ground state.Comment: 4 pages, 4 eps figures; published versio

    Non-Abelian black holes in string theory

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    We study a family of 5-dimensional non-Abelian black holes that can be obtained by adding an instanton field to the well-known D1D5W Abelian black holes. Naively, the non-Abelian fields seem to contribute to the black-hole entropy but not to the mass due to their rapid fall-off at spatial infinity. By uplifting the 5-dimensional supergravity solution to 10-dimensional Heterotic Supergravity first and then dualizing it into a Type-I Supergravity solution, we show that the non-Abelian fields are associated to D5-branes dissolved into the D9-branes (dual to the Heterotic "gauge 5-branes") and that their associated RR charge does not, in fact, contribute to the entropy, which only depends on the number16 pages of D-strings and D5 branes and the momentum along the D-strings, as in the Abelian case. These "dissolved" or "gauge" D5-branes do contribute to the mass in the expected form. The correct interpretation of the 5-dimensional charges in terms of the string-theory objects solves the non-Abelian hair puzzle, allowing for the microscopic accounting of the entropy. We discuss the validity of the solution when alpha prime corrections are taken into account.Comment: Latex 2e file, 21 pages. A full appendix on alpha prime corrections and the corresponding discussions have been added. The conclusions have suffered minor changes. Version accepted in JHE

    Gas and dust from solar metallicity AGB stars

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    We study the asymptotic giant branch (AGB) evolution of stars with masses between 1 M⊙−8.5 M⊙1~M_{\odot} - 8.5~M_{\odot}. We focus on stars with a solar chemical composition, which allows us to interpret evolved stars in the Galaxy. We present a detailed comparison with models of the same chemistry, calculated with a different evolution code and based on a different set of physical assumptions. We find that stars of mass ≥3.5 M⊙\ge 3.5~M_{\odot} experience hot bottom burning at the base of the envelope. They have AGB lifetimes shorter than ∼3×105\sim 3\times 10^5 yr and eject into their surroundings gas contaminated by proton-capture nucleosynthesis, at an extent sensitive to the treatment of convection. Low mass stars with 1.5 M⊙≤M≤3 M⊙1.5~M_{\odot} \le M \le 3~M_{\odot} become carbon stars. During the final phases the C/O ratio grows to ∼3\sim 3. We find a remarkable agreement between the two codes for the low-mass models and conclude that predictions for the physical and chemical properties of these stars, and the AGB lifetime, are not that sensitive to the modelling of the AGB phase. The dust produced is also dependent on the mass: low-mass stars produce mainly solid carbon and silicon carbide dust, whereas higher mass stars produce silicates and alumina dust. Possible future observations potentially able to add more robustness to the present results are also discussed.Comment: 27 pages, 24 figures; accepted for publication in MNRA
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