48,127 research outputs found

    Anomalies and Hawking radiation from the Reissner-Nordstr\"om black hole with a global monopole

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    We extend the work by S. Iso, H. Umetsu and F. Wilczek [Phys. Rev. Lett. 96 (2006) 151302] to derive the Hawking flux via gauge and gravitational anomalies of a most general two-dimensional non-extremal black hole space-time with the determinant of its diagonal metric differing from the unity (−g≠1\sqrt{-g} \neq 1) and use it to investigate Hawking radiation from the Reissner-Nordstrom black hole with a global monopole by requiring the cancellation of anomalies at the horizon. It is shown that the compensating energy momentum and gauge fluxes required to cancel gravitational and gauge anomalies at the horizon are precisely equivalent to the (1+1)(1+1)-dimensional thermal fluxes associated with Hawking radiation emanating from the horizon at the Hawking temperature. These fluxes are universally determined by the value of anomalies at the horizon.Comment: 18 pages, 0 figure. 1 footnote and 4 new reference adde

    Multi-boson effects and the normalization of the two-pion correlation function

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    The two-pion correlation function can be defined as a ratio of either the measured momentum distributions or the normalized momentum space probabilities. We show that the first alternative avoids certain ambiguities since then the normalization of the two-pion correlator contains important information on the multiplicity distribution of the event ensemble which is lost in the second alternative. We illustrate this explicitly for specific classes of event ensembles.Comment: 6 pages, three figures,submit to PR

    On some notions of good reduction for endomorphisms of the projective line

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    Let Ί\Phi be an endomorphism of \SR(\bar{\Q}), the projective line over the algebraic closure of \Q, of degree ≄2\geq2 defined over a number field KK. Let vv be a non-archimedean valuation of KK. We say that Ί\Phi has critically good reduction at vv if any pair of distinct ramification points of Ί\Phi do not collide under reduction modulo vv and the same holds for any pair of branch points. We say that Ί\Phi has simple good reduction at vv if the map Ίv\Phi_v, the reduction of Ί\Phi modulo vv, has the same degree of Ί\Phi. We prove that if Ί\Phi has critically good reduction at vv and the reduction map Ίv\Phi_v is separable, then Ί\Phi has simple good reduction at vv.Comment: 15 page

    Evidence for a Kondo destroying quantum critical point in YbRh2Si2

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    The heavy-fermion metal YbRh2_{2}Si2_{2} is a weak antiferromagnet below TN=0.07T_{N} = 0.07 K. Application of a low magnetic field Bc=0.06B_{c} = 0.06 T (⊄c\perp c) is sufficient to continuously suppress the antiferromagnetic (AF) order. Below T≈10T \approx 10 K, the Sommerfeld coefficient of the electronic specific heat Îł(T)\gamma(T) exhibits a logarithmic divergence. At T<0.3T < 0.3 K, Îł(T)∌T−ϔ\gamma(T) \sim T^{-\epsilon} (Ï”:0.3−0.4\epsilon: 0.3 - 0.4), while the electrical resistivity ρ(T)=ρ0+aT\rho(T) = \rho_{0} + aT (ρ0\rho_{0}: residual resistivity). Upon extrapolating finite-TT data of transport and thermodynamic quantities to T=0T = 0, one observes (i) a vanishing of the "Fermi surface crossover" scale T∗(B)T^{*}(B), (ii) an abrupt jump of the initial Hall coefficient RH(B)R_{H}(B) and (iii) a violation of the Wiedemann Franz law at B=BcB = B_{c}, the field-induced quantum critical point (QCP). These observations are interpreted as evidence of a critical destruction of the heavy quasiparticles, i.e., propagating Kondo singlets, at the QCP of this material.Comment: 20 pages, 8 figures, SCES 201

    A Tracker Solution for a Holographic Dark Energy Model

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    We investigate a kind of holographic dark energy model with the future event horizon the IR cutoff and the equation of state -1. In this model, the constraint on the equation of state automatically specifies an interaction between matter and dark energy. With this interaction included, an accelerating expansion is obtained as well as the transition from deceleration to acceleration. It is found that there exists a stable tracker solution for the numerical parameter d>1d>1, and dd smaller than one will not lead to a physical solution. This model provides another possible phenomenological framework to alleviate the cosmological coincidence problem in the context of holographic dark energy. Some properties of the evolution which are relevant to cosmological parameters are also discussed.Comment: 10 pages, 3 figures; accepted for publication in Int.J.Mod.Phys.

    Reconstructing generalized ghost condensate model with dynamical dark energy parametrizations and observational datasets

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    Observations of high-redshift supernovae indicate that the universe is accelerating at the present stage, and we refer to the cause for this cosmic acceleration as ``dark energy''. In particular, the analysis of current data of type Ia supernovae (SNIa), cosmic large-scale structure (LSS), and the cosmic microwave background (CMB) anisotropy implies that, with some possibility, the equation-of-state parameter of dark energy may cross the cosmological-constant boundary (w=−1w=-1) during the recent evolution stage. The model of ``quintom'' has been proposed to describe this w=−1w=-1 crossing behavior for dark energy. As a single-real-scalar-field model of dark energy, the generalized ghost condensate model provides us with a successful mechanism for realizing the quintom-like behavior. In this paper, we reconstruct the generalized ghost condensate model in the light of three forms of parametrization for dynamical dark energy, with the best-fit results of up-to-date observational data.Comment: 8 pages, 3 figures; references added; accepted for publication in Mod. Phys. Lett.

    Break up of heavy fermions at an antiferromagnetic instability

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    We present results of high-resolution, low-temperature measurements of the Hall coefficient, thermopower, and specific heat on stoichiometric YbRh2Si2. They support earlier conclusions of an electronic (Kondo-breakdown) quantum critical point concurring with a field induced antiferromagnetic one. We also discuss the detachment of the two instabilities under chemical pressure. Volume compression/expansion (via substituting Rh by Co/Ir) results in a stabilization/weakening of magnetic order. Moderate Ir substitution leads to a non-Fermi-liquid phase, in which the magnetic moments are neither ordered nor screened by the Kondo effect. The so-derived zero-temperature global phase diagram promises future studies to explore the nature of the Kondo breakdown quantum critical point without any interfering magnetism.Comment: minor changes, accepted for publication in JPS

    Dissipative Effects in the Electronic Transport through DNA Molecular Wires

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    We investigate the influence of a dissipative environment which effectively comprises the effects of counterions and hydration shells, on the transport properties of short \DNA wires. Their electronic structure is captured by a tight-binding model which is embedded in a bath consisting of a collection of harmonic oscillators. Without coupling to the bath a temperature independent gap opens in the electronic spectrum. Upon allowing for electron-bath interaction the gap becomes temperature dependent. It increases with temperature in the weak-coupling limit to the bath degrees of freedom. In the strong-coupling regime a bath-induced {\it pseudo-gap} is formed. As a result, a crossover from tunneling to activated behavior in the low-voltage region of the II-VV characteristics is observed with increasing temperature. The temperature dependence of the transmission near the Fermi energy, t(EF)t(E_{\rm F}), manifests an Arrhenius-like behavior in agreement with recent transport experiments. Moreover, t(EF)t(E_{\rm F}) shows a weak exponential dependence on the wire length, typical of strong incoherent transport. Disorder effects smear the electronic bands, but do not appreciably affect the pseudo-gap formation

    Relativistic precession and spin dynamics of an elliptic Rydberg wave packet

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    Time evolution of wave packets built from the eigenstates of the Dirac equation for a hydrogenic system is considered. We investigate the space and spin motion of wave packets which, in the non-relativistic limit, are stationary states with a probability density distributed uniformly along the classical, elliptical orbit (elliptic WP). We show that the precession of such a WP, due to relativistic corrections to the energy eigenvalues, is strongly correlated with the spin motion. We show also that the motion is universal for all hydrogenic systems with an arbitrary value of the atomic number Z.Comment: Latex2e, uses IOP style files (included), 10 pages, 5 jpg figures, 1 postscript figure. Relation between precession time and radiative liftime added (eq.(12)). Accepted for publication in J. Phys.
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