5,032 research outputs found

    Zero Temperature Limit of Holographic Superconductors

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    We consider holographic superconductors whose bulk description consists of gravity minimally coupled to a Maxwell field and charged scalar field with general potential. We give an analytic argument that there is no "hard gap": the real part of the conductivity at low frequency remains nonzero (although typically exponentially small) even at zero temperature. We also numerically construct the gravitational dual of the ground state of some holographic superconductors. Depending on the charge and dimension of the condensate, the infrared theory can have emergent conformal or just Poincare symmetry. In all cases studied, the area of the horizon of the dual black hole goes to zero in the extremal limit, consistent with a nondegenerate ground state.Comment: 27 pages, 8 figure

    Power corrections to the π0γ\pi^0\gamma transition form factor and pion distribution amplitudes

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    Employing the standard hard-scattering approach and the running coupling method we calculate a class of power-suppressed corrections 1/Q2n,n=1,2,3,...\sim 1/Q^{2n},n=1,2,3,... to the electromagnetic π0γ\pi^0\gamma transition form factor (FF) Q2Fπγ(Q2)Q^2F_{\pi\gamma}(Q^2) arising from the end-point x0,1x \to 0,1 integration regions. In the investigations we use a hard-scattering amplitude of the subprocess γ+γq+qˉ\gamma+\gamma^{*} \to q +\bar{q}, symmetrized under exchange μR2μˉR2\mu_R^2 \leftrightarrow \bar{\mu}_R^2 important for exclusive processes containing two external photons. In the computations the pion model distribution amplitudes (DA's) with one and two non-asymptotic terms are employed. The obtained predictions are compared with the CLEO data and constraints on the DA parameters b2(μ02)b_2(\mu_0^2) and b4(μ02)b_4(\mu_0^2) at the normalization point μ02=1GeV2\mu_0^2=1 GeV^2 are extracted. Further restrictions on the pion DA's are deduced from the experimental data on the electromagnetic FF Fπ(Q2)F_{\pi}(Q^2).Comment: 23 pages, 6 figures; the version published in Phys. Rev. D69, 094010 (2004

    Additive N-Step Markov Chains as Prototype Model of Symbolic Stochastic Dynamical Systems with Long-Range Correlations

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    A theory of symbolic dynamic systems with long-range correlations based on the consideration of the binary N-step Markov chains developed earlier in Phys. Rev. Lett. 90, 110601 (2003) is generalized to the biased case (non equal numbers of zeros and unities in the chain). In the model, the conditional probability that the i-th symbol in the chain equals zero (or unity) is a linear function of the number of unities (zeros) among the preceding N symbols. The correlation and distribution functions as well as the variance of number of symbols in the words of arbitrary length L are obtained analytically and verified by numerical simulations. A self-similarity of the studied stochastic process is revealed and the similarity group transformation of the chain parameters is presented. The diffusion Fokker-Planck equation governing the distribution function of the L-words is explored. If the persistent correlations are not extremely strong, the distribution function is shown to be the Gaussian with the variance being nonlinearly dependent on L. An equation connecting the memory and correlation function of the additive Markov chain is presented. This equation allows reconstructing a memory function using a correlation function of the system. Effectiveness and robustness of the proposed method is demonstrated by simple model examples. Memory functions of concrete coarse-grained literary texts are found and their universal power-law behavior at long distances is revealed.Comment: 19 pages, 8 figure

    Research Progress of Coloring Aluminum Pigments by Corrosion Protection Method

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    AbstractWith the increasing of the aesthetic value of people and pursue of colorful, coloring aluminum pigments will have broad application prospects. Chromatic sliver printing ink is a kind of flake aluminum pigments which has had the surface modification treatment. It has metallic luster of aluminum powder and chromatic colors at the same time. Chromatic aluminum pigments is widely used in automobile, coatings, printing ink, printing and dyeing, etc industries and fields such as art adornment because of its characteristics such as chromatic color, strong corrosion resistance, good insulation, permanent, strong mental luster, low cost and so on. So preparing a new kind of chromatic silver plasma ink is of great significance. The reporting of domestic and international documents of coloring aluminum pigments by corrosion protection methods mainly are adsorptive, sedimentation and coating method

    Cosmic tomography with weak gravitational lensing

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    We explored the Universe using weak gravitational lensing, a phenomenon that occurs when light from distant galaxies is bent by the gravitational fields of closer cosmic objects, much like how a lens distorts light. Studying these distortions gives us insights into massive objects, such as galaxy clusters, and the large-scale structure of the Universe. However, analysing these weak lensing effects, though powerful, is challenging. Accurately detecting and interpreting these minute distortions require careful management of uncertainties, both from observational techniques and the models we employ. In our study, we rigorously controlled these uncertainties. By enhancing our analysis methods, we provided more accurate constraints on key cosmological parameters. Furthermore, we studied lensing effects around galaxy groups, shedding light on the relationship between the enigmatic dark matter – a difficult-to-detect but predominant component of the Universe – and the galaxies we observe. In conclusion, our research advanced the weak lensing analysis and broadened our understanding of the Universe.Galaxie

    Aspects of the Screening Length and Drag Force in Two Alternative Gravity Duals of the Quark-gluon Plasma

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    We compute the screening length of mesons with different angular momentum JJ from two gravity dual theories. Both the asymptotically AdS5AdS_{5} and Sakai-Sugimoto metrics are considered in the calculations. Using the dual description of the quark as a classical string ending on the probe brane, we obtain the interacting potential between the heavy quark and antiquark after rotating the background metric. The result shows that the screening length of mesons with different JJ is well fit to aJ/Ta_{J}/T. The constant aJa_{J} is determined for J=0,1,2J=0,1,2 by taking advantage of numerical techniques. Finally, we calculate the drag force and relaxation times from the Sakai-Sugimoto metric and compare with the ones obtained in the AdS5AdS_{5}. The application of our result to charmonium and bottomonium at RHIC and LHC is briefly discussed.Comment: 18 pages, 6 figures, 2 tables, version to appear in JHEP, acknowledgment adde

    Appearance and disappearance of superconductivity in SmFe1-xNixAsO (x = 0.0 to 1.0)

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    Bulk polycrystalline Ni-substituted SmFe1-xNixAsO (x = 0.0 to 1.0) samples are synthesized by solid state reaction route in an evacuated sealed quartz tube. The cell volume decreases with increase of Ni content in SmFe1-xNixAsO, thus indicating successful substitution of smaller ion Ni at Fe site. The resistivity measurements showed that the spin-density-wave (SDW) transition is suppressed drastically with Ni doping and subsequently superconductivity is achieved in a narrow range of x from 0.04 to 0.10 with maximum Tc of 9K at x = 0.06. For higher content of Ni (x > 0.10), the system becomes metallic and superconductivity is not observed down to 2K. The magneto-transport [R(T)H] measurements exhibited the upper critical field [Hc2(0)] of up to 300kOe. The flux flow activation energy (U/kB) is estimated ~98.37K for 0.1T field. Magnetic susceptibility measurements also confirms bulk superconductivity for x = 0.04, 0.06 and 0.08 samples. The lower critical field (Hc1) is around 100Oe at 2K for x = 0.06 sample. Heat capacity CP(T) measurements exhibited a hump like transition pertaining to SDW in Fe planes at around 150K and an AFM ordering of Sm spins below temperature of 5.4K for ordered Sm spins [TN(Sm)]. Though, the SDW hump for Fe spins disappears for Ni doped samples, the TN (Sm) remains unaltered but with a reduced transition height, i.e., decreased entropy. In conclusion, complete phase diagram of SmFe1-xNixAsO (x = 0.0 to 1.0) is studied in terms of its structural, electrical, magnetic and thermal properties.Comment: 18 pages text + Figures; comments suggestions welcome ([email protected]

    Radiative Tau Lepton Pair Production as a Probe of Anomalous Electromagnetic Couplings of the Tau

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    We calculate the squared matrix element for the process e+ e- --> tau+ tau- gamma allowing for anomalous magnetic and electric dipole moments at the tau tau gamma vertex. No interferences are neglected and no approximations of light fermion masses are made. We show that anomalous moments affect not only the cross section, but also the shape of the photon energy and angular distributions. We also demonstrate that in the case of the anomalous magnetic dipole moment, the contribution from interference involving Standard Model and anomalous amplitudes is significant compared to the contribution from anomalous amplitudes alone. A program to perform the calculation is available and it may be employed as a Monte Carlo generator.Comment: 14 pages, 8 figures submitted to Nuclear Physics

    Improved superconducting properties of MgB2

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    We present electrical transport, magnetization, and specific heat measurements on bulk MgB2 samples (T_{c} = 38.5 K) synthesized under 200 MPa pressure using a process based on hot isostatic pressing with cooling under pressure. The samples are fully dense and display excellent superconducting properties, including a narrow superconducting transition width (\Delta T_{c} = 0.75 K), a high upper critical field H_{c2} (H_{c2}(0) ~ 155 kOe), and a critical current density J_{c} that is the largest yet measured for bulk samples of MgB2 (J_{c}(0) ~ 1.4 MA/cm^{2}). Specific heat measurements yielded a jump \Delta C at T_{c} of 92 mJ/mol K. These superconducting properties are comparable to those obtained with techniques that are not so well suited to industrial scale fabrication.Comment: 7 text pages, 5 figures, submitted to Physica
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