2,661 research outputs found

    Low temperature and high pressure Raman and x-ray studies of pyrochlore Tb2_2Ti2_2O7_7 : phonon anomalies and possible phase transition

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    We have carried out temperature and pressure-dependent Raman and x-ray measurements on single crystals of Tb2_2Ti2_2O7_7. We attribute the observed anomalous temperature dependence of phonons to phonon-phonon anharmonic interactions. The quasiharmonic and anharmonic contributions to the temperature-dependent changes in phonon frequencies are estimated quantitatively using mode Gr\"{u}neisen parameters derived from pressure-dependent Raman experiments and bulk modulus from high pressure x-ray measurements. Further, our Raman and x-ray data suggest a subtle structural deformation of the pyrochlore lattice at \sim 9 GPa. We discuss possible implications of our results on the spin-liquid behaviour of Tb2_2Ti2_2O7_7.Comment: 10 figures, 26 pages. Appeared in Physical Review B, vol-79, pp-134112 (2009

    Temperature dependent Raman and x-ray studies of spin-ice pyrochlore Dy2Ti2O7Dy_2Ti_2O_7 and non-magnetic pyrochlore Lu2Ti2O7Lu_2Ti_2O_7

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    We present here temperature-dependent Raman, x-ray diffraction and specific heat studies between room temperature and 12 K on single crystals of spin-ice pyrochlore compound Dy2Ti2O7Dy_2Ti_2O_7 and its non-magnetic analogue Lu2Ti2O7Lu_2Ti_2O_7. Raman data show a "new" band not predicted by factor group analysis of Raman-active modes for the pyrochlore structure in Dy2Ti2O7Dy_2Ti_2O_7, appearing below a temperature of Tc=T_c=110 K with a concomitant contraction of the cubic unit cell volume as determined from the powder x-ray diffraction analysis. Low temperature Raman experiments on O18^{18}-isotope substituted Dy2Ti2O7Dy_2Ti_2O_7 confirm the phonon origin of the "new" mode. These findings, absent in Lu2Ti2O7Lu_2Ti_2O_7, suggest that the room temperature cubic lattice of the pyrochlore Dy2Ti2O7Dy_2Ti_2O_7 undergoes a "subtle" structural transformation near TcT_c. We find anomalous \textit{red-shift} of some of the phonon modes in both the Dy2Ti2O7Dy_2Ti_2O_7 and the Lu2Ti2O7Lu_2Ti_2O_7 as the temperature decreases, which is attributed to strong phonon-phonon anharmonic interactions.Comment: 28 pages, 9 figures (Accepted for publication in Physical Review B

    Trapping in complex networks

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    We investigate the trapping problem in Erdos-Renyi (ER) and Scale-Free (SF) networks. We calculate the evolution of the particle density ρ(t)\rho(t) of random walkers in the presence of one or multiple traps with concentration cc. We show using theory and simulations that in ER networks, while for short times ρ(t)exp(Act)\rho(t) \propto \exp(-Act), for longer times ρ(t)\rho(t) exhibits a more complex behavior, with explicit dependence on both the number of traps and the size of the network. In SF networks we reveal the significant impact of the trap's location: ρ(t)\rho(t) is drastically different when a trap is placed on a random node compared to the case of the trap being on the node with the maximum connectivity. For the latter case we find \rho(t)\propto\exp\left[-At/N^\frac{\gamma-2}{\gamma-1}\av{k}\right] for all γ>2\gamma>2, where γ\gamma is the exponent of the degree distribution P(k)kγP(k)\propto k^{-\gamma}.Comment: Appendix adde

    Linear and nonlinear rheology of wormlike micelles

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    Several surfactant molecules self-assemble in solution to form long, cylindrical, flexible wormlike micelles. These micelles can be entangled with each other leading to viscoelastic phases. The rheological properties of such phases are very interesting and have been the subject of a large number of experimental and theoretical studies in recent years. We shall report on our recent work on the macrorheology, microrheology and nonlinear flow behaviour of dilute aqueous solutions of a surfactant CTAT (Cetyltrimethylammonium Tosilate). This system forms elongated micelles and exhibits strong viscoelasticity at low concentrations (\sim 0.9 wt%) without the addition of electrolytes. Microrheology measurements of G(ω)G(\omega) have been done using diffusing wave spectroscopy which will be compared with the conventional frequency sweep measurements done using a cone and plate rheometer. The second part of the paper deals with the nonlinear rheology where the measured shear stress σ\sigma is a nonmonotonic function of the shear rate γ˙\dot{\gamma}. In stress-controlled experiments, the shear stress shows a plateau for γ˙\dot{\gamma} larger than some critical strain rate, similar to the earlier reports on CPyCl/NaSal system. Cates et al have proposed that the plateau is a signature of mechanical instability in the form of shear bands. We have carried out extensive experiments under controlled strain rate conditions, to study the time-dependence of shear stress. The measured time series of shear stress has been analysed in terms of correlation integrals and Lyapunov exponents to show unambiguously that the behaviour is typical of low dimensional dynamical systems.Comment: 15 pages, 10 eps figure

    Sequences of globally regular and black hole solutions in SU(4) Einstein-Yang-Mills theory

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    SU(4) Einstein-Yang-Mills theory possesses sequences of static spherically symmetric globally regular and black hole solutions. Considering solutions with a purely magnetic gauge field, based on the 4-dimensional embedding of su(2)su(2) in su(4)su(4), these solutions are labelled by the node numbers (n1,n2,n3)(n_1,n_2,n_3) of the three gauge field functions u1u_1, u2u_2 and u3u_3. We classify the various types of solutions in sequences and determine their limiting solutions. The limiting solutions of the sequences of neutral solutions carry charge, and the limiting solutions of the sequences of charged solutions carry higher charge. For sequences of black hole solutions with node structure (n,j,n)(n,j,n) and (n,n,n)(n,n,n), several distinct branches of solutions exist up to critical values of the horizon radius. We determine the critical behaviour for these sequences of solutions. We also consider SU(4) Einstein-Yang-Mills-dilaton theory and show that these sequences of solutions are analogous in most respects to the corresponding SU(4) Einstein-Yang-Mills sequences of solutions.Comment: 40 pages, 5 tables, 19 Postscript figures, use revtex.st

    First Passage Properties of the Erdos-Renyi Random Graph

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    We study the mean time for a random walk to traverse between two arbitrary sites of the Erdos-Renyi random graph. We develop an effective medium approximation that predicts that the mean first-passage time between pairs of nodes, as well as all moments of this first-passage time, are insensitive to the fraction p of occupied links. This prediction qualitatively agrees with numerical simulations away from the percolation threshold. Near the percolation threshold, the statistically meaningful quantity is the mean transit rate, namely, the inverse of the first-passage time. This rate varies non-monotonically with p near the percolation transition. Much of this behavior can be understood by simple heuristic arguments.Comment: 10 pages, 9 figures, 2-column revtex4 forma

    Sequences of Einstein-Yang-Mills-Dilaton Black Holes

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    Einstein-Yang-Mills-dilaton theory possesses sequences of neutral static spherically symmetric black hole solutions. The solutions depend on the dilaton coupling constant γ\gamma and on the horizon. The SU(2) solutions are labelled by the number of nodes nn of the single gauge field function, whereas the SO(3) solutions are labelled by the nodes (n1,n2)(n_1,n_2) of both gauge field functions. The SO(3) solutions form sequences characterized by the node structure (j,j+n)(j,j+n), where jj is fixed. The sequences of magnetically neutral solutions tend to magnetically charged limiting solutions. For finite jj the SO(3) sequences tend to magnetically charged Einstein-Yang-Mills-dilaton solutions with jj nodes and charge P=3P=\sqrt{3}. For j=0j=0 and jj \rightarrow \infty the SO(3) sequences tend to Einstein-Maxwell-dilaton solutions with magnetic charges P=3P=\sqrt{3} and P=2P=2, respectively. The latter also represent the scaled limiting solutions of the SU(2) sequence. The convergence of the global properties of the black hole solutions, such as mass, dilaton charge and Hawking temperature, is exponential. The degree of convergence of the matter and metric functions of the black hole solutions is related to the relative location of the horizon to the nodes of the corresponding regular solutions.Comment: 71 pages, Latex2e, 29 ps-figures include

    Exact eigenvalue spectrum of a class of fractal scale-free networks

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    The eigenvalue spectrum of the transition matrix of a network encodes important information about its structural and dynamical properties. We study the transition matrix of a family of fractal scale-free networks and analytically determine all the eigenvalues and their degeneracies. We then use these eigenvalues to evaluate the closed-form solution to the eigentime for random walks on the networks under consideration. Through the connection between the spectrum of transition matrix and the number of spanning trees, we corroborate the obtained eigenvalues and their multiplicities.Comment: Definitive version accepted for publication in EPL (Europhysics Letters

    O(12) limit and complete classification of symmetry schemes in proton-neutron interacting boson model

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    It is shown that the proton-neutron interacting boson model (pnIBM) admits new symmetry limits with O(12) algebra which break F-spin but preserves the quantum number M_F. The generators of O(12) are derived and the quantum number `v' of O(12) for a given boson number N is determined by identifying the corresponding quasi-spin algebra. The O(12) algebra generates two symmetry schemes and for both of them, complete classification of the basis states and typical spectra are given. With the O(12) algebra identified, complete classification of pnIBM symmetry limits with good M_F is established.Comment: 22 pages, 1 figur
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