3,382 research outputs found

    Manifestation of geometric frustration on magnetic and thermodynamic properties of pyrochlores Sm2X2O7Sm_2X_2O_7 (X=Ti, Zr)

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    We present here magnetization, specific heat and Raman studies on single-crystalline specimens of the first pyrochlore member Sm2Ti2O7Sm_2Ti_2O_7 of the rare-earth titanate series. Its analogous compound Sm2Zr2O7Sm_2Zr_2O_7 in the rare-earth zirconate series is also investigated in the polycrystalline form. The Sm spins in Sm2Ti2O7Sm_2Ti_2O_7 remain unordered down to at least T = 0.5 K. The absence of magnetic ordering is attributed to very small values of exchange (θcw 0.26K\theta_{cw} ~ -0.26 K) and dipolar interaction (μeff 0.15μB\mu_{eff} ~ 0.15 \mu_B) between the Sm3+Sm^{3+} spins in this pyrochlore. In contrast, the pyrochlore Sm2Zr2O7Sm_2Zr_2O_7 is characterized by a relatively large value of Sm-Sm spin exchange (θcw 10K\theta_{cw} ~ - 10 K); however, long-range ordering of the Sm3+Sm^{3+} spins is not established at least down to T = 0.67 K, due to frustration of the Sm3+Sm^{3+} spins on the pyrochlore lattice. The ground state of Sm3+Sm^{3+} ions in both pyrochlores is a well-isolated Kramer's doublet. The higher-lying crystal field excitations are observed in the low-frequency region of the Raman spectra of the two compounds recorded at T = 10 K. At higher temperatures, the magnetic susceptibility of Sm2Ti2O7Sm_2Ti_2O_7 shows a broad maximum at T = 140 K while that of Sm2Zr2O7Sm_2Zr_2O_7 changes monotonically. Whereas Sm2Ti2O7Sm_2Ti_2O_7 is a promising candidate for investigating spin-fluctuations on a frustrated lattice as indicated by our data, the properties of Sm2Zr2O7Sm_2Zr_2O_7 seem to conform to a conventional scenario where geometrical frustration of the spin exclude their long-range ordering.Comment: 24 pages, 6 figures, Accepted for publication in Phys. Rev.

    Correlated Prompt Fission Data in Transport Simulations

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    Detailed information on the fission process can be inferred from the observation, modeling and theoretical understanding of prompt fission neutron and γ\gamma-ray~observables. Beyond simple average quantities, the study of distributions and correlations in prompt data, e.g., multiplicity-dependent neutron and \gray~spectra, angular distributions of the emitted particles, nn-nn, nn-γ\gamma, and γ\gamma-γ\gamma~correlations, can place stringent constraints on fission models and parameters that would otherwise be free to be tuned separately to represent individual fission observables. The FREYA~and CGMF~codes have been developed to follow the sequential emissions of prompt neutrons and γ\gamma-rays~from the initial excited fission fragments produced right after scission. Both codes implement Monte Carlo techniques to sample initial fission fragment configurations in mass, charge and kinetic energy and sample probabilities of neutron and γ\gamma~emission at each stage of the decay. This approach naturally leads to using simple but powerful statistical techniques to infer distributions and correlations among many observables and model parameters. The comparison of model calculations with experimental data provides a rich arena for testing various nuclear physics models such as those related to the nuclear structure and level densities of neutron-rich nuclei, the γ\gamma-ray~strength functions of dipole and quadrupole transitions, the mechanism for dividing the excitation energy between the two nascent fragments near scission, and the mechanisms behind the production of angular momentum in the fragments, etc. Beyond the obvious interest from a fundamental physics point of view, such studies are also important for addressing data needs in various nuclear applications. (See text for full abstract.)Comment: 39 pages, 57 figure files, published in Eur. Phys. J. A, reference added this versio

    New object and new place reactions of Rattus meltada

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    Are Steadily Moving Crystals Unstable?

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    We study the dynamics of small fluctuations about the uniform state of a crystal moving through a dissipative medium, e.g. a sedimenting colloidal crystal or a moving flux lattice, using a set of continuum equations for the displacement fields, and a one-dimensional driven lattice-gas model for the coupled concentration and tilt fields. For the colloidal crystal we predict a continuous nonequilibrium phase transition to a clumped state above a critical Peclet number.Comment: 4 pages, revtex, 2 .eps figures, uses epsf.sty; To be published in Phys. Rev. Lett. This version is substantially rewritten but the essential content is the same as befor

    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

    Open and endovascular repair of the nontraumatic isolated aortic arch aneurysm

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    ObjectiveRepair of isolated aortic arch aneurysms (nontraumatic) by either open (OAR) or endovascular (TEVAR) methods is associated with need for hypothermic circulatory arrest, complex debranching procedures, or use of marginal proximal landing zones. This study evaluates outcomes for treatment of this cohort.MethodsOf 2153 patients undergoing arch repair (1993-2013), 137 (mean age, 60 years) were treated with isolated arch resection for nontraumatic aneurysms. Treatment was by open (n = 93), hybrid (n = 11), or TEVAR (n = 33) methods, with the last two approaches reserved for poor OAR candidates. Treatment was predominantly for saccular (n = 53) or fusiform (n = 30) aneurysms or dissection (n = 15). Rupture was present in 15%. Prior aortic repair was performed in the ascending (n = 30), arch (n = 40), descending (n = 24), or abdominal (n = 9) aorta. Propensity score adjustment was performed for multivariable analysis to account for baseline differences in patient groups as well as treatment selection bias.ResultsEarly mortality was seen in nine patients (7%). Morbidity included stroke (n = 9), paraplegia (n = 1), and need for dialysis (n = 5) or tracheostomy (n = 10). A composite outcome of death and stroke was independently predicted by advancing age (P = .055) and performance of a hybrid procedure (P = .012). The 15-year survival was 59%, with late mortality predicted by increasing age, presence of peripheral vascular disease, and perioperative stroke (all P < .05). The 10-year freedom from aortic rupture or reintervention was 75% and was higher after OAR (2-year OAR, 94% vs TEVAR or hybrid, 78%; P = .018). After propensity-adjusted Cox regression analysis, both prior abdominal aortic aneurysmectomy (P = .017) and an endovascular or hybrid procedure (P = .001) independently predicted late aortic rupture or need for reintervention.ConclusionsIsolated arch repair remains a high-risk procedure occurring frequently in the reoperative setting. Despite being performed in a higher risk group, endovascular strategies yielded similar outcomes but with an increased risk for aorta-related complications. These data support ongoing efforts to develop branched endografts specifically tailored for arch disease to potentially reduce morbidity related to currently available approaches

    Granger Causality and Cross Recurrence Plots in Rheochaos

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    Our stress relaxation measurements on wormlike micelles using a Rheo-SALS (rheology + small angle light scattering) apparatus allow simultaneous measurements of the stress and the scattered depolarised intensity. The latter is sensitive to orientational ordering of the micelles. To determine the presence of causal influences between the stress and the depolarised intensity time series, we have used the technique of linear and nonlinear Granger causality. We find there exists a feedback mechanism between the two time series and that the orientational order has a stronger causal effect on the stress than vice versa. We have also studied the phase space dynamics of the stress and the depolarised intensity time series using the recently developed technique of cross recurrence plots (CRPs). The presence of diagonal line structures in the CRPs unambiguously proves that the two time series share similar phase space dynamics.Comment: 10 pages, 7 figure

    Mean-field analysis of the q-voter model on networks

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    We present a detailed investigation of the behavior of the nonlinear q-voter model for opinion dynamics. At the mean-field level we derive analytically, for any value of the number q of agents involved in the elementary update, the phase diagram, the exit probability and the consensus time at the transition point. The mean-field formalism is extended to the case that the interaction pattern is given by generic heterogeneous networks. We finally discuss the case of random regular networks and compare analytical results with simulations.Comment: 20 pages, 10 figure

    Non-resonant microwave absorption studies of superconducting MgB_2

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    Non-resonant microwave absorption(NRMA) studies of superconducting MgB_2 at a frequency of 9.43 GHz in the field range -50 Gauss to 5000 Gauss are reported. The NRMA results indicate near absence of intergranular weak links. A linear temperature dependence of the lower critical field H_c1 is observed indicating a non s-wave superconductivity. However, the phase reversal of the NRMA signal which could suggest d-wave symmetry is also not observed.Comment: 8 pages, 2 figure
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