3,475 research outputs found

    Evolution of correlation strength in KxFe(2-y)Se2 superconductor doped with S

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    We report the evolution of thermal transport properties of iron-based superconductor Kx_xFe2y_{2-y}Se2_2 with sulfur substitution at Se sites. Sulfur doping suppresses the superconducting TcT_c as well as the Seebeck coefficient. The Seebeck coefficient of all crystals in the low temperature range can be described very well by diffusive thermoelectric response model. The zero-temperature extrapolated value of Seebeck coefficient divided by temperature S/TS/T gradually decreases from 0.48μV/K2-0.48 \mu V/K^2 to a very small value \sim 0.03 μ\muV/K2^2 where TcT_c is completely suppressed. The normal state electron Sommerfeld term (γn\gamma_n) of specific heat also decreases with the increase of sulfur content. The dcrease of S/TS/T and γn\gamma_n reflects a suppression of the density of states at the Fermi energy, or a change in the Fermi surface that would induce the suppression of correlation strength.Comment: 5 Pages, 4 figures, 1 Table; submitted to Physical Review

    DILEMA: KIBER ILI SAJBER

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    Assuming that all the wider application of information technology, in addition to a number of diverse changes, in our lives introduces new terminology, which, unfortunately, too easily and uncritically, and often without an elementary understanding of the essence of the meaning of terms, easily introduces in our language, causing problems and dilemmas in their use, the author wishes to in this paper point to several open questions of terminology and also to try to clarify the dilemma of using the term: kiber or cyber.Polazeći od činjenice da sve šira primena informacione tehnologije, pored niza najraznovrsnijih promena, u naš život uvodi i novu terminologiju, koja se, nažalost, olako, nekritički, a često i bez elementarnog razumevanja suštine značenja pojedinih termina, olako uvodi u naš jezik, izazivajući probleme i dileme u njihovoj upotrebi, autor želi da u ovom prilogu ukaže na nekoliko otvorenih terminoloških pitanja i istovremeno da pokuša da razjasni dilemu upotrebe termina: kiber ili sajber

    121,123Sb NQR as a microscopic probe in Te doped correlated semimetal FeSb2 : emergence of electronic Griffith phase, magnetism and metallic behavior %

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    121,123Sb^{121,123}Sb nuclear quadrupole resonance (NQR) was applied to Fe(Sb1xTex)2Fe(Sb_{1-x}Te_x)_2 in the low doping regime (\emph{x = 0, 0.01} and \emph{0.05}) as a microscopic zero field probe to study the evolution of \emph{3d} magnetism and the emergence of metallic behavior. Whereas the NQR spectra itself reflects the degree of local disorder via the width of the individual NQR lines, the spin lattice relaxation rate (SLRR) 1/T1(T)1/T_1(T) probes the fluctuations at the SbSb - site. The fluctuations originate either from conduction electrons or from magnetic moments. In contrast to the semi metal FeSb2FeSb_2 with a clear signature of the charge and spin gap formation in 1/T1(T)T(exp/(ΔkBT))1/T_1(T)T ( \sim exp/ (\Delta k_BT) ) , the 1\% TeTe doped system exhibits almost metallic conductivity and a almost filled gap. A weak divergence of the SLRR coefficient 1/T1(T)TTnT0.21/T_1(T)T \sim T^{-n} \sim T^{-0.2} points towards the presence of electronic correlations towards low temperatures wheras the \textit{5\%} TeTe doped sample exhibits a much larger divergence in the SLRR coefficient showing 1/T1(T)TT0.721/T_1(T)T \sim T^{-0.72} . According to the specific heat divergence a power law with n = 2 m = 0.56n\ =\ 2\ m\ =\ 0.56 is expected for the SLRR. Furthermore TeTe-doped FeSb2FeSb_2 as a disordered paramagnetic metal might be a platform for the electronic Griffith phase scenario. NQR evidences a substantial asymmetric broadening of the 121,123Sb^{121,123}Sb NQR spectrum for the \emph{5\%} sample. This has purely electronic origin in agreement with the electronic Griffith phase and stems probably from an enhanced SbSb-TeTe bond polarization and electronic density shift towards the TeTe atom inside SbSb-TeTe dumbbell

    Thermoelectric studies of KxFe2-ySe2: weakly correlated superconductor

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    We report thermal transport measurement of KxFe2-ySe2 superconducting single crystal. Significant peak anomaly in thermal conductivity is observed at nearly TC/2 indicating a large phonon mean-free-path in the superconducting state. The zero-temperature extrapolated thermoelectric power is smaller than the value in typical strongly correlated superconductors, implying large normalized Fermi temperature. In contrast to other iron superconductors, thermoelectric power in our sample does not exhibit significant anomalies. These findings indicate that KxFe2-ySe2 is a weakly or intermediately correlated superconductor without significant Fermi surface nesting.Comment: Revised version, 5 pages, 5 figures, Will appear in Physical Review

    Wiedemann-Franz law and non-vanishing temperature scale across the field-tuned quantum critical point of YbRh2Si2

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    The in-plane thermal conductivity kappa(T) and electrical resistivity rho(T) of the heavy-fermion metal YbRh2Si2 were measured down to 50 mK for magnetic fields H parallel and perpendicular to the tetragonal c axis, through the field-tuned quantum critical point, Hc, at which antiferromagnetic order ends. The thermal and electrical resistivities, w(T) and rho(T), show a linear temperature dependence below 1 K, typical of the non-Fermi liquid behavior found near antiferromagnetic quantum critical points, but this dependence does not persist down to T = 0. Below a characteristic temperature T* ~ 0.35 K, which depends weakly on H, w(T) and rho(T) both deviate downward and converge in the T = 0 limit. We propose that T* marks the onset of short-range magnetic correlations, persisting beyond Hc. By comparing samples of different purity, we conclude that the Wiedemann-Franz law holds in YbRh2Si2, even at Hc, implying that no fundamental breakdown of quasiparticle behavior occurs in this material. The overall phenomenology of heat and charge transport in YbRh2Si2 is similar to that observed in the heavy-fermion metal CeCoIn5, near its own field-tuned quantum critical point.Comment: 8 figures, 8 page

    Comment on "Spatial optical solitons in highly nonlocal media" and related papers

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    In a recent paper [A. Alberucci, C. Jisha, N. Smyth, and G. Assanto, Phys. Rev. A 91, 013841 (2015)], Alberucci et al. have studied the propagation of bright spatial solitary waves in highly nonlocal media. We find that the main results in that and related papers, concerning soliton shape and dynamics, based on the accessible soliton (AS) approximation, are incorrect; the correct results have already been published by others. These and other inconsistencies in the paper follow from the problems in applying the AS approximation in earlier papers by the group that propagated to the later papers. The accessible soliton theory cannot describe accurately the features and dynamics of solitons in highly nonlocal media.Comment: 2 page

    Enhanced Magnetization from Proton Irradiated Bulk van der Waals Magnet CrSiTe3

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    Van der Waals (vdWs) crystals have attracted a great deal of scientific attention due to their interesting physical properties and widespread practical applications. Among all, CrSiTe3 (CST) is a ferromagnetic semiconductor with the Curie temperature (TC) of ~32 K. In this letter, we study the magnetic properties of bulk CST single-crystal upon proton irradiation with the fluence of 1x1018 protons/cm2. Most significantly, we observed an enhancement (23%) in the saturation magnetization from 3.9 {\mu}B to 4.8 {\mu}B and is accompanied by an increase in the coercive field (465-542 Oe) upon proton irradiation. Temperature-dependent X-band electron paramagnetic resonance measurements show no additional magnetically active defects/vacancies that are generated upon proton irradiation. The findings from X-ray photoelectron spectroscopy and Raman measurements lead us to believe that modification in the spin-lattice coupling and introduction of disorder could cause enhancement in saturation magnetization. This work demonstrates that proton irradiation is a feasible method in modifying the magnetic properties of vdWs crystals, which represents a significant step forward in designing future spintronic and magneto-electronic applications
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