1,059 research outputs found

    Ferromagnetic quantum critical fluctuations in YbRh_2(Si_{0.95}Ge_{0.05})_2

    Full text link
    The bulk magnetic susceptibility χ(T,B)\chi(T,B) of YbRh2_2(Si0.95_{0.95}Ge0.05_{0.05})2_2 has been investigated %by ac-and dc-magnetometry at low temperatures and close to the field-induced quantum critical point at Bc=0.027B_c=0.027 T. For B0.05B\leq 0.05 T a Curie-Weiss law with a negative Weiss temperature is observed at temperatures below 0.3 K. Outside this region, the susceptibility indicates ferromagnetic quantum critical fluctuations: χ(T)T0.6\chi(T)\propto T^{-0.6} above 0.3 K, while at low temperatures the Pauli susceptibility follows χ0(BBc)0.6\chi_0\propto (B-B_c)^{-0.6} and scales with the coefficient of the T2T^2 term in the electrical resistivity. The Sommerfeld-Wilson ratio is highly enhanced and increases up to 30 close to the critical field.Comment: Physical Review Letters, to be publishe

    Quantum criticality in the cubic heavy-fermion system CeIn_{3-x}Sn_x

    Full text link
    We report a comprehensive study of CeIn3x_{3-x}Snx_x (0.55x0.8)(0.55 \leq x \leq 0.8) single crystals close to the antiferromagnetic (AF) quantum critical point (QCP) at xc0.67x_c\approx 0.67 by means of the low-temperature thermal expansion and Gr\"uneisen parameter. This system represents the first example for a {\it cubic} heavy fermion (HF) in which TNT_{\rm N} can be suppressed {\it continuously} down to T=0. A characteristic sign change of the Gr\"uneisen parameter between the AF and paramagnetic state indicates the accumulation of entropy close to the QCP. The observed quantum critical behavior is compatible with the predictions of the itinerant theory for three-dimensional critical spinfluctuations. This has important implications for the role of the dimensionality in HF QCPs.Comment: Physical Review Letters, to be publishe

    Physics of Polymorphic Transitions in CeRuSn

    Full text link
    We report a detailed study of the polymorphic transitions in ternary stannide CeRuSn on high quality single crystals through a combination of X-ray diffraction experiments conducted at 300, 275 and 120 K, and measurements of the thermal expansion, magnetization, and resistivity, along main crystallographic axes. In addition, the transition was followed as a function of pressure up to 0.8 GPa. The present X-ray diffraction data show that the room temperature polymorph consists of the lattice doubled along the c axis with respect to the CeCoAl-type structure consistent with previous reports. Upon cooling, the compound undergoes two successive transitions, first to a quintuple (290 K) and than to a triple CeCoAl superstructure at 225 K. The transitions are accompanied by a tremendous volume change due to a strong shrinking of the lattice along the c axis, which is clearly observed in thermal expansion. We advance arguments that the volume collapse originates from an increasing number of crystallographically inequivalent Ce sites and the change of ratio between the short and long Ce-Ru bonds. The observed properties of the polymorphic transition in CeRuSn are reminiscent of the transition in elementary Cerium, suggesting that similar physics, i.e., a Kondo influenced transition and strong lattice vibrations might be the driving forces

    Storende elementen in beeld : de impact van menselijke artefacten op de landschapsbeleving nader onderzocht

    Get PDF
    Om beleidsopties in beeld te brengen, is de invloed onderzocht van de vormgeving van een drietal doorgaans vrij storende elementen op de impact die deze elementen hebben op de aantrekkelijkheid van het landschap. Het betreft windturbineparken, bedrijventerreinen en grote stallen. Bij alle drie elementen is gekeken naar het effect van mitigerende maatregelen, meestal in de vorm van beplanting, alsmede naar het afstandsverval van de impact. Voor windturbineparken is verder gekeken naar het aantal turbines, de hoogte van de masten en de opstelling. Voor bedrijventerreinen waren dit het soort terrein, de omvang, en de hoogte. Voor grote stallen waren het de lengte en het gebruikte materiaal voor de wanden, respectievelijk het dak. Een en ander is systematisch onderzocht middels foto’s en realistische fotomontages, waarbij een beoordelaar slechts één variant van (een element in) een bepaald landschap voorgelegd kreeg. De beoordelaars waren ruim 2000 leden van een panel van het onderzoeksbureau GfK

    Magnetic-Field Induced Quantum Critical Point in YbRh2_2Si2_2

    Full text link
    We report low-temperature calorimetric, magnetic and resistivity measurements on the antiferromagnetic (AF) heavy-fermion metal YbRh2_2Si2_2 (TN={T_N =} 70 mK) as a function of magnetic field BB. While for fields exceeding the critical value Bc0{B_{c0}} at which TN0{T_N\to0} the low temperature resistivity shows an AT2{AT^2} dependence, a 1/(BBc0){1/(B-B_{c0})} divergence of A(B){A(B)} upon reducing BB to Bc0{B_{c0}} suggests singular scattering at the whole Fermi surface and a divergence of the heavy quasiparticle mass. The observations are interpreted in terms of a new type of quantum critical point separating a weakly AF ordered from a weakly polarized heavy Landau-Fermi liquid state.Comment: accepted for publication in Phys. Rev. Let

    Tuning Heavy Fermion Systems into Quantum Criticality by Magnetic Field

    Full text link
    We discuss a series of thermodynamic, magnetic and electrical transport experiments on the two heavy fermion compounds CeNi2Ge2 and YbRh2Si2 in which magnetic fields, B, are used to tune the systems from a Non-Fermi liquid (NFL) into a field-induced FL state. Upon approaching the quantum-critical points from the FL side by reducing B we analyze the heavy quasiparticle (QP) mass and QP-QP scattering cross sections. For CeNi2Ge2 the observed behavior agrees well with the predictions of the spin-density wave (SDW) scenario for three-dimensional (3D) critical spin-fluctuations. By contrast, the observed singularity in YbRh2Si2 cannot be explained by the itinerant SDW theory for neither 3D nor 2D critical spinfluctuations. Furthermore, we investigate the magnetization M(B) at high magnetic fields. For CeNi2Ge2 a metamagnetic transition is observed at 43 T, whereas for YbRh2Si2 a kink-like anomaly occurs at 10 T in M vs B (applied along the easy basal plane) above which the heavy fermion state is completely suppressed.Comment: 15 pages, 8 figures, submitted to Journal of Low Temperature Physics, special Series on "High Magnetic Field Facilities

    Specific heat of heavy fermion CePd2Si2 in high magnetic fields

    Full text link
    We report specific heat measurements on the heavy fermion compound CePd2Si2 in magnetic fields up to 16 T and in the temperature range 1.4-16 K. A sharp peak in the specific heat signals the antiferromagnetic transition at T_N ~ 9.3 K in zero field. The transition is found to shift to lower temperatures when a magnetic field is applied along the crystallographic a-axis, while a field applied parallel to the tetragonal c-axis does not affect the transition. The magnetic contribution to the specific heat below T_N is well described by a sum of a linear electronic term and an antiferromagnetic spin wave contribution. Just below T_N, an additional positive curvature, especially at high fields, arises most probably due to thermal fluctuations. The field dependence of the coefficient of the low temperature linear term, gamma_0, extracted from the fits shows a maximum at about 6 T, at the point where an anomaly was detected in susceptibility measurements. The relative field dependence of both T_N and the magnetic entropy at T_N scales as [1-(B/B_0)^2] for B // a, suggesting the disappearance of antiferromagnetism at B_0 ~ 42 T. The expected suppression of the antiferromagnetic transition temperature to zero makes the existence of a magnetic quantum critical point possible.Comment: to be published in Journal of Physics: Condensed Matte
    corecore