1,327 research outputs found

    Ytterbium divalency and lattice disorder in near-zero thermal expansion YbGaGe

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    While near-zero thermal expansion (NZTE) in YbGaGe is sensitive to stoichiometry and defect concentration, the NZTE mechanism remains elusive. We present x-ray absorption spectra that show unequivocally that Yb is nearly divalent in YbGaGe and the valence does not change with temperature or with nominally 1% B or 5% C impurities, ruling out a valence-fluctuation mechanism. Moreover, substantial changes occur in the local structure around Yb with B and C inclusion. Together with inelastic neutron scattering measurements, these data indicate a strong tendency for the lattice to disorder, providing a possible explanation for NZTE in YbGaGe.Comment: 4 pages, 4 figure, supplementary inf

    Understanding the complex phase diagram of uranium: the role of electron-phonon coupling

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    We report an experimental determination of the dispersion of the soft phonon mode along [1,0,0] in uranium as a function of pressure. The energies of these phonons increase rapidly, with conventional behavior found by 20 GPa, as predicted by recent theory. New calculations demonstrate the strong pressure (and momentum) dependence of the electron-phonon coupling, whereas the Fermi-surface nesting is surprisingly independent of pressure. This allows a full understanding of the complex phase diagram of uranium, and the interplay between the charge-density wave and superconductivity

    Elastic and thermodynamic properties of the shape-memory alloy AuZn

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    The current work reports on the elastic shear moduli, internal friction, and the specific heat of the B2 cubic ordered alloy AuZn as a function of temperature. Measurements were made on single-crystal and polycrystalline samples using Resonant Ultrasound Spectroscopy (RUS), semi-adiabatic calorimetry and stress-strain measurements. Our results confirm that this alloy exhibits the shape-memory effect and a phase transition at 64.75 K that appears to be continuous (second-order) from the specific heat data. It is argued that the combination of equiatomic composition and a low transformation temperature constrain the chemical potential and its derivatives to exhibit behavior that lies at the borderline between that of a first-order (discontinuous) and a continuous phase transition. The acoustic dissipation does not peak at the transtion temperature as expected, but shows a maximum well into the low-temperature phase. The Debye temeprature value of 219 K, obtained from the low-temperature specific heat data is in favorable agreement with that determined from the acoustic data (207 K) above the transition.Comment: 25 pages, 6 figures, submitted to Phys. Rev.

    Experimental electronic heat capacities of α\alpha- and δ\delta-Plutonium; heavy-fermion physics in an element

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    We have measured the heat capacities of δ\delta-Pu0.95_{0.95}Al0.05_{0.05} and α\alpha-Pu over the temperature range 2-303 K. The availability of data below 10 K plus an estimate of the phonon contribution to the heat capacity based on recent neutron-scattering experiments on the same sample enable us to make a reliable deduction of the electronic contribution to the heat capacity of δ\delta-Pu0.95_{0.95}Al0.05_{0.05}; we find γ=64±3\gamma = 64 \pm 3 mJK2^{-2}mol1^{-1} as T0T \to 0. This is a factor 4\sim 4 larger than that of any element, and large enough for δ\delta-Pu0.95_{0.95}Al0.05_{0.05} to be classed as a heavy-fermion system. By contrast, γ=17±1\gamma = 17 \pm 1 mJK2^{-2}mol1^{-1} in α\alpha-Pu. Two distinct anomalies are seen in the electronic contribution to the heat capacity of δ\delta-Pu0.95_{0.95}Al0.05_{0.05}, one or both of which may be associated with the formation of the α\alpha'- martensitic phase. We suggest that the large γ\gamma-value of δ\delta-Pu0.95_{0.95}Al0.05_{0.05} may be caused by proximity to a quantum-critical point.Comment: 4 pages, 4 figure

    In vivo staging of frontotemporal lobar degeneration TDP-43 type C pathology

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    Background: TDP-43 type C is one of the pathological forms of frontotemporal lobar degeneration (FTLD) and mainly associated clinically with the semantic variant of primary progressive aphasia (svPPA). We aimed to define in vivo the sequential pattern of neuroanatomical involvement in a cohort of patients with FTLD-TDP type C pathology. Methods: We extracted the volumes of a set of cortical and subcortical regions from MRI scans of 19 patients with post mortem confirmed TDP-43 type C pathology (all with left hemisphere-predominant atrophy at baseline). In the initial development phase, we used w-scores computed from 81 cognitively normal controls to define a set of sequential stages of neuroanatomical involvement within the FTLD-TDP type C cohort where a w-score of < − 1.65 was considered abnormal. In a subsequent validation phase, we used 31 follow-up scans from 14 of the 19 patients in the same cohort to confirm the staging model. Results: Four sequential stages were identified in the initial development phase. Stage 1 was defined by atrophy in the left amygdala, medial temporal cortex, temporal pole, lateral temporal cortex and right medial temporal cortex; Stage 2 by atrophy in the left supratemporal cortex; Stage 3 by atrophy in the right anterior insula; and Stage 4 by atrophy in the right accumbens. In the validation phase, calculation of w-scores in the longitudinal scans confirmed the staging system, with all patients either staying in the same stage or progressing to a later stage at follow-up. Conclusion: In vivo imaging is able to detect distinct stages of neuroanatomical involvement in FTLD-TDP type C pathology. Using an imaging-derived staging system allows a more refined stratification of patients with svPPA during life

    Coulomb-U and magnetic moment collapse in δ\delta-Pu

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    The around-the-mean-field version of the LDA+U method is applied to investigate electron correlation effects in δ\delta-Pu. It yields a non-magnetic ground state of δ\delta-Pu, and provides a good agreement with experimental equilibrium volume, bulk modulus and explains important features of the photoelectron spectra
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