368 research outputs found

    Mossbauer and magnetization studies of amorphous NdFeB compositionally modulated thin films

    Get PDF
    Several NdFeB compositionally modulated thin films are studied by using both conversion electron Mossbauer spectra and SQUID (superconducting quantum-interference-device) magnetometry. Both the hyperfine fields and the easy magnetization magnitude are not correlated with the modulation characteristic length (lambda) while the magnetization perpendicular to the thin-film plane decreases as lambda increases. The spectra were recorded at room temperature being the gamma rays perpendicular to the substrate plane. The magnetization measurements were recorded by using a SHE SQUID magnetometer in applied magnetic fields up to 5.5 T and in the temperature range between 1.8 and 30 K

    Ultra-high critical current densities of superconducting YBa2_2Cu3_3O7−δ_{7-\delta} thin films in the overdoped state

    Full text link
    Doping is one of the most relevant paths to tune the functionality of cuprates, it determines carrier density and the overall physical properties of these impressive superconducting materials. We present an oxygen doping study of YBa2_2Cu3_3O7−δ_{7-\delta} (YBCO) thin films from underdoped to overdoped state, correlating the measured charge carrier density, nHn_\textrm{H}, the hole doping, pp, and the critical current density, JcJ_\textrm{c}. Our results show a continuous increase of JcJ_\textrm{c} with charge carrier density, reaching 90 MA/cm2^2 at 5 K for pp-doping at the Quantum Critical Point (QCP), linked to an increase of the superconducting condensation energy. The ultra-high JcJ_\textrm{c} achived corresponds to a third of the depairing current, i.e. a value 60 % higher than ever reported in YBCO films. The overdoped regime is characterized by a sudden increase of nHn_\textrm{H}, associated to the reconstruction of the Fermi-surface at the QCP. Overdoping YBCO opens a promising route to extend the current carrying capabilities of REBCO coated conductors for applications

    Observation of insulator-metal transition in EuNiO3_{3} under high pressure

    Full text link
    The charge transfer antiferromagnetic (TN_{N} =220 K) insulator EuNiO3_{3} undergoes, at ambient pressure, a temperature-induced metal insulator MI transition at TMI_{MI}=463 K. We have investigated the effect of pressure (up to p~20 GPa) on the electronic, magnetic and structural properties of EuNiO3_{3} using electrical resistance measurements, {151}^Eu nuclear resonance scattering of synchrotron radiation and x-ray diffraction, respectively. With increasing pressure we find at pc_{c} =5.8 GPa a transition from the insulating state to a metallic state, while the orthorhombic structure remains unchanged up to 20 GPa. The results are explained in terms of a gradual increase of the electronic bandwidth with increasing pressure, which results in a closing of the charge transfer gap. It is further shown that the pressure-induced metallic state exhibits magnetic order with a lowervalue of TN_{N} (TN_{N} ~120 K at 9.4 GPa) which disappears between 9.4 and 14.4 GPa.Comment: 10 pages, 3 figure

    A hidden Goldstone mechanism in the Kagom\'e lattice antiferromagnet

    Full text link
    In this paper, we study the phases of the Heisenberg model on the \kagome lattice with antiferromagnetic nearest neighbour coupling J1J_1 and ferromagnetic next neighbour coupling J2J_2. Analysing the long wavelength, low energy effective action that describes this model, we arrive at the phase diagram as a function of χ=J2J1\chi = \frac{J_2}{J_1} . The interesting part of this phase diagram is that for small χ\chi, which includes χ=0\chi =0, there is a phase with no long range spin order and with gapless and spin zero low lying excitations. We discuss our results in the context of earlier, numerical and experimental work.Comment: 21 pages, latex file with 5 figure

    Complejos de cefalexina con cationes de elementos del cuarto periodo. I.-Estudio en disolución acuosa

    Get PDF
    The formation of the complexes, in aqueous solution, between the cephalexin and sorne ious of the fourth period elements has been investigated by potentiometric and spectrophotometric methods. The stability constants has been determinated.Se ha investigado la formación de complejos, en disolución acuosa, de cefalexina [ácido 7-(D-2-amino-2-fenil-acetamido )-3-metil-8-oxo-S-tia-1-azabiciclo [4.2.O] oct-2-eno-2-carboxilico] con cationes de elementos del cuarto período, por métodos potenciométricos y espectrofotométricos. Se han determinado asímismo las constantes de formación de complejos

    Complejos de cefalexina con cationes de elementos del cuarto periodo. I.-Estudio en disolución acuosa

    Get PDF
    Se ha investigado la formación de complejos, en disolución acuosa, de cefalexina [ácido 7-(D-2-amino-2-fenil-acetamido )-3-metil-8-oxo-S-tia-1-azabiciclo [4.2.O] oct-2-eno-2-carboxilico] con cationes de elementos del cuarto período, por métodos potenciométricos y espectrofotométricos. Se han determinado asímismo las constantes de formación de complejos.The formation of the complexes, in aqueous solution, between the cephaIexin and sorne ious of the fourth period elements has been investigated by potentiometric and spectrophotometric methods. The stability constants has been determinated

    Magneto-thermodynamics of the spin-1/2 Kagome antiferromagnet

    Full text link
    In this paper, we use a new hybrid method to compute the thermodynamic behavior of the spin-1/2 Kagome antiferromagnet under the influence of a large external magnetic field. We find a T^2 low-temperature behavior and a very low sensitivity of the specific heat to a strong external magnetic field. We display clear evidence that this low temperature magneto-thermal effect is associated to the existence of low-lying fluctuating singlets, but also that the whole picture (T^2 behavior of Cv and thermally activated spin susceptibility) implies contribution of both non magnetic and magnetic excitations. Comparison with experiments is made.Comment: 4 pages, LaTeX 2.09 and RevTeX with 3 figures embedded in the text. Version to appear in Phys. Rev. Let
    • …
    corecore