L.J. Azevedo
Sandia National Laboratories
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Featured researches published by L.J. Azevedo.
Molecular Crystals and Liquid Crystals | 1986
Thomas J. Emge; Peter C. W. Leung; Mark A. Beno; Hau H. Wang; Millicent A. Firestone; Kevin S. Webb; K. Douglas Carlson; Jack M. Williams; E.L. Venturini; L.J. Azevedo; J. E. Schirber
Abstract In the isostructural series of β-(BEDT-TTF)2X organic metals, abbreviated β-(ET)2X, where X is a trihalide anion, I3-, I2Br- or IBr2-, and where ET is bis-(ethylenedithio) tetrathiafulvalene (C10S8H8), the salt containing the disordered asymmetric I2Br- anion has atypical structural and electronic properties compared to those containing the symmetrical and ordered I-3 and IBr2- anions.
Molecular Crystals and Liquid Crystals | 1985
L.J. Azevedo; E.L. Venturini; J. E. Schirber; Jack M. Williams; H. B. Wang; Thomas J. Emge
Abstract We have undertaken an electron spin resonance study at both low and high magnetic field on the superconducting phase of the ambient pressure superconductor (BEDT-TTF>2I3, (ET)2I3, over the temperature range 1-300 K and hydrostatic pressure range from 0 to 2 kbar. At ambient pressure the ESR results are consistent with the picture of (ET)2I3 as a metal. Superconductivity is observed at 1.6 K via low field ESR. Application of modest pressures strongly suppresses the superconducting transition temperature. At pressures above about 0.3 kbar the superconductivity is suppressed in favor of an as-yet-unidentified magnetic state whose onset is at 7K. Through an analysis of the microwave ESR lineshape we find that the microwave conductivity over the temperature range 5-50 K is in agreement with dc measurements.
Solid State Communications | 1987
F.L.A. Machado; W.G. Clark; L.J. Azevedo; D.P. Yang; W. A. Hines; J. I. Budnick; M.X. Quan
Abstract Low temperature heat capacity and magnetization measurements are reported for the Al 80 Mn 20 alloy in the quasicrystalline icosahedral phase. The heat capacity, which was measured for temperatures ranging from 0.5 to 5.0 K and magnetic fields up to 11.7 kOe, shows a broad magnetic contribution around 1.0 K. The linear electronic contribution does not indicate an anomalously high density-of-states at the Fermi energy as predicted theoretically for quasicrystalline systems. The d.c. magnetization, which was measured from 2.0 to 300 K and with magnetic fields up to 50 kOe, indicates an effective number of one 11 μ B localized magnetic moment for approximately every 100 Mn atoms. The low field susceptibility follows the Curie-Weiss law for temperatures ≧ 10 K, while a spin-glass-like ordering is observed at low temperatures.
Inorganic Chemistry | 1984
Jack M. Williams; Mark A. Beno; Hsien Hau Wang; Peter E. Reed; L.J. Azevedo; J. E. Schirber
Die elektrochemische Oxidation von Bis-[ethylendithiol-tetrathiafulven in 1,1,2-Trichlorethan in Gegenwart von Bu4N[ReO4] oder Bu4N[BrO4] als unterstutzende Elektrolyte fuhrt zu den Radikalkation-Titelsalzen.
Solid State Communications | 1987
F.L.A. Machado; W.G. Clark; D.P. Yang; W. A. Hines; L.J. Azevedo; B.C. Giessen; M.X. Quan
Abstract Low temperature heat capacity and magnetization measurements are reported for the quasicrystalline decagonal (T-phase) alloy Al7 8Mn2 2. The heat capacity measurements were performed over the temperature range from 0.5 to 5.0 K and for applied magnetic fields of zero and 12.7 kOe. In this range, the heat capacity is characterized by a broad anomaly near 1 K and no field dependence. The dc magnetization, which was measured from 1.7 to 300 K and with magnetic fields up to 50 kOe, indicates an effective number of one 25.6 μB localized moment for approximately every 240 Mn atoms. The magnetic susceptibility follows the Curie-Weiss law for T ≧ 15 K, while a spin-glass-like ordering is observed at 7.8 K. Comparisons are made with similar measurements previously reported for the related quasicrystalline icosahedral (I-phase) Al8 0Mn2 0 alloy.
Physica B-condensed Matter | 1981
L.J. Azevedo; J. E. Schirber; R. L. Greene; E. M. Engler
Abstract A high field phase transition in the metallic phase of the organic conductor (TMTSF) 2 PF 6 at low temperatures has been studied by measuring the spin lattice relaxation rate of the methyl group protons. The transition temperature increases with field, is highly pressure dependent and depends on the projection of the magnetic field along the crystalline c axis.
Journal of The Less Common Metals | 1986
David Emin; G. A. Samara; L.J. Azevedo; E.L. Venturini; H.H Madden; G.C Nelson; J.A Shelnutt; B. Morosin; M Moss; C. Wood
D.c. conductivity, Hall mobility and Seebeck coefficient measurements on boron carbides, B1−xCx (0.1 ⩽ x ⩽ 0.2), between 300 and 1200 K are interpreted in terms on the hopping of small bipolaronic holes between B11C icosahedra that are inequivalent in energy and electron-lattice coupling strength.
Molecular Crystals and Liquid Crystals | 1985
J. E. Schirber; L.J. Azevedo; Jack M. Williams
Abstract A contactless technique has been developed for tracking the metallic, spin density wave and superconducting ground states of organic superconductors as a function of pressure and temperature.
Solid State Communications | 1986
J. E. Schirber; L.J. Azevedo; J. F. Kwak; E.L. Venturini; Mark A. Beno; H.H. Wang; Jack M. Williams
Abstract A simple recipe for the formation and recovery at ambient pressure of the 8K superconducting state of β-(BEDT-TTF) 2 I 3 is described. This technique will facilitate detailed studies of the 8K state.
Physica B-condensed Matter | 1986
Jack M. Williams; Mark A. Beno; Hau H. Wang; Urs Geiser; Thomas J. Emge; Peter C. W. Leung; G. W. Crabtree; K. Douglas Carlson; L.J. Azevedo; E.L. Venturini; J. E. Schirber; J. F. Kwak; M.-H. Whangbo
Invited paper Ambient-pressure superconductivity has now been discovered in five systems based on BEDT-TTF:X, X - = polyatomic, monovalent anion. The highest T c reported is 5 K, in (BEDT-TTF) 2 AuI 2 , and it appears that much higher T c s are possible if disorder (molecular and anionic), and structural modulation, can be avoided in new derivatives containing monovalent triatomic anions. A modulated structure has been observed in (BEDT-TTF) 2 1, using neutron and X-ray scattering, but does not appear to form in (BEDT-TFF) 2 X, X = I 2 Br - , AuI - 2 and IBr2 down to T = 10-20 K.