J. D. Jorgensen’s research while affiliated with Lawrence Livermore National Laboratory and other places
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The 2nd Polish-US Conference held at Wrocław and Karpacz, Poland, 17-21 August 1998;
Proceedings:
New Developments in High Temperature Superconductivity, Springer LNP 545, Eds. J. Klamut, B.W. Veal, B.M. Dabrowski, P.W. Klamut, M. Kazimierski
The crystal structure of PrCoO 3 has been studied with high-resolution neutron powder diffraction and pair-distribution-function analysis in the temperature range from 12–600 K. The compound has the orthorhombic (Pbnm) perovskite structure over the entire temperature range. The temperature dependence of the average Co-O bond length shows clear anomalies near 60 K and 200 K where anomalous temperature dependencies of thermal conductivity and magnetic susceptibility have been reported. The data show a constant intermediate-spin-state fraction within 60 < T < 200 K and excitation of high-spin-state Co(III) above 200 K.
Mixed-conducting ceramic oxides have potential uses in high-temperature electrochemical applications such as solid oxide fuel cells, batteries, sensors, and oxygen-permeable membranes. The Sr-Fe-Co-O system combines high electronic/ionic conductivity with appreciable oxygen permeability at elevated temperatures. Dense ceramic membranes made of this material can be used to separate high-purity oxygen from air without the need for external electrical circuitry, or to partially oxidize methane to produce syngas. Samples of SrâFe{sub 3-x}CoâO{sub y} (with x = 0, 0.6, 1.0, and 1.4) were prepared by solid-state reaction method in atmospheres with various oxygen partial pressures (pOâ) and were characterized by X-ray diffraction, scanning electron microscopy, and electrical conductivity testing. Phase components of the sample are dependent on cobalt concentration and pOâ. Electrical conductivity increases with increasing temperature and cobalt content in the material.
The mixed-conducting Sr-Fe-Co oxide has potential use as a gas separation membrane. Its superior oxygen transport reveals the feasibility of using oxide membranes in large-scale oxygen separation. Sr2Fe3-xCoxOy (with x = 0.0, 0.3, 0.6, and 1.0) samples were made by solid state reaction. To understand the oxygen transport mechanism in this system, conductivity and thermogravimetry experiments were conducted at high temperature in various oxygen partial pressure environments. The oxygen diffusion coefficient was determined from the time relaxation transient behavior of the specimen after switching the surrounding atmosphere. Mobility of the charge carrier was derived from relative conductivity and weight changes. X-ray diffraction experiments were carried out on these samples to determine their crystal structures.
The potential applications of mixed-conducting ceramic oxides include solid-oxide fuel cells, rechargeable batteries, gas sensors and oxygen-permeable membranes. Several perovskite-derived mixed Sr-Fe-Co oxides show not only high electrical-conductivity but also appreciable oxygen-permeability at elevated temperatures. For example, dense ceramic membranes of SrFeCo0.5O3-δ can be used to separate oxygen from air without the need for external electrical circuitry. The separated oxygen can be directly used for the partial oxidation of methane to produce syngas. Quantitative phase analysis of the SrFeCo0.5O3-δ material has revealed that it is predominantly composed of two Sr-Fe-Co-O systems, Sr4Fe6-xCoxO13 and SrFe1−xCoxO3-δ. Here we report preliminary structural findings on the SrFe1−xCoxO3-δ (0 ≤ x ≥ 0.3) system.
We discuss the effects of doping on the Cu chain sites in YBa2Cu3−xMxO6+y. The relationship between bond lengths obtained from neutron scattering and charge transfer is evaluated in terms of bond valence. In particular, it is concluded that removing an oxygen from the chains transfers one electron to the planes.
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http://dx.doi.org/10.1557/PROC-156-119
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@inproceedings{OPL:8118834,author = {Miceli,P. F. and Tarascon,J. M. and Greene,L. H. and Barboux,P. and Jorgensen,J. D. and Rhyne,J. J. and Neumann,D. A.},title = {Charge Transfer and Bond Lengths in YBa2Cu3−xMxO6+y},booktitle = {Symposium M – High Temperature Superconductors: Relationships Between Properties, Structure, and Solid State Chemistry},series = {MRS Proceedings},volume = {156},year = {1989},doi = {10.1557/PROC-156-119},URL = {http://journals.cambridge.org/article_S1946427400386043},}
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Charge Transfer and Bond Lengths in YBa2Cu3−xMxO6+y
P. F. Miceli,J. M. Tarascon,L. H. Greene,P. Barboux,J. D. Jorgensen,J. J. Rhyne and D. A. Neumann (1989).
MRS Proceedings , Volume 156 , 1989, 119
http://journals.cambridge.org/action/displayAbstract?aid=8118834
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Charge Transfer and Bond Lengths in YBa2Cu3−xMxO6+y
P. F. Miceli,
J. M. Tarascon,
L. H. Greene,
P. Barboux,
J. D. Jorgensen,
J. J. Rhyne
and D. A. Neumann 1989
MRS Proceedings,
,Volume156,
1989,
119
http://journals.cambridge.org/abstract_S1946427400386043
P. F. Miceli,
J. M. Tarascon,
L. H. Greene,
P. Barboux,
J. D. Jorgensen,
J. J. Rhyne
and D. A. Neumann
(1989).
Charge Transfer and Bond Lengths in YBa2Cu3−xMxO6+y.
MRS Proceedings,
156,
119
doi:10.1557/PROC-156-119.
0Comments
We have determined the crystal structures of five phases in the Bal-xKxBiO3 system for 0≤x≤0.5 and 10K≤T≤473K. Superconductivity occurs only in a cubic perovskite phase with the maximum Tc at the transition to an orthorhombic, Ibmm, phase. The commensurate structure of this orthorhombic phase, which involves only tilting of the Bi06 octahedra, provides no explanation for its non-metallic behavior. However, an incommensurate structural modulation, observed by electron diffraction, may provide a rationalization. Thus, the maximum Tc at the phase boundary may result from competition between superconductivity and a charge density wave. Further studies of the phase diagram at high temperatures, where controlled oxygen atmospheres are required, reveal an unusual reentrant formation of a potassium-containing impurity phase which explains the need for synthesis techniques that involve initially reacting in a reducing atmosphere, followed by oxygenation at lower temperature.
Single‐phase samples of (Ba1‐xKx)(Bi1‐xSby)O3 have been synthesized over a limited compositional range using a two‐step procedure: high‐temperature firing in a low oxygen partial pressure followed by low‐temperature oxygen annealing. For y=0 and 0.37<x<0.50, samples have a simple cubic structure and are bulk superconductors with Tc gradually decreasing from 30 to 22K as x increases to 0.50. For fixed x and y>0 samples are superconducting again with a simple cubic structure and with Tc gradually decreasing as y increases.
Atomic pair distribution function analysis has demonstrated displacements of Tl and O atoms within the Tl-O layers with shortrange ordering of lower symmetry than the crystallographic lattice. Two models have been proposed for these displacements. Rietveld analysis neither confirms nor contradicts these models. Temperature-dependent PDF measurements show changes in local structure correlating with temperature.
The phonon densities-of-states (DOS) of superconducting Ba 1−x K x Bi ¹⁶ O 3 and Ba 1−x K x Bi ¹⁸ O 3 (x=0.4) are determined using molecular dynamics (MD) simulations and inelastic neutron scattering measurements. The reference isotope-effect exponent is obtained from the mass variation of the first frequency moment of the phonon DOS. The energy gap, oxygen isotope-effect exponent and electron tunneling characteristics are calculated within the framework of Eliashberg theory of electron-phonon coupling.
Citations (57)
... These topics have been most heavily investigated in theory and experiment in structures based on square lattices in the cuprates [4,13] and Fe superconductors [3,14,15]. Correlated metals with hexagonal/triangular symmetry are much less common, with the best-known example being the triangular lattice cobaltates [16,17], which however are complicated by Na vacancy ordering and water intercalation [18]. ...
... It is known that the character of the magnetic exchange interactions in systems with a perovskite structure containing manganese ions is determined by the magnitude of the [13,14]. Thus, the magnetic properties of manganites containing predominantly trivalent manganese ions can be explained within the model of superexchange interactions, assuming the type and magnitude of exchange interactions to be determined by the nature of the chemical bonds Mn-O. ...
... The superconducting transition was confirmed by the measurements of the magnetic moment in zero-field cooling (ZFC) and field-cooling (FC) modes, which show diamagnetic throws at ~ 31 K (Fig.1f). These results are in accordance with the results reported previously [35][36][37][38] . ...
... etc., the catalytic activity of pure SCO was rarely reported [12][13][14]. Until 2013, Lee et al. firstly unveiled a dramatically enhanced the oxygen reduction catalytic activity in BM-SCO films by controlling the crystallographic orientation of one-dimensional oxygen vacancy channels in the brownmillerite lattice and found SCO film exhibits significant activity for the carbon monoxide oxidation reaction [3,4,15]. In 2016, Stevenson et al. [16] proved SrCoO 2.7 is a high, room temperature-specific activity and mass activity toward water electrolysis. ...
... Nitrides have an additional advantage that the discharge product i.e. Li 3 N is an excellent ionic conductor [138], which provides additional conductivity during electrochemical cycling. Transition metal nitrides having general formula of Li 3-x M x N (M= V, Cr, Fe, Co, Ni, Cu, Zn) [139][140][141][142][143][144][145] have been visualized as conversion anode in the literature. ...
... An increase in temperature leads to an increase in the tolerance factor in many systems. 93 For manganates with Sr 2+ , Ca 2+ , or Ba 2+ on the A site, as a rule of thumb according to Fig. 6 in a publication by Dabrowski et al., one can state that the tolerance factor increases by approx. 0.002 at 800 K, by 0.010 at 1000 K, and by 0.020 at 1300 K (all with respect to the calculated tolerance factor at 0 K). ...
... If the size of initial FM domains is too small, it is hard for the FM clusters to be merged with neighboring FM domains, then no EB effect can be observed. The magnetic state of the parent compound La 0.5 Sr 0.5 MnO 3 exhibits FM ground state with AFM clusters in low-temperature region 30,31 . Upon Co doping, the double exchange interaction between Mn 3+ and Mn 4+ would be partially destroyed and some of the FM ground state would be transformed to a robust AFM state 32,33 . ...
... The examinations of compressibility for C 60 using He, Ne and Ar as pressure media and the study of diffusion kinetics in solid C 60 have been carried out under the conditions of high pressure at around several kbar [6][7][8][9]. In these, the chemical interactions have not been discussed. ...
... Quelquesétudes ontété effectuées dans ce sens dans les oxydes, notamment la famille des oxydes de vanadium (vanadates) [Lüscher et al., 2004;Gavilano et al., 2005], ou encore le composé La 4 Cu 3 MoO 12 [VanderGriend et al., 1999], appartenant a la même série (Ln n Cu n−1 M n+2 O 3n ) que le composé La 3 Cu 2 VO 9 faisant l'objet de ce chapitre. Cesétudes, utilisant une grande variété de techniques expérimentales (magnétomètrie, chaleur spécifique, diffusion neutronique, ...), sont souvent agrémentées de modèles théoriques, avec comme volonté de décrire les différenteséchelles d'énergie de ces systèmes [Wang, 2001]. ...
... In the figure there are also denoted compositional ranges which will be discussed in the following sections: RMnO 3 , Sr 1−x Ca x MnO 3 , La 0.5 Sr 0.5−y Ba y Mn 3.5+ O 3 , and RBaMn 2 O 6 . While the randomly-substituted Sr 1−x Ca x MnO 3 and La 0.5 Sr 0.5−y Ba y MnO 3 compounds could be relatively easily obtained in Ar, the synthesis of a well layered-ordered RBaMn 2 O 6 compounds required accurate control of the oxygen content near O 5 at high temperatures by using in situ thermogravimetric analysis (TGA) apparatus with H 2 /Ar flow [4,10,13]. ...