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At least 973 records · Page 54

Probing the local structure of Bi 2 O 3 chemical derivatives: the neglected cation sublattice

High-resolution synchrotron X-ray diffraction data confirm the stabilization of the average structure at ambient temperatures as a defect fluorite structure in ternary and quaternary oxides of Bi 2 O 3 , where some Bi cations are replaced with Dy 3+ and/or Er 3+ , Nb 5+ and W 6+ . Rietveld refinement of the diffraction data indicates that when the larger cation Er 3+ (0.89 Å) is replaced with smaller cations W 6+ (0.42 Å) and/or Nb 5+ (0.48 Å), the unit-cell parameter a, based on the relative ionic radii of the substituents, counterintuitively increases. Total scattering data show that the identity of the cation substituent is important in determining the positions of some Bi cations in the defect fluorite structure. Er 3+ and Dy 3+ cations induce monoclinic-like distortions that extend only locally in the Bi 3+ sublattice. X-ray absorption spectroscopy provides evidence that some Dy cations, in the δ phases, prefer to keep a similar local environment to that in the parent Dy 2 O 3 . W cations are found to be predominantly tetrahedrally coordinated in the δ phases explored in this work.

36 MATERIALS SCIENCE↗

Thermal Analysis of High Entropy Rare Earth Oxides

Phase transformations in multicomponent rare earth sesquioxides were studied by splat quenching from the melt, high temperature differential thermal analysis and synchrotron X-ray diffraction on laser-heated samples. Three compositions were prepared by the solution combustion method: (La,Sm,Dy,Er,RE) 2 O 3 , where all oxides are in equimolar ratios and RE is Nd or Gd or Y. After annealing at 800 °C, all powders contained mainly a phase of C-type bixbyite structure. After laser melting, all samples were quenched in a single-phase monoclinic B-type structure. Thermal analysis indicated three reversible phase transitions in the range 1900–2400 °C, assigned as transformations into A, H, and X rare earth sesquioxides structure types. Unit cell volumes and volume changes on C-B, B-A, and H-X transformations were measured by X-ray diffraction and consistent with the trend in pure rare earth sesquioxides. The formation of single-phase solid solutions was predicted by Calphad calculations. The melting point was determined for the (La,Sm,Dy,Er,Nd) 2 O 3 sample as 2456 ± 12 °C, which is higher than for any of constituent oxides. An increase in melting temperature is probably related to nonideal mixing in the solid and/or the melt and prompts future investigation of the liquidus surface in Sm 2 O 3 -Dy 2 O 3 , Sm 2 O 3 -Er 2 O 3 , and Dy 2 O 3 -Er 2 O 3 systems.

36 MATERIALS SCIENCE↗

A novel measurement of initial-state gluon radiation in hadron collisions using Drell-Yan events

A study of initial-state gluon radiation (ISR) in hadron collisions is presented using Drell-Yan (DY) events produced in proton-antiproton collisions by the Tevatron collider at a center-of-mass energy of 1.96 TeV. This paper adopts a novel approach which uses the mean value of the Z/$\gamma^*$ transverse momentum $ $ in DY events as a powerful observable to characterize the effect of ISR. In a data sample corresponding to an integrated luminosity of 9.4 fb$^{-1}$ collected with the CDF Run II detector, $ $ is measured as a function of the Z/$\gamma^*$ invariant mass. It is found that these two observables have a dependence, $ = -8 + 2.2 \ln m_{DY}^2$ [GeV/c], where $m_{DY}$ is the value of the Z/$\gamma^*$ mass measured in units of GeV/$c^2$. This linear dependence is observed for the first time in this analysis. It may be exploited to model the effect of ISR and constrain its impact in other processes.

72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS↗

Materials Data on DyTh by Materials Project

ThDy is Tetraauricupride structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Th is bonded in a body-centered cubic geometry to eight equivalent Dy atoms. All Th–Dy bond lengths are 3.47 Å. Dy is bonded in a body-centered cubic geometry to eight equivalent Th atoms.

36 MATERIALS SCIENCE↗

Materials Data on DyNi by Materials Project

DyNi crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Dy is bonded in a 7-coordinate geometry to seven equivalent Ni atoms. There are a spread of Dy–Ni bond distances ranging from 2.86–2.93 Å. Ni is bonded in a 9-coordinate geometry to seven equivalent Dy and two equivalent Ni atoms. Both Ni–Ni bond lengths are 2.55 Å.

36 MATERIALS SCIENCE↗

Materials Data on DyBPd3 by Materials Project

DyPd3B is (Cubic) Perovskite structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Dy is bonded to twelve equivalent Pd atoms to form DyPd12 cuboctahedra that share corners with twelve equivalent DyPd12 cuboctahedra, faces with six equivalent DyPd12 cuboctahedra, and faces with eight equivalent BPd6 octahedra. All Dy–Pd bond lengths are 3.05 Å. Pd is bonded to four equivalent Dy and two equivalent B atoms to form a mixture of distorted corner, edge, and face-sharing PdDy4B2 octahedra. The corner-sharing octahedra tilt angles range from 0–60°. Both Pd–B bond lengths are 2.16 Å. B is bonded to six equivalent Pd atoms to form BPd6 octahedra that share corners with six equivalent BPd6 octahedra and faces with eight equivalent DyPd12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°.

36 MATERIALS SCIENCE↗

Materials Data on DyAu by Materials Project

AuDy is Tetraauricupride structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Dy is bonded in a body-centered cubic geometry to eight equivalent Au atoms. All Dy–Au bond lengths are 3.12 Å. Au is bonded in a body-centered cubic geometry to eight equivalent Dy atoms.

36 MATERIALS SCIENCE↗

Materials Data on DyAu2 by Materials Project

Au2Dy crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Dy is bonded in a distorted q6 geometry to ten equivalent Au atoms. There are two shorter (3.04 Å) and eight longer (3.05 Å) Dy–Au bond lengths. Au is bonded in a 10-coordinate geometry to five equivalent Dy atoms.

36 MATERIALS SCIENCE↗

Materials Data on DyHg2 by Materials Project

DyHg2 crystallizes in the hexagonal P6/mmm space group. The structure is three-dimensional. Dy is bonded to twelve equivalent Hg atoms to form a mixture of distorted edge and face-sharing DyHg12 cuboctahedra. All Dy–Hg bond lengths are 3.34 Å. Hg is bonded in a 9-coordinate geometry to six equivalent Dy and three equivalent Hg atoms. All Hg–Hg bond lengths are 2.86 Å.

36 MATERIALS SCIENCE↗

Materials Data on DyTl by Materials Project

DyTl is Tetraauricupride structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Dy is bonded in a body-centered cubic geometry to eight equivalent Tl atoms. All Dy–Tl bond lengths are 3.29 Å. Tl is bonded in a body-centered cubic geometry to eight equivalent Dy atoms.

36 MATERIALS SCIENCE↗

Materials Data on DySi by Materials Project

DySi crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Dy is bonded in a 7-coordinate geometry to seven equivalent Si atoms. There are a spread of Dy–Si bond distances ranging from 2.95–3.16 Å. Si is bonded in a 9-coordinate geometry to seven equivalent Dy and two equivalent Si atoms. Both Si–Si bond lengths are 2.49 Å.

36 MATERIALS SCIENCE↗

Materials Data on DyAl by Materials Project

DyAl is Tetraauricupride structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Dy is bonded in a body-centered cubic geometry to eight equivalent Al atoms. All Dy–Al bond lengths are 3.12 Å. Al is bonded in a body-centered cubic geometry to eight equivalent Dy atoms.

36 MATERIALS SCIENCE↗

Materials Data on Dy2C by Materials Project

Dy2C is trigonal omega-like structured and crystallizes in the trigonal R-3m space group. The structure is two-dimensional and consists of three Dy2C sheets oriented in the (0, 0, 1) direction. Dy is bonded in a distorted T-shaped geometry to three equivalent C atoms. All Dy–C bond lengths are 2.47 Å. C is bonded to six equivalent Dy atoms to form edge-sharing CDy6 octahedra.

36 MATERIALS SCIENCE↗

Materials Data on DySi2 by Materials Project

DySi2 is hexagonal omega structure-like structured and crystallizes in the tetragonal I4_1/amd space group. The structure is three-dimensional. Dy is bonded to twelve equivalent Si atoms to form a mixture of edge and face-sharing DySi12 cuboctahedra. There are eight shorter (3.07 Å) and four longer (3.14 Å) Dy–Si bond lengths. Si is bonded in a 9-coordinate geometry to six equivalent Dy and three equivalent Si atoms. There are two shorter (2.34 Å) and one longer (2.40 Å) Si–Si bond lengths.

36 MATERIALS SCIENCE↗

Materials Data on Dy5Si3B by Materials Project

Dy5BSi3 crystallizes in the hexagonal P6_3/mcm space group. The structure is three-dimensional. there are two inequivalent Dy3+ sites. In the first Dy3+ site, Dy3+ is bonded in a 7-coordinate geometry to two equivalent B3- and five equivalent Si4- atoms. Both Dy–B bond lengths are 2.59 Å. There are a spread of Dy–Si bond distances ranging from 2.98–3.45 Å. In the second Dy3+ site, Dy3+ is bonded to six equivalent Si4- atoms to form a mixture of distorted corner, edge, and face-sharing DySi6 octahedra. The corner-sharing octahedral tilt angles are 33°. All Dy–Si bond lengths are 3.06 Å. B3- is bonded to six equivalent Dy3+ atoms to form face-sharing BDy6 octahedra. Si4- is bonded in a 9-coordinate geometry to nine Dy3+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on DyZnRh by Materials Project

DyRhZn crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Dy is bonded in a 5-coordinate geometry to five equivalent Rh atoms. There are three shorter (2.92 Å) and two longer (2.93 Å) Dy–Rh bond lengths. Rh is bonded in a 9-coordinate geometry to five equivalent Dy and four equivalent Zn atoms. There are a spread of Rh–Zn bond distances ranging from 2.64–2.70 Å. Zn is bonded in a 4-coordinate geometry to four equivalent Rh atoms.

36 MATERIALS SCIENCE↗

Materials Data on Dy2AlCo2 by Materials Project

Dy2Co2Al crystallizes in the orthorhombic Immm space group. The structure is three-dimensional. Dy is bonded in a 10-coordinate geometry to six equivalent Co atoms. There are four shorter (2.90 Å) and two longer (2.91 Å) Dy–Co bond lengths. Co is bonded in a 9-coordinate geometry to six equivalent Dy, one Co, and two equivalent Al atoms. The Co–Co bond length is 2.44 Å. Both Co–Al bond lengths are 2.52 Å. Al is bonded to four equivalent Co atoms to form distorted edge-sharing AlCo4 cuboctahedra.

36 MATERIALS SCIENCE↗

Materials Data on DyIr2 by Materials Project

DyIr2 is Cubic Laves structured and crystallizes in the cubic Fd-3m space group. The structure is three-dimensional. Dy is bonded in a 12-coordinate geometry to twelve equivalent Ir atoms. All Dy–Ir bond lengths are 3.14 Å. Ir is bonded to six equivalent Dy and six equivalent Ir atoms to form a mixture of edge, face, and corner-sharing IrDy6Ir6 cuboctahedra. All Ir–Ir bond lengths are 2.68 Å.

36 MATERIALS SCIENCE↗