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At least 91 records · Page 5

Compositional redistribution during casting of Hg sub 0.8 Cd sub 0.2 Te alloys

A series of Hg(0.8)Cd(0.2)Te ingots was cast both vertically and horizontally under well-defined thermal conditions by using a two-zone furnace with isothermal heat-pipe liners. The main objective of the experiments was to establish correlations between casting parameters and compositional redistribution and to develop ground-based data for a proposed flight experiment of casting of Hg(1-x)Cd(x)Te alloys under reduced gravity conditions. The compositional variations along the axial and radial directions were determined by precision density measurements, infrared transmission spectra, and X-ray energy dispersion spectrometry. Comparison between the experimental results and a numerical simulation of the solidification process of Hg(0.8)Cd(0.2)Te is described.

Su, Ching-Hua↗

Compositional redistribution during casting of Hg(0.8)Cd(0.2)Te alloys

A series of Hg(0.8)Cd(0.2)Te ingots was cast both vertically and horizontally under well-defined thermal conditions by using a two-zone furnace with isothermal heat-pipe liners. The main objective of the experiments was to establish correlations between casting parameters and compositional redistribution and to develop ground-based data for a proposed flight experiment of casting of Hg(1-x)Cd(x)Te alloys under reduced gravity conditions. The compositional variations along the axial and radial directions were determined by precision density measurements, infrared transmission spectra, and X-ray energy dispersion spectrometry. Comparison between the experimental results and a numerical simulation of the solidification process of Hg(0.8)Cd(0.2)Te is described.

Su, Ching-Hua↗

A study of the influence of Hg(6(3)P2) population in a low-pressure discharge on mercury ion emission at 194.2 nm

A low-pressure mercury-argon discharge, similar to the type existing in the mercury lamp for the trapped-ion standard, is probed with a new technique of laser spectroscopy to determine the influence of the Hg(6 3P(sub 2)) population on discharge emission. The discharge is excited with inductively coupled rf power. Variations in the intensity of emission lines in the discharge were examined as lambda = 546.1 nm light from a continuous wave (CW) laser excited the Hg(6 3P(sub 2)) to (7 3S (sub 1)) transition. The spectrum of the discharge viewed in the region of laser irradiation showed increased emission in lambda = 546.1, 435.8, 404.7, 253.7, and 194.2 nm lines. Other lines in Hg I exhibited a decrease in emission. When the discharge was viewed outside the region of laser irradiation, all lines exhibited an increased emission. Based on these results, it is concluded that the dominant mechanism for the excitation of higher lying levels of mercury is the the electron-impact excitation via the 3P(sub 2) level. The depopulation of this metastable is also responsible for the observed increase in the electron temperature when the laser irradiates the discharge. It is also concluded that the 3P(sub 2) metastable level of mercury does not play a significant role in the excitation of the 3P(sub 1/2) level of mercury ion.

Maleki, L.↗

Directional Solidification and Characterization of Hg(0.89) Mn(0.11)Te

Two boules of Hg(0.89)Mn(0.11)Te(MMT) were solidified using the vertical Bridgman-Stockbarger method. Translation rates of 0.09 and 0. 18 microns/s were used. The influence of growth rate on axial compositional homogeneity in the MMT boules was evaluated experimentally by conducting precision density measurements on radial slices taken from each boule. In addition, Plane Front Solidification theory and segregation coefficient (k) data for the Hg(1-x)Mn(x)Te system were used to fit theoretical composition profiles to the measured MMT axial composition profiles. The strong correlation between the measured and calculated MMT axial composition profiles indicates diffusion dominated axial solute redistribution in the boules under the applied growth conditions. The analysis of the MMT axial composition profiles by Plane Front Solidification theory allowed the calculation of the effective diffusion coefficient (D(eff) = 3.5 x l0(exp -5) sq cm/s). The k-values for the Hg(1-x)Mn(x)Te system and the D(sub eff) - value were then used to verify that both boules were solidified under conditions which did not exceed the Constitutional Supercooling Criteria under ideal conditions. Finally, a preliminary examination of the radial compositional variation in each MMT was made using Fourier Transform Infra-Red Spectroscopy (FTIR). The radial homogeneity in the MMT boules was found to be comparable for both translation rates.

Price, M. W.↗

Density, Electrical Conductivity and Viscosity of Hg(sub 0.8)Cd(sub 0.2)Te Melt

The density, viscosity, and electrical conductivity of Hg(sub 0.8)Cd(sub 0.2)Te melt were measures as a function of temperature. A pycnometric method was used to measure the melt density in the temperature range of 1072 to 1122 K. The viscosity and electrical conductivity were determined using a transient torque method from 1068 to 1132 K. The density result from this study is within 0.3% of the published data. However, the current viscosity result is approximately 30% lower than the existing data. The electrical conductivity of Hg(sub 0.8)Cd(sub 0.2)Te melt as a function of temperature, which is not available in the literature, is also determined. The analysis of the temperature dependent electrical conductivity and the relationship between the kinematic viscosity and density indicated that the structure of the melt appeared to be homogeneous when the temperature was above 1090 K. A structural transition occurred in the Hg(sub 0.8)Cd(sub 0.2)Te melt as the temperature was decreased to below 1090 K.

Li, C.↗

Density, Electrical Conductivity and Viscosity of Hg(0.8)Cd(0.2)Te Melt

The density, viscosity, and electrical conductivity of Hg(0.8)Cd(0.2)Te melt were measured as a function of temperature. A pycnometric method was used to measure the melt density in the temperature range of 1072 to 1122 K. The viscosity and electrical conductivity were determined using a transient torque method from 1068 to 1132 K. The density result from this study is within 0.3% of the published data. However, the current viscosity result is approximately 30% lower than the existing data. The electrical conductivity of Hg(0.8)Cd(0.2)Te melt as a function of temperature, which is not available in the literature, is also determined. The analysis of the temperature dependent electrical conductivity and the relationship between the kinematic viscosity and density indicated that the structure of the melt appeared to be homogeneous when the temperature was above 1090 K. A structural transition occurred in the Hg(0.8)Cd(0.2)Te melt as the temperature was decreased to below 1090 K

Li, C.↗

Thermophysical Properties and Structural Transition of Hg(0.8)Cd(0.2)Te Melt

Thermophysical properties, namely, density, viscosity, and electrical conductivity of Hg(sub o.8)Cd(sub 0.2)Te melt were measured as a function of temperature. A pycnometric method was used to measure the melt density in the temperature range of 1072 to 1122 K. The viscosity and electrical conductivity were simultaneously determined using a transient torque method from 1068 to 1132 K. The density result from this study is within 0.3% of the published data. However, the current viscosity result is approximately 30% lower than the existing data. The electrical conductivity of Hg(sub o.8)Cd(sub 0.2)Te melt as a function of temperature, which is not available in the literature, is also determined. The analysis of the temperature dependent electrical conductivity and the relationship between the kinematic viscosity and density indicated that the structure of the melt appeared to be homogeneous when the temperature was above 1090 K. A structural transition occurred in the Hg(sub 0.8)Cd(0.2)Te melt as the temperature was decreased from 1090 K to the liquidus temperature.

Li, C.↗

Materials Data on Hg(PO3)2 by Materials Project

Hg(PO3)2 crystallizes in the orthorhombic Pbca space group. The structure is three-dimensional. Hg2+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Hg–O bond distances ranging from 2.23–2.63 Å. There are two inequivalent P5+ sites. In the first P5+ site, P5+ is bonded to four O2- atoms to form corner-sharing PO4 tetrahedra. There are a spread of P–O bond distances ranging from 1.50–1.61 Å. In the second P5+ site, P5+ is bonded to four O2- atoms to form corner-sharing PO4 tetrahedra. There are a spread of P–O bond distances ranging from 1.50–1.62 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a bent 150 degrees geometry to two P5+ atoms. In the second O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Hg2+ and one P5+ atom. In the third O2- site, O2- is bonded in a 1-coordinate geometry to two equivalent Hg2+ and one P5+ atom. In the fourth O2- site, O2- is bonded in a 1-coordinate geometry to one Hg2+ and one P5+ atom. In the fifth O2- site, O2- is bonded in a bent 120 degrees geometry to two P5+ atoms. In the sixth O2- site, O2- is bonded in a distorted single-bond geometry to two equivalent Hg2+ and one P5+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Hg(IO3)2 by Materials Project

Hg(IO3)2 crystallizes in the monoclinic P2_1 space group. The structure is three-dimensional. Hg2+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Hg–O bond distances ranging from 2.25–2.97 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted single-bond geometry to one Hg2+ and two I5+ atoms. There are one shorter (1.84 Å) and one longer (2.60 Å) O–I bond lengths. In the second O2- site, O2- is bonded in a distorted single-bond geometry to two equivalent Hg2+ and two equivalent I5+ atoms. There are one shorter (1.83 Å) and one longer (2.71 Å) O–I bond lengths. In the third O2- site, O2- is bonded in a 2-coordinate geometry to one Hg2+ and two I5+ atoms. There are one shorter (1.86 Å) and one longer (2.79 Å) O–I bond lengths. In the fourth O2- site, O2- is bonded in a 1-coordinate geometry to one Hg2+ and two equivalent I5+ atoms. There are one shorter (1.84 Å) and one longer (2.66 Å) O–I bond lengths. In the fifth O2- site, O2- is bonded in a distorted trigonal planar geometry to two equivalent Hg2+ and one I5+ atom. The O–I bond length is 1.88 Å. In the sixth O2- site, O2- is bonded in a 2-coordinate geometry to one Hg2+ and two I5+ atoms. There are one shorter (1.86 Å) and one longer (2.64 Å) O–I bond lengths. There are two inequivalent I5+ sites. In the first I5+ site, I5+ is bonded to six O2- atoms to form distorted corner-sharing IO6 octahedra. The corner-sharing octahedral tilt angles are 48°. In the second I5+ site, I5+ is bonded in a 5-coordinate geometry to five O2- atoms.

36 MATERIALS SCIENCE↗

Materials Data on Hg(Mo3Cl7)2 by Materials Project

Hg(Mo3Cl7)2 crystallizes in the cubic Pn-3 space group. The structure is three-dimensional. Mo2+ is bonded to five Cl1- atoms to form MoCl5 square pyramids that share a cornercorner with one HgCl6 octahedra and edges with four equivalent MoCl5 square pyramids. The corner-sharing octahedral tilt angles are 48°. There are three shorter (2.48 Å) and two longer (2.49 Å) Mo–Cl bond lengths. Hg2+ is bonded to six equivalent Cl1- atoms to form HgCl6 octahedra that share corners with six equivalent MoCl5 square pyramids. All Hg–Cl bond lengths are 2.74 Å. There are three inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a 12-coordinate geometry to three equivalent Mo2+ atoms. In the second Cl1- site, Cl1- is bonded in a distorted bent 120 degrees geometry to one Mo2+ and one Hg2+ atom. In the third Cl1- site, Cl1- is bonded in a 3-coordinate geometry to three equivalent Mo2+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Hg(AuF4)2 by Materials Project

Hg(AuF4)2 crystallizes in the tetragonal P4/mcc space group. The structure is three-dimensional. Au3+ is bonded in a square co-planar geometry to four equivalent F1- atoms. All Au–F bond lengths are 1.97 Å. Hg2+ is bonded in a 8-coordinate geometry to eight equivalent F1- atoms. All Hg–F bond lengths are 2.43 Å. F1- is bonded in a distorted bent 120 degrees geometry to one Au3+ and one Hg2+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Hg(AsO3)2 by Materials Project

Hg(AsO3)2 crystallizes in the trigonal P-31m space group. The structure is three-dimensional. Hg2+ is bonded to six equivalent O2- atoms to form HgO6 octahedra that share corners with twelve equivalent AsO6 octahedra. The corner-sharing octahedral tilt angles are 53°. All Hg–O bond lengths are 2.41 Å. As5+ is bonded to six equivalent O2- atoms to form AsO6 octahedra that share corners with six equivalent HgO6 octahedra and edges with three equivalent AsO6 octahedra. The corner-sharing octahedral tilt angles are 53°. All As–O bond lengths are 1.87 Å. O2- is bonded in a distorted trigonal planar geometry to one Hg2+ and two equivalent As5+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Hg(CO2)2 by Materials Project

Hg(CO2)2 crystallizes in the monoclinic P2_1 space group. The structure is zero-dimensional and consists of two mercuric formate molecules. Hg2+ is bonded in a distorted linear geometry to two O2- atoms. Both Hg–O bond lengths are 2.13 Å. There are two inequivalent C3+ sites. In the first C3+ site, C3+ is bonded in a bent 120 degrees geometry to two O2- atoms. There is one shorter (1.24 Å) and one longer (1.30 Å) C–O bond length. In the second C3+ site, C3+ is bonded in a bent 120 degrees geometry to two O2- atoms. There is one shorter (1.24 Å) and one longer (1.30 Å) C–O bond length. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a single-bond geometry to one C3+ atom. In the second O2- site, O2- is bonded in a single-bond geometry to one C3+ atom. In the third O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Hg2+ and one C3+ atom. In the fourth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Hg2+ and one C3+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Hg(BiS2)2 by Materials Project

HgBi2S4 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are two inequivalent Hg2+ sites. In the first Hg2+ site, Hg2+ is bonded to six S2- atoms to form distorted HgS6 octahedra that share corners with two equivalent BiS6 octahedra, corners with four equivalent BiS7 square pyramids, edges with two equivalent HgS6 octahedra, and edges with six equivalent BiS7 square pyramids. The corner-sharing octahedral tilt angles are 66°. There are two shorter (2.40 Å) and four longer (3.24 Å) Hg–S bond lengths. In the second Hg2+ site, Hg2+ is bonded to six S2- atoms to form distorted HgS6 octahedra that share corners with four equivalent BiS6 octahedra, corners with four equivalent BiS7 square pyramids, edges with two equivalent HgS6 octahedra, and edges with six equivalent BiS6 octahedra. The corner-sharing octahedral tilt angles are 8°. There are two shorter (2.39 Å) and four longer (3.27 Å) Hg–S bond lengths. There are two inequivalent Bi3+ sites. In the first Bi3+ site, Bi3+ is bonded to six S2- atoms to form BiS6 octahedra that share corners with three HgS6 octahedra, corners with four equivalent BiS7 square pyramids, edges with three equivalent HgS6 octahedra, edges with four equivalent BiS6 octahedra, and an edgeedge with one BiS7 square pyramid. The corner-sharing octahedra tilt angles range from 8–66°. There are a spread of Bi–S bond distances ranging from 2.65–3.17 Å. In the second Bi3+ site, Bi3+ is bonded to seven S2- atoms to form distorted BiS7 square pyramids that share corners with four HgS6 octahedra, corners with four equivalent BiS6 octahedra, an edgeedge with one BiS6 octahedra, edges with three equivalent HgS6 octahedra, edges with two equivalent BiS7 square pyramids, and faces with two equivalent BiS7 square pyramids. The corner-sharing octahedra tilt angles range from 9–64°. There are a spread of Bi–S bond distances ranging from 2.62–3.48 Å. There are four inequivalent S2- sites. In the first S2- site, S2- is bonded in a 1-coordinate geometry to one Hg2+ and four Bi3+ atoms. In the second S2- site, S2- is bonded in a 5-coordinate geometry to two equivalent Hg2+ and three equivalent Bi3+ atoms. In the third S2- site, S2- is bonded to one Hg2+ and three Bi3+ atoms to form distorted SHgBi3 tetrahedra that share corners with three equivalent SHg2Bi3 square pyramids and corners with three equivalent SHgBi3 tetrahedra. In the fourth S2- site, S2- is bonded to two equivalent Hg2+ and three equivalent Bi3+ atoms to form distorted SHg2Bi3 square pyramids that share corners with two equivalent SHg2Bi3 square pyramids, corners with three equivalent SHgBi3 tetrahedra, and edges with five equivalent SHg2Bi3 square pyramids.

36 MATERIALS SCIENCE↗

Materials Data on Hg(SbO3)2 by Materials Project

Hg(SbO3)2 is zeta iron carbide-derived structured and crystallizes in the trigonal P-31m space group. The structure is three-dimensional. Hg2+ is bonded to six equivalent O2- atoms to form HgO6 octahedra that share corners with twelve equivalent SbO6 octahedra. The corner-sharing octahedral tilt angles are 53°. All Hg–O bond lengths are 2.44 Å. Sb5+ is bonded to six equivalent O2- atoms to form SbO6 octahedra that share corners with six equivalent HgO6 octahedra and edges with three equivalent SbO6 octahedra. The corner-sharing octahedral tilt angles are 53°. All Sb–O bond lengths are 2.02 Å. O2- is bonded in a distorted trigonal planar geometry to one Hg2+ and two equivalent Sb5+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Hg(BiO3)2 by Materials Project

Hg(BiO3)2 is Hydrophilite-derived structured and crystallizes in the tetragonal P4_2/mnm space group. The structure is three-dimensional. Hg2+ is bonded to six O2- atoms to form HgO6 octahedra that share corners with eight equivalent BiO6 octahedra and edges with two equivalent BiO6 octahedra. The corner-sharing octahedra tilt angles range from 53–54°. There are two shorter (2.27 Å) and four longer (2.34 Å) Hg–O bond lengths. Bi5+ is bonded to six O2- atoms to form BiO6 octahedra that share corners with four equivalent HgO6 octahedra, corners with four equivalent BiO6 octahedra, an edgeedge with one HgO6 octahedra, and an edgeedge with one BiO6 octahedra. The corner-sharing octahedra tilt angles range from 47–54°. There are a spread of Bi–O bond distances ranging from 2.16–2.21 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a trigonal planar geometry to one Hg2+ and two equivalent Bi5+ atoms. In the second O2- site, O2- is bonded in a distorted trigonal planar geometry to one Hg2+ and two equivalent Bi5+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Hg(SbO3)2 by Materials Project

Hg(SbO3)2 is zeta iron carbide-derived structured and crystallizes in the tetragonal P4_2/mnm space group. The structure is three-dimensional. Hg2+ is bonded to six O2- atoms to form HgO6 octahedra that share corners with eight equivalent SbO6 octahedra and edges with two equivalent SbO6 octahedra. The corner-sharing octahedra tilt angles range from 54–57°. There are two shorter (2.27 Å) and four longer (2.35 Å) Hg–O bond lengths. Sb5+ is bonded to six O2- atoms to form SbO6 octahedra that share corners with four equivalent HgO6 octahedra, corners with four equivalent SbO6 octahedra, an edgeedge with one HgO6 octahedra, and an edgeedge with one SbO6 octahedra. The corner-sharing octahedra tilt angles range from 39–57°. There are four shorter (2.03 Å) and two longer (2.05 Å) Sb–O bond lengths. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a trigonal planar geometry to one Hg2+ and two equivalent Sb5+ atoms. In the second O2- site, O2- is bonded in a 3-coordinate geometry to one Hg2+ and two equivalent Sb5+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Hg(TeO3)2 by Materials Project

Hg(TeO3)2 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. Hg2+ is bonded in a 5-coordinate geometry to five O2- atoms. There are a spread of Hg–O bond distances ranging from 2.25–2.55 Å. There are two inequivalent Te5+ sites. In the first Te5+ site, Te5+ is bonded to five O2- atoms to form a mixture of edge and corner-sharing TeO5 trigonal bipyramids. There are a spread of Te–O bond distances ranging from 1.87–2.05 Å. In the second Te5+ site, Te5+ is bonded to five O2- atoms to form a mixture of distorted edge and corner-sharing TeO5 square pyramids. There are a spread of Te–O bond distances ranging from 1.85–2.53 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a 3-coordinate geometry to one Hg2+ and two Te5+ atoms. In the second O2- site, O2- is bonded in a water-like geometry to one Hg2+ and one Te5+ atom. In the third O2- site, O2- is bonded in a distorted trigonal planar geometry to one Hg2+ and two Te5+ atoms. In the fourth O2- site, O2- is bonded in a 3-coordinate geometry to one Hg2+ and two Te5+ atoms. In the fifth O2- site, O2- is bonded in a bent 150 degrees geometry to one Hg2+ and one Te5+ atom. In the sixth O2- site, O2- is bonded in a bent 150 degrees geometry to two Te5+ atoms.

36 MATERIALS SCIENCE↗