Search Results - (Author, Cooperation:R. Hazen)
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1B. Bolukbasi ; N. Berente ; J. Cutcher-Gershenfeld ; L. Dechurch ; C. Flint ; M. Haberman ; J. L. King ; E. Knight ; B. Lawrence ; E. Masella ; C. McElroy ; B. Mittleman ; M. Nolan ; M. Radik ; N. Shin ; C. A. Thompson ; S. Winter ; I. Zaslavsky ; M. L. Allison ; D. Arctur ; J. Arrigo ; A. K. Aufdenkampe ; J. Bass ; J. Crowell ; M. Daniels ; S. Diggs ; C. Duffy ; Y. Gil ; B. Gomez ; S. Graves ; R. Hazen ; L. Hsu ; D. Kinkade ; K. Lehnert ; C. Marone ; D. Middleton ; A. Noren ; G. Pearthree ; M. Ramamurthy ; E. Robinson ; G. Percivall ; S. Richard ; C. Suarez ; D. Walker
American Association for the Advancement of Science (AAAS)
Published 2013Staff ViewPublication Date: 2013-11-30Publisher: American Association for the Advancement of Science (AAAS)Print ISSN: 0036-8075Electronic ISSN: 1095-9203Topics: BiologyChemistry and PharmacologyComputer ScienceMedicineNatural Sciences in GeneralPhysicsKeywords: *Access to Information ; Periodicals as Topic/*economics ; Research/*economicsPublished by: -
2Bristow, T. F., Rampe, E. B., Achilles, C. N., Blake, D. F., Chipera, S. J., Craig, P., Crisp, J. A., Des Marais, D. J., Downs, R. T., Gellert, R., Grotzinger, J. P., Gupta, S., Hazen, R. M., Horgan, B., Hogancamp, J. V., Mangold, N., Mahaffy, P. R., McAdam, A. C., Ming, D. W., Morookian, J. M., Morris, R. V., Morrison, S. M., Treiman, A. H., Vaniman, D. T., Vasavada, A. R., Yen, A. S.
American Association for the Advancement of Science (AAAS)
Published 2018Staff ViewPublication Date: 2018-06-07Publisher: American Association for the Advancement of Science (AAAS)Electronic ISSN: 2375-2548Topics: Natural Sciences in GeneralPublished by: -
3Staff View
ISSN: 1089-7550Source: AIP Digital ArchiveTopics: PhysicsNotes: The crystal structure of synthetic BeO, bromellite, has been determined at several pressures to 5.0 GPa and several temperatures to 1183 K. The single variable atomic-positional parameter, z of oxygen, does not vary significantly with pressure, but does undergo a small increase with temperature. The hexagonal axial ratio c/a is constant with pressure, but decreases slightly from 1.624±0.001 to 1.623±0.001 between 300 and 1183 K. The observed crystal bulk modulus is 212±3 GPa, if K' is assumed to be 4. The bulk modulus of the beryllium tetrahedron in BeO is 210 GPa, identical to that of the crystal, and close to the value observed for beryllium tetrahedra in other beryllium minerals. The average volume thermal expansivity of the BeO beryllium tetrahedron between 298 and 1183 K is 2.5±0.2×10−5 K−1, compared to 2.66±0.10×10−5 K−1 for the crystal.Type of Medium: Electronic ResourceURL: -
4Staff View
ISSN: 0006-291XSource: Elsevier Journal Backfiles on ScienceDirect 1907 - 2002Topics: BiologyChemistry and PharmacologyPhysicsType of Medium: Electronic ResourceURL: -
5Staff View
ISSN: 0304-4165Keywords: (Rat hemidiaphragm) ; Cyclic AMP ; Glycogen synthase ; Hormonal regulation ; Insulin ; Protein kinaseSource: Elsevier Journal Backfiles on ScienceDirect 1907 - 2002Topics: BiologyChemistry and PharmacologyMedicinePhysicsType of Medium: Electronic ResourceURL: -
6Angel, R. J. ; Gasparik, T. ; Ross, N. L. ; Finger, L. W. ; Prewitt, C. T. ; Hazen, R. M.
[s.l.] : Nature Publishing Group
Published 1988Staff ViewISSN: 1476-4687Source: Nature Archives 1869 - 2009Topics: BiologyChemistry and PharmacologyMedicineNatural Sciences in GeneralPhysicsNotes: [Auszug] The synthesis of Na(Mgo.5Si0.5) Si2O6 pyroxene and its unit-cell parameters based upon X-ray powder diffraction were reported by Gasparik2. Single crystals were synthesized from a stoichiometric mix of high-purity SiO2, MgO and Na2Si2O5 at 1,600°C and 150kbar using a split-sphere anvil ...Type of Medium: Electronic ResourceURL: -
7Finger, L. W. ; Ko, J. ; Hazen, R. M. ; Gasparik, T. ; Hemley, R. J. ; Prewitt, C. T. ; Weidner, D. J.
[s.l.] : Nature Publishing Group
Published 1989Staff ViewISSN: 1476-4687Source: Nature Archives 1869 - 2009Topics: BiologyChemistry and PharmacologyMedicineNatural Sciences in GeneralPhysicsNotes: [Auszug] FIG. 1 Raman spectra of phase B (top curve) and anhydrous phase B (bottom curve) measured with 457.9-nm laser excitation (-25 mW) and 5-crrT1 resolution. The peaks in the phase B spectrum, which arise from OH-stretching vibrations, appear at 3,414 and 3,356 cm"1, frequencies similar to those found4 ...Type of Medium: Electronic ResourceURL: -
8Veblen, D. R. ; Heaney, P. J. ; Angel, R. J. ; Finger, L. W. ; Hazen, R. M. ; Prewitt, C. T. ; Ross, N. L. ; Chu, C. W. ; Hor, P. H. ; Meng, R. L.
[s.l.] : Nature Publishing Group
Published 1988Staff ViewISSN: 1476-4687Source: Nature Archives 1869 - 2009Topics: BiologyChemistry and PharmacologyMedicineNatural Sciences in GeneralPhysicsNotes: [Auszug] The present observations are from samples BCSCO-a and BCSCO-b of Hazen et al.2. All selected-area electron diffraction microscopy (SAED), X-ray analytical electron microscopy (AEM), and high-resolution transmission electron microscopy (HRTEM) experiments were performed with a Philips 420 ...Type of Medium: Electronic ResourceURL: -
9Angel, R. J. ; Hazen, R. M. ; McCormick, T. C. ; Prewitt, C. T. ; Smyth, J. R.
Springer
Published 1988Staff ViewISSN: 1432-2021Source: Springer Online Journal Archives 1860-2000Topics: Chemistry and PharmacologyGeosciencesPhysicsNotes: Abstract The compressibilities of the three end-member feldspars have been determined between 1 bar and 50 kbar by single crystal X-ray diffraction techniques, using a Merrill-Bassett type diamond anvil cell with three crystals loaded simultaneously. Low albite (ordered aluminium-silicon distribution) and high sanidine (disordered Al-Si) show similar behaviour on compression, with bulk moduli (linear fit to volume-pressure data) of 0.70 and 0.67 Mbar respectively. The most compressible cell axis of all three feldspars studied is a, indicating that the major change in the feldspar framework with pressure is a shortening of the overall length of the “crankshaft chains” by reduction of T-O-T angles. Anorthite shows anomalous behaviour in that we have observed a previously unreported reversible phase transition at a pressure between 25.5 and 29.5 kbar. This transition is marked by large discontinuities in the unit cell angles and a small decrease of 0.2 percent in the cell volume with increasing pressure. The high-pressure phase is less compressible than the low-pressure phase, the bulk moduli being 0.94 and 1.06 Mbar respectively. There was no evidence of a monoclinic to triclinic inversion in sanidine that was expected to occur between 20 and 30 kbar on the basis of previous work on intermediate alkali feldspars.Type of Medium: Electronic ResourceURL: -
10Kudoh, Y. ; Finger, L. W. ; Hazen, R. M. ; Prewitt, C. T. ; Kanzaki, M. ; Veblen, D. R.
Springer
Published 1993Staff ViewISSN: 1432-2021Source: Springer Online Journal Archives 1860-2000Topics: Chemistry and PharmacologyGeosciencesPhysicsNotes: Abstract The unique cation-disordered crystal structures of two samples of phase E, a non-stoichiometric, hydrous silicate synthesized in a uniaxial, split-sphere, multi-anvil apparatus at conditions above 13 GPa and 1000° C, have been solved and refined in space group $$\bar 3$$ . The compositions and unit cells for the two materials, assuming six oxygens per cell, are Mg2.08Si1.16H3.20O6, a=2.9701(1) Å, c=13.882(1) Å V = 106.05(4) Å3 for sample 1, and Mg2.17Si1.01H3.62O6, a=2.9853(6) Å, c=13.9482(7) Å, V= 107.65(4) Å3 for sample 2. The structure contains layers with many features of brucite-type units, with the layers stacked in a rhombohedral arrangement. The layers are cross linked by silicon in tetrahedral coordination and magnesium in octahedral coordination, as well as hydrogen bonds. Interlay er octahedra share edges with intralayer octahedra. Interlayer tetrahedra would share faces with intralayer octahedra. To avoid this situation, there are vacancies within the layers. There is, however, no long-range order in the occupation of these sites, as indicated by the lack of a superstructure. Selected-area electron diffraction patterns show walls of diffuse intensity similar in geometry and magnitude to those observed in short-range-ordered alloys and Hågg phases. Phase E thus appears to represent a new class of disordered silicates, which may be thermodynamically metastable.Type of Medium: Electronic ResourceURL: -
11Staff View
ISSN: 1432-2021Source: Springer Online Journal Archives 1860-2000Topics: Chemistry and PharmacologyGeosciencesPhysicsNotes: Abstract Relative compressibilities of five silicate garnets were determined by single-crystal x-ray diffraction on crystals grouped in the same high-pressure mount. The specimens include a natural pyrope [(Mg2.84Fe0.10Ca0,06) Al2Si3O12], and four synthetic specimens with octahedrally-coordinated silicon: majorite [Mg3(MgSi)Si3O12], calcium-bearing majorite [(Ca0.49Mg2.51)(MgSi)Si3012], sodium majorite [(Na1.88Mgp0.12)(Mg0.06Si1.94)Si3O12], and an intermediate composition [(Na0.37Mg2.48)(Mg0.13Al1.07 Si080) Si3O12]. Small differences in the compressibilities of these crystals are revealed because they are subjected simultaneously to the same pressure. Bulk-moduli of the garnets range from 164.8 ± 2.3 GPa for calcium majorite to 191.5 ± 2.5 GPa for sodium majorite, assuming K′=4. Two factors, molar volume and octahedral cation valence, appear to control garnet compression.Type of Medium: Electronic ResourceURL: -
12Staff View
ISSN: 1432-2021Source: Springer Online Journal Archives 1860-2000Topics: Chemistry and PharmacologyGeosciencesPhysicsNotes: Abstract The unit-cell dimensions and crystal structure of sillimanite at various pressures up to 5.29 GPa have been refined from single-crystal X-ray diffraction data. As pressure increases, a and b decrease linearly, whereas c decreases nonlinearly with a slightly positive curvature. The axial compression ratios at room pressure are βa:βb:βc=1.22:1.63:1.00. Sillimanite exhibits the least compressibility along c, but the least thermal expansivity along a (Skinner et al. 1961; Winter and Ghose 1979). The bulk modulus of sillimanite is 171(1) GPa with K′=4 (3), larger than that of andalusite (151 GPa), but smaller than that of kyanite (193 GPa). The bulk moduli of the [Al1O6], [Al2O4], and [SiO4] polyhedra are 162(8), 269(33), and 367(89) GPa, respectively. Comparison of high-pressure data for Al2SiO5 polymorphs reveals that the [SiO4] tetrahedra are the most rigid units in all these polymorphic structures, whereas the [AlO6] octahedra are most compressible. Furthermore, [AlO6] octahedral compressibilities decrease from kyanite to sillimanite, to andalusite, the same order as their bulk moduli, suggesting that [AlO6] octahedra control the compression of the Al2SiO5 polymorphs. The compression of the [Al1O6] octahedron in sillimanite is anisotropic with the longest Al1-OD bond shortening by ∼1.9% between room pressure and 5.29 GPa and the shortest Al1-OB bond by only 0.3%. The compression anisotropy of sillimanite is primarily a consequence of its topological anisotropy, coupled with the compression anisotropy of the Al-O bonds within the [Al1O6] octahedron.Type of Medium: Electronic ResourceURL: