108,652 research outputs found
Evans, J D, 406196
No full textThis record was harvested from a previous catalogue system and will be withdrawn in 2025. Information in this record may be superseded or incomplete. Visit this record in UMA's new catalogue at: https://archives.library.unimelb.edu.au/nodes/view/384158Surname: EVANS. Given Name(s) or Initials: J D. Military Service Number or Last Known Location: 406196. Missing, Wounded and Prisoner of War Enquiry Card Index Number: 45377.228780
Item: [2016.0049.16451] "Evans, J D, 406196
Letter from G. N. D. Evans, December 4, 1967
No full textLetter from G. N. D. Evans to Fayez Sayegh, December 4, 1967, regarding his appearance on the David Susskind show and the Arab-Israeli conflict
Dr. D. J. Evans
No full textDr. D. J. Evans, a Baptist minister from Atlanta, GA, speaks in a Furman classroom during the annual Religious Emphasis Week
Sheet 5-D, Job 3-J
No full textInk-on-linen drawing for typical northwest quarter plan for apartment building [Belvedere Apts.], Social Hall Ave. and State St., Salt Lake City, by Miller, Woolley & Evans, March 27, 1919. Created for the Church of Jesus Christ of Latter-day Saints43
Sheet 2-D, Job 3-J
No full textInk-on-linen drawing of the northwest quarter ground floor plan for apartment building [Belvedere Apts.], Social Hall Ave. and State St., Salt Lake City, by Miller, Woolley & Evans, Architects, January 6, 1919. Created for the Church of Jesus Christ of Latter-day Saints34
Evidence for the decay B0→J/ψω and measurement of the relative branching fractions of meson decays to J/ψη and J/ψη′
No full textFirst evidence of the B 0 → J / ψ ω decay is found and the B s 0 → J / ψ η and B s 0 → J / ψ η ′ decays are studied using a dataset corresponding to an integrated luminosity of 1.0 fb -1 collected by the LHCb experiment in proton-proton collisions at a centre-of-mass energy of sqrt(s) = 7 TeV. The branching fractions of these decays are measured relative to that of the B 0 → J / ψ ρ 0 decay:frac(B (B 0 → J / ψ ω), B (B 0 → J / ψ ρ 0)) = 0.89 ± 0.19 (stat) - 0.13 + 0.07 (syst),frac(B (B s 0 → J / ψ η), B (B 0 → J / ψ ρ 0)) = 14.0 ± 1.2 (stat) - 1.5 + 1.1 (syst) - 1.0 + 1.1 (frac(f d, f s)),frac(B (B s 0 → J / ψ η ′), B (B 0 → J / ψ ρ 0)) = 12.7 ± 1.1 (stat) - 1.3 + 0.5 (syst) - 0.9 + 1.0 (frac(f d, f s)), where the last uncertainty is due to the knowledge of f d / f s, the ratio of b-quark hadronization factors that accounts for the different production rate of B 0 and B s 0 mesons. The ratio of the branching fractions of B s 0 → J / ψ η ′ and B s 0 → J / ψ η decays is measured to befrac(B (B s 0 → J / ψ η ′), B (B s 0 → J / ψ η)) = 0.90 ± 0.09 (stat) - 0.02 + 0.06 (syst)
Glyn Daniel et J. D. Evans, The Western Mediterranean
No full textDelvoye Charles. Glyn Daniel et J. D. Evans, The Western Mediterranean. In: L'antiquité classique, Tome 36, fasc. 1, 1967. p. 370
Glyn Daniel et J. D. Evans, The Western Mediterranean
No full textDelvoye Charles. Glyn Daniel et J. D. Evans, The Western Mediterranean. In: L'antiquité classique, Tome 36, fasc. 1, 1967. p. 370
Alva J. Niles Collection
No full textPhotograph of Brig. General Alva J. Niles, Lt. Col. Charles W. Vanway, US Army, and UNIDENTIFIED, Portland, OR. Photo by D. Perry Evans, Portland, OR, October 1928
Solvent-modified dynamic porosity in chiral 3D kagome frameworks
No full textExtent: 9p.Dynamically porous metal-organic frameworks (MOFs) with a chiral quartz-based structure have been synthesized from the multidentate ligand 2,2'-dihydroxybiphenyl-4,4'-dicarboxylate (H2diol). Compounds [Ni(II)(H2diol)(S)2]·xS (where S = DMF or DEF) show marked changes in 77 K N2 uptake between partially desolvated [Ni(II)(H2diol)(S)2] (only the pore solvent is removed) and fully desolvated [Ni(II)(H2diol)] forms. Furthermore, [Ni(II)(H2diol)(DMF)2] displays additional solvent-dependent porosity through the rotation of DMF molecules attached to the axial coordination sites of the Ni(II) centre. A unique feature of the four coordinate Ni(II) centre in [Ni(II)(H2diol)] is the dynamic response to its chemical environment. Exposure of [Ni(II)(H2diol)] to H2O and MeOH vapour leads to coordination of both axial sites of the Ni centres and to the generation of a solvated framework, whereas exposure to EtOH, DMF, acetone, and MeCN does not lead to any change in metal coordination or structure metrics. MeOH vapour adsorption was able to be tracked by time-dependent magnetometry as the solvated and desolvated structures have different magnetic moments. Solvated and desolvated forms of the MOF show remarkable differences in their thermal expansivities; [Ni(II)(H2diol)(DMF)2]·DMF displays marked positive thermal expansion (PTE) in the c-axis, yet near to zero thermal expansion, between 90 and 450 K, is observed for [Ni(II)(H2diol)]. These new MOF architectures demonstrate a dynamic structural and colourimetric response to selected adsorbates via a unique mechanism that involves a reversible change in the coordination environment of the metal centre. These coordination changes are mediated throughout the MOF by rotational mobility about the biaryl bond of the ligand.Tony D. Keene, Damien Rankine, Jack D. Evans, Peter D. Southon, Cameron J. Kepert, Jade B. Aitken, Christopher J. Sumby and Christian J. Doona
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