106,835 research outputs found
Davison, A G, 423667
No full textThis record was harvested from a previous catalogue system and will be withdrawn in 2025. Information in this record may be superseded or incomplete.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/380947Surname: DAVISON. Given Name(s) or Initials: A G. Military Service Number or Last Known Location: 423667. Missing, Wounded and Prisoner of War Enquiry Card Index Number: 52551.195645
Item: [2016.0049.13240] "Davison, A G, 423667
Surface density of states in the many-neighbor approximation
No full textPT: J; CR: DAVISON SG, 1969, CHEM PHYS LETT, V3, P424 DAVISON SG, 1972, INT J QUANTUM CHEM, V6, P387 DAVISON SG, 1976, INT J QUANTUM CHEM, V10, P867 ECONOMOU EN, 1983, SOLID STATE SCI SER, V7 KALKSTEIN D, 1971, SURF SCI, V26, P85 LAVIS DA, UNPUB LAVIS DA, 1985, J PHYS C SOLID STATE, V18, P1387; NR: 7; TC: 4; J9: J PHYS CHEM; PG: 4; GA: A0336Source type: Electronic(1
Davison R.-B. — Commonwealth Immigrants
No full textT. G. Davison R.-B. — Commonwealth Immigrants. In: Population, 20ᵉ année, n°1, 1965. p. 153
Davison R.-B. — Commonwealth Immigrants
No full textT. G. Davison R.-B. — Commonwealth Immigrants. In: Population, 20ᵉ année, n°1, 1965. p. 153
Multisite bond and overlap treatment of polymer-chain band structure
No full textThe usual tight-binding (TB) approximation, employed in electronic structure calculations, is extended to include the more-distant neighbor sites than the first. In doing so, a simple power law is adopted to describe the bond and overlap contributions, which enables the energy dispersion relation to be obtained in a closed analytic form. The resulting energy band structure has markedly different features from its TB Counterpart to which it reduces in the appropriate limits. In particular, local extrema always occur at the TB stationary values, although these may not both be band edges. Another intermediate critical point may arise, which is one of the band edges, the other being located at one of the TB extrema. (C) 2003 Wiley Periodicals, Inc.PT: J; CR: ALSTRUP I, 1968, PHYS STATUS SOLIDI, V28, P555 ANDRE JM, 1990, INT J QUANTUM CHEM S, V24, P65 DAVISON SG, 1967, J SURF SCI, V6, P323 DAVISON SG, 1969, CHEM PHYS LETT, V3, P424 DAVISON SG, 1970, SOLID STATE PHYS, V25, P1 DAVISON SG, 1972, INT J QUANTUM CHEM, V6, P387 DAVISON SG, 1976, INT J QUANTUM CHEM, V10, P867 DAVISON SG, 1986, J PHYS CHEM-US, V90, P652 DAVISON SG, 1996, BASIC THEORY SURFACE DAVISON SG, 2002, ACTA PHYS CHIM DEBRE, V189, P34 FAIRBAIRN WM, 1968, SURF SCI, V9, P439 FUJIMOTO H, 1987, CHEM PHYS LETT, V141, P485 GILBERT TL, 1962, J MATH PHYS, V3, P107 HOFFMANN R, 1991, MACROMOLECULES, V24, P3725 KARPFEN A, 1982, PHYS SCR T, V1, P79 KOSTER GF, 1954, PHYS REV, V95, P1167 LAVIS DA, 1986, J PHYS C SOLID STATE, V19, P3125 LOWDIN PO, 1950, J CHEM PHYS, V18, P365 LOWDIN PO, 1951, J CHEM PHYS, V19, P1579 MCKINNON BA, 1995, PHYS REV B, V52, P14531 MIRABELLA DA, 1994, AM J PHYS, V62, P162 MIRABELLA DA, 1994, PHYS REV B, V50, P12152 MIRABELLA DA, 1998, INT J QUANTUM CHEM, V68, P285 MISKOVIC ZL, 1996, CHEM PHYS LETT, V260, P647 RUEDENBERG K, 1961, J CHEM PHYS, V34, P1878 SLATER JC, 1930, PHYS REV, V35, P509 SPRINGBORG M, 1989, PHYS REV B, V40, P3333 SPRINGBORG M, 2000, INT J QUANTUM CHEM, V77, P843 TAFERNER WT, 1997, CHEM PHYS LETT, V269, P171 TOMASEK M, 1960, J CZECH J PHYS B, V10, P268; NR: 30; TC: 0; J9: INT J QUANTUM CHEM; PG: 6; GA: 717VPSource type: Electronic(1
G. M. Kirkwood, A Study of Sophoclean Drama
No full textDavison J. A. G. M. Kirkwood, A Study of Sophoclean Drama. In: L'antiquité classique, Tome 28, fasc. 2, 1959. pp. 351-352
G. M. Kirkwood, A Study of Sophoclean Drama
No full textDavison J. A. G. M. Kirkwood, A Study of Sophoclean Drama. In: L'antiquité classique, Tome 28, fasc. 2, 1959. pp. 351-352
G. M. A. Grube, The Greek and Roman Critics
No full textDavison J. A. G. M. A. Grube, The Greek and Roman Critics. In: L'antiquité classique, Tome 35, fasc. 2, 1966. pp. 631-632
Surface states in electrochemisorption
No full textThe recursive Green function (RGF) method is used to obtain the surface and adatom RGFs for an electrified substate. The electrochemisorption (ECS) process is described, by invoking the Anderson-Newns (AN) model, whereby a self-consistent treatment of the ECS energy and charge transfer is provided. The role of the electric field, and the presence of surface states (SS), in governing magnetic and non-magnetic ECS is discussed in the case of H-Cr. (C) 2001 Elsevier Science Ltd. All rights reserved.PT: J; CR: ANDERSON PW, 1961, PHYS REV, V124, P41 DAVISON SG, 1988, SURF SCI, V200, P265 DAVISON SG, 1996, BASIC THEORY SURFACE DAVISON SG, 1997, J PHYS-CONDENS MAT, V9, P6371 ENGLISH RA, 1996, PROG SURF SCI, V53, P323 ENGLISH RA, 1997, PROG SURF SCI, V54, P241 ENGLISH RA, 1998, SURF SCI, V397, P251 MUSCAT JP, 1978, PROG SURF SCI, V9, P1 NEWNS DM, 1969, PHYS REV, V178, P1123; NR: 9; TC: 0; J9: PROG SURF SCI; PG: 11; GA: 460QCSource type: Electronic(1
sr516/iSALE3D_oblique_impacts:
No full textAdditional supporting information. Ejecta data from the model simulations used in Raducan, S. D., Davison, T. M., Collins, G. S. (2021) Ejecta distribution and momentum transfer from oblique impacts on asteroid surfaces. Icarus
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