Search results for "HOD"
showing 10 items of 16270 documents
Rapid evaluation of notch stress intensity factors using the peak stress method with 3D tetrahedral finite element models: Comparison of commercial c…
2022
The peak stress method (PSM) allows a rapid application of the notch stress intensity factor (NSIF) approach to the fatigue life assessment of welded structures, by employing the linear elastic peak stresses evaluated by FE analyses with coarse meshes. Because of the widespread adoption of 3D modeling of large and complex structures in the industry, the PSM has recently been boosted by including four-node and ten-node tetrahedral elements of Ansys FE software, which allows to discretize complex geometries. In this paper, a Round Robin among eleven Italian Universities has been performed to calibrate the PSM with seven different commercial FE software packages. Several 3D mode I, II and III …
CCDC 762079: Experimental Crystal Structure Determination
2010
Related Article: Duc Hanh Nguyen, H.Laureano, S.Juge, P.Kalck, J.-C.Daran, Y.Coppel, M.Urrutigoity, M.Gouygou|2009|Organometallics|28|6288|doi:10.1021/om900684w
CCDC 804806: Experimental Crystal Structure Determination
2013
Related Article: D.H.Nguyen, J.Bayardon, C.Salomon-Bertrand, S.Juge, P.Kalck, J.-C.Daran, M.Urrutigoity, M.Gouygou|2012|Organometallics|31|857|doi:10.1021/om2008265
Comparative theoretical study of the Ag–MgO (100) and (110) interfaces
1999
We have calculated the atomic and electronic structures of Ag–MgO(100) and (110) interfaces using a periodic (slab) model and an ab initio Hartree–Fock approach with a posteriori electron correlation corrections. The electronic structure information includes interatomic bond populations, effective charges, and multipole moments of ions. This information is analyzed in conjunction with the interface binding energy and the equilibrium distances for both interfaces for various coverages. There are significant differences between partly covered surfaces and surfaces with several layers of metal, and these can be understood in terms of electrostatics and the electron density changes. For complet…
CCDC 194089: Experimental Crystal Structure Determination
2003
Related Article: M.Poyatos, E.Mas-Marza, J.A.Mata, M.Sanau, E.Peris|2003|Eur.J.Inorg.Chem.||1215|doi:10.1002/ejic.200390157
CCDC 814708: Experimental Crystal Structure Determination
2011
Related Article: N.Khiri, E.Bertrand, M.-J.Ondel-Eymin, Y.Rousselin, J.Bayardon, P.D.Harvey, S.Juge|2010|Organometallics|29|3622|doi:10.1021/om100520u
CCDC 1426906: Experimental Crystal Structure Determination
2016
Related Article: Erik Ekengard, Kamlesh Kumar, Thibault Fogeron, Carmen de Kock, Peter J. Smith, Matti Haukka, Magda Monari, Ebbe Nordlander|2016|Dalton Trans.|45|3905|doi:10.1039/C5DT03739E
Re: Technique of internal mammary dissection using pectoralis major flap to prevent contour deformities
2009
Structure, morphology and photoluminescence emissions of ZnMoO4: RE 3+=Tb3+ - Tm3+ - X Eu3+ (x = 1, 1.5, 2, 2.5 and 3 mol%) particles obtained by the…
2018
Made available in DSpace on 2018-12-11T17:36:34Z (GMT). No. of bitstreams: 0 Previous issue date: 2018-06-25 Coordenação de Aperfeiçoamento de Pessoal de Nível Superior (CAPES) Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq) Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP) Ministerio de Economía y Competitividad ZnMoO4 and ZnMoO4: RE3+ = 1% Tb3+, 1% Tm3+, x Eu3+ (x = 1, 1.5, 2, 2.5 and 3 mol%) particles were prepared by a sonochemical method. The influence of the dopant content on photoluminescent behavior was investigated. The X-ray diffraction results confirmed the formation of the α-ZnMoO4 phase with a triclinic crystalline structure. The influence of th…
Energy transfer in LH2 of Rhodospirillum Molischianum, studied by subpicosecond spectroscopy and configuration interaction exciton calculations.
2001
Two color transient absorption measurements were performed on a LH2 complex from Rhodospirillum molischianum by using several excitation wavelengths (790, 800, 810, and 830 nm) and probing in the spectral region from 790 to 870 nm at room temperature. The observed energy transfer time of ∼1.0 ps from B800 to B850 at room temperature is longer than the corresponding rates in Rhodopseudomonas acidophila and Rhodobacter sphaeroides. We observed variations (0.9-1.2 ps) of B800-850 energy transfer times at different B800 excitation wavelengths, the fastest time (0.9 ps) was obtained with 800 nm excitation. At 830 nm excitation the energy transfer to the B850 ring takes place within 0.5 ps. The m…