Results 171 to 180 of about 8,968 (231)
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The O16(He3, α)O15 and the O16(He3, He3)O16 reactions
Nuclear Physics, 1965Abstract Angular distributions of the O 16 (He 3 , α)O 15 g.s. reaction have been measured over the angular range 2.5–172° at laboratory energies of 8,8.5,9,9.42 and 10 MeV. Excitation functions have also been measured at angles of 45, 75 and 150° over this energy range. The peak and the total cross section varies by a factor of two over this energy
W.Parker Alford, L.M. Blau, D. Cline
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Production of heavy fragments in the reaction O16 + O16
Nuclear Physics, 1962Abstract Heavy framents produced in the bombardment of an oxygen target with 10 MeV per amu (atomic mass unit) oxygen ions have been investigated with a proportional counter-CsI scintillator telescope. This arrangement permitted identification of the nuclear charge (species) of fragments from lithium through neon, as well as measurement of the energy
P.G. Roll, F.E. Steigert
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Structure of a surface polysaccharide from Acinetobacter baumannii O16
Carbohydrate Research, 1996Simon R Haseley, Stephen G Wilkinson
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The Ep = 2.66 MeV resonance in O16(p, p)O16
Nuclear Physics, 1965Abstract The absolute differential cross section has been measured over the Ep = 2.66 MeV resonance [Ex(F17) = 3.10 MeV] in O16(p, p)O16 at the following angles in the centre-of-mass system: 54.5°, 70.5°, 90.0°, 107.0°, 125.5°, 140.5° and 151.3°. Also angular distributions (15 angles from θc.m.
V. Gomes +3 more
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Physics Letters, 1962
Gaseous nitrogen, enriched to 95% in N/sup 15/, was enclosed in a small duralumin chamber into which a beam of protons, collimated to a 16-in. diameter, could be directed through entrance and exit foils of thin nickel. Center-of mass differential scattering cross sections were measured at 70.1 to 140.8 deg as a function of proton energy at the target ...
G. Dearnaley +3 more
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Gaseous nitrogen, enriched to 95% in N/sup 15/, was enclosed in a small duralumin chamber into which a beam of protons, collimated to a 16-in. diameter, could be directed through entrance and exit foils of thin nickel. Center-of mass differential scattering cross sections were measured at 70.1 to 140.8 deg as a function of proton energy at the target ...
G. Dearnaley +3 more
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Structure of the O16 antigen of Stenotrophomonas maltophilia
Carbohydrate Research, 2001A polysaccharide containing D-ribose, N-acetyl-D-glucosamine, and N-acetyl-D-mannosamine was isolated from the phenol-soluble lipopolysaccharide extracted from defatted cell walls of the reference strain (560) for serogroup O16 of Stenotrophomonas maltophilia.
A M, Winn, S G, Wilkinson
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Nuclear Physics, 1962
Abstract An approximate Hartree-Fock self-consistent-field calculation is carried out for the ground state of the O16 nucleus. The two-body interaction used has a finite hard core as well as tensor and Serber exchange interaction. Our zeroth-order wave function gives an improved ground state energy of −116.3 MeV as compared to −87.8 MeV obtained with
Nazakat Ullah, R.K. Nesbet
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Abstract An approximate Hartree-Fock self-consistent-field calculation is carried out for the ground state of the O16 nucleus. The two-body interaction used has a finite hard core as well as tensor and Serber exchange interaction. Our zeroth-order wave function gives an improved ground state energy of −116.3 MeV as compared to −87.8 MeV obtained with
Nazakat Ullah, R.K. Nesbet
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Search for structure in the elastic scattering of O16 by O16 utilizing a gas target
Nuclear Physics, 1965Abstract Excitation curves for the elastic scattering of O 16 by O 16 have been taken with approximately 40 keV resolution in the bombarding energy range from 19 to 27 MeV. No significant resonant structure was observed confirming earlier work with a resolution of 250 keV.
E.B. Carter +3 more
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Cross sections for the O16(d, p0)O17, O16(d, p1O17∗ and O16(d, α0)N14 reactions from 0.8 to 1.7 MeV
Nuclear Physics, 1964Abstract Absolute cross sections for the O 16 (d, p 0 )O 17 , O 16 (d, p 1 )O 17∗ and O 16 (d, α 0 )N 14 reactions have been measured from 0.8 to 1.7 MeV at laboratory angles of 51.4°, 66.9°, 86.7°, 127.7°, 142.2° and 164.3°.
H.C. Kim +3 more
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Nuclear Physics, 1965
Abstract Even parity states in O 16 are studied using the shell model in the jj coupling scheme with a zero-range, spin-dependent residual interaction. This necessitates consideration of both one particle-one hole excitations through two oscillators shells and two particle-two hole excitations. The unperturbed energy spectrum is taken from data of
J.M. Eisenberg, B.M. Spicer, M.E. Rose
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Abstract Even parity states in O 16 are studied using the shell model in the jj coupling scheme with a zero-range, spin-dependent residual interaction. This necessitates consideration of both one particle-one hole excitations through two oscillators shells and two particle-two hole excitations. The unperturbed energy spectrum is taken from data of
J.M. Eisenberg, B.M. Spicer, M.E. Rose
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