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AbstractAbstract
[en] Total reaction cross sections, σR, for 8B, 12C, and 14N on natSi were measured from about 20 to 60 MeV/A. The σR for 12C and 14N compared reasonably well with conventional strong absorption and microscopic calculations. Measured σR for 8B were slightly larger than those for the two heavier nuclei, and notably larger than the conventional calculations. The 8B data were well reproduced by microscopic calculations using the same matter distribution used to explain the 8B guadrupole moment data, and therefore provide new evidence for the existence of a proton halo in 8B
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Fall meeting of the Division of Nuclear Physics of the American Physical Society; Bloomington, IN (United States); 25-28 Oct 1995; CONF-9510116--
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No abstract available
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Austin, S.M. (ed.); p. 360-364; 1972; Plenum Publishing Corp; New York; Symposium on the two-body force in nuclei; Ann Arbor, Michigan, USA; 7 Sep 1971
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Book
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Conference
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BARYONS, BEAMS, CHARGED PARTICLES, DIRECT REACTIONS, ELEMENTARY PARTICLES, ELEMENTS, ENERGY RANGE, EVEN-ODD NUCLEI, FERMIONS, HADRONS, HELIUM, HELIUM ISOTOPES, HYDROGEN ISOTOPES, ION BEAMS, ISOTOPES, KINETICS, LIGHT NUCLEI, MEV RANGE, NONMETALS, NUCLEAR REACTIONS, NUCLEI, NUCLEONS, ODD-EVEN NUCLEI, RARE GASES, REACTION KINETICS, SPECTRA, STABLE ISOTOPES
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[en] Recent double coincidence data for the 6Li + 6Li → 2α + 2d reaction show double spectator pole (DSP) peaks much sharper than those predicted from realistic 6Li cluster wave functions. The PWBA correctly predicts the centers and approximate amplitudes of these peaks. However, their widths remain much too large even when all obvious straightforward improvements - symmetry under boson exchange, Coulomb cluster wave functions, a finite-range participant interaction potential, and deuteron structure - are added to the model. (orig.)
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Journal Article
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Numerical Data
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Nuclear Physics. A; ISSN 0375-9474; ; v. 379(1); p. 191-204
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[en] Recent extensive measurements of total reaction cross sections (σR) for 38, 65, and 97 MeV deuterons on targets from 9Be to 208Pb were fitted with microscopic model calculations. Using accepted two- and three-parameter Fermi matter distributions for the targets, zero-range nucleon-nucleon forces, and eikonal orbits for the projectile, reasonable fits were obtained when the impact parameter was corrected for Coulomb force effects. Correcting the orbit for nuclear force effects worsened the fits somewhat, as did the use of finite-range nuclear forces; we argue however that it is redundant to make both of these corrections. The results were nearly independent of whether a Hulthacute en, Gartenhaus, or Gaussian form factor was used for the deuteron matter distribution. An attempt to fit older d+Pb σR measurements near 25 MeV indicated either a failure of the model at low energies or a need for remeasurement of those data. copyright 1997 The American Physical Society
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[en] Simple theoretical estimates of the cross sections for 2n removal from 6He and for combined 2n and 4n removal from 8He are compared with new measurements on Si targets at 0 endash 55 MeV/nucleon. Nuclear effects, described by a microscopic theory of Esbensen and Bertsch, account for nearly all of the observed cross sections. The electric dipole response function for 6He obtained by Danilin et al., whose calculations include valence n-n correlations, is used to predict a Coulomb dissociation cross section about 10% as large as that for nuclear dissociation. A smaller upper limit for 8He Coulomb dissociation is found by applying the non-energy-weighted sum rule. Equally good fits to the 800-MeV/nucleon 6,8He+C fragmentation data are obtained. copyright 1997 The American Physical Society
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CARBON 12 TARGET, CORRELATIONS, COULOMB FIELD, CROSS SECTIONS, DISSOCIATION, ELECTRIC DIPOLES, FRAGMENTATION, GEV RANGE 01-10, HEAVY ION-NUCLEUS REACTIONS, HELIUM 6 REACTIONS, HELIUM 8 REACTIONS, MEV RANGE 100-1000, NUCLEAR FRAGMENTATION, NUCLEI WITH MASS NUMBER 20 TO 38, NUCLEON-NUCLEON INTERACTIONS, RESPONSE FUNCTIONS, SILICON 28 TARGET, SUM RULES
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[en] The differential cross sections for 2H(6Li,α) α* (20.08 MeV) and 2H(6Li,α) α were measured at 300 c.m. from E/sub Li/ = 10 to 31 MeV. Possible evidence is presented for 8Be states decaying by α* emission, near the 3- and 4+ levels of an αα* rotational band in 8Be predicted by resonating group calculations
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Journal Article
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Phys. Rev., C; v. 19(1); p. 293-296
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ALPHA DECAY RADIOISOTOPES, ANGULAR MOMENTUM, BERYLLIUM ISOTOPES, CROSS SECTIONS, ENERGY LEVELS, ENERGY RANGE, EVEN-EVEN NUCLEI, EXCITED STATES, HEAVY ION REACTIONS, ISOTOPES, LIGHT NUCLEI, MEV RANGE, NUCLEAR REACTIONS, NUCLEI, PARTICLE PROPERTIES, RADIOISOTOPES, SECONDS LIVING RADIOISOTOPES, SPECTRA, TARGETS, VARIATIONAL METHODS
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No abstract available
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Journal Article
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Nuclear Physics. A; v. 204(3); p. 433-453
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BOUND STATE, DEUTERIUM, DIFFERENTIAL CROSS SECTIONS, DWBA, EXCHANGE INTERACTIONS, FEYNMAN DIAGRAM, FINAL-STATE INTERACTIONS, HELIUM 3, HELIUM 3 BEAMS, KNOCK-OUT REACTIONS, LABORATORY SYSTEM, MANY-BODY PROBLEM, MATRIX ELEMENTS, MEV RANGE 10-100, NEUTRONS, PICKUP REACTIONS, PROTONS, S MATRIX, WAVE FUNCTIONS
BARYONS, BEAMS, BORN APPROXIMATION, CROSS SECTIONS, DIAGRAMS, DIRECT REACTIONS, ELEMENTARY PARTICLES, ELEMENTS, ENERGY RANGE, EVEN-ODD NUCLEI, FERMIONS, FUNCTIONS, HADRONS, HELIUM, HELIUM ISOTOPES, HYDROGEN ISOTOPES, INTERACTIONS, ION BEAMS, ISOTOPES, LIGHT NUCLEI, MATRICES, MEV RANGE, NONMETALS, NUCLEAR REACTIONS, NUCLEI, NUCLEONS, RARE GASES, STABLE ISOTOPES
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[en] Microscopic calculations of nuclear reaction cross sections and total reaction probabilities are compared with measurements for the d+Si, 3,4He+Si, and d+Ge systems at energies ranging from 2 to 53 MeV/nucleon. Good agreement is obtained, except for 3He+Si at the very lowest energies, when zero-range nucleon-nucleon forces are assumed and realistic nuclear density distributions are used in the tail regions, where the models are most sensitive. The agreement is less good for finite-range forces. A strong absorption model gives much poorer agreement with the recent 4He+Si measurements than do the microscopic models
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[en] The internal momentum spectrum of p+n pairs produced in the /sup 6/Li(/alpha/,2/alpha/)pn reaction at 118 MeV was measured for those pairs whose c.m. was at rest after the reaction. This spectrum was calculated with a plane wave impulse approximation model, having no free parameters, for two p/sub 3/2/ nucleons initially bound in a harmonic oscillator potential. The calculation gave reasonable agreement with measured values of both the normalization of the spectrum and its dependence upon the p+n internal energy, when the final nucleons were described by Yamaguchi, Paris, or Reid wave functions and the data were reduced by the final-state energy prescription. Less satisfactory fits were obtained with p+n plane waves and/or the initial-state energy prescription
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Journal Article
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ACCELERATORS, BARYONS, CATIONS, CHARGED PARTICLES, COINCIDENCE METHODS, COUNTING TECHNIQUES, CYCLIC ACCELERATORS, CYCLOTRONS, DISTRIBUTION, ELEMENTARY PARTICLES, ENERGY RANGE, FERMIONS, FUNCTIONS, HADRONS, HEAVY ION ACCELERATORS, HELIUM IONS, HYDROGEN IONS, HYDROGEN IONS 1 PLUS, IONIZING RADIATIONS, IONS, ISOCHRONOUS CYCLOTRONS, MATHEMATICAL MODELS, MEV RANGE, NUCLEAR REACTIONS, NUCLEON-NUCLEON POTENTIAL, POTENTIALS, RADIATIONS, TARGETS
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No abstract available
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Journal Article
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Nuclear Physics. A; v. 206(1); p. 207-216
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