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AbstractAbstract
[en] A molecular orbital theory is formulated based on α transfer for the interpretation of subbarrier fusion enhancement. The molecular potential induced by α transfer causes the enhancement of the fusion. The fusion cross section is calculated for the 24Mg + 32S case. Good fits to experimental data can be reached naturally
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[en] The oscillatory structure appeared in the differential cross section of the reaction for 16O(16O, 12C)20Ne may be explained by particle transfer from covalent channel to ionic channel in the nuclear molecular orbital theory
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[en] In the differential cross sections for the elastic scattering between an α-conjugate target and projectile, a rising oscillatory structure is often observed in the backward-angle region. An α-transfer mechanism is proposed to explain this anomalous phenomenon. A nuclear molecular-orbit approximation theory for both 1α- and 2α-transfer processes has been formulated and applied to 16O+20Ne and 12C+20Ne scattering systems with different projectile energies. The experimental rising structures shown in these scatterings are well reproduced with parameters fairly consistent with spectroscopic data. An independent-α-particle model wave function has been used for the evaluation of the exchange potential, which gives better agreement with experiment than the Buttle-Goldfarb approximation can usually provide. (orig.)
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Nuclear Physics. A; ISSN 0375-9474; ; v. 438(1); p. 281-300
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ALPHA-TRANSFER REACTIONS, ANGULAR DISTRIBUTION, CARBON 12, CARBON 12 REACTIONS, CLUSTER MODEL, DIFFERENTIAL CROSS SECTIONS, ELASTIC SCATTERING, EXCHANGE INTERACTIONS, FOUR-NUCLEON TRANSFER REACTION, HEAVY ION REACTIONS, MAGNESIUM 24, MAGNESIUM 24 TARGET, MEV RANGE 10-100, MULTI-NUCLEON TRANSFER REACTIO, NEON 20, NEON 20 TARGET, NUCLEAR MOLECULES, ORBITS, OXYGEN 16, OXYGEN 16 REACTIONS, THEORETICAL DATA, WAVE FUNCTIONS, WOODS-SAXON POTENTIAL
CARBON ISOTOPES, CROSS SECTIONS, DATA, DIRECT REACTIONS, DISTRIBUTION, ENERGY RANGE, EVEN-EVEN NUCLEI, FUNCTIONS, INFORMATION, INTERACTIONS, ISOTOPES, LIGHT NUCLEI, MAGNESIUM ISOTOPES, MATHEMATICAL MODELS, MEV RANGE, NEON ISOTOPES, NUCLEAR MODELS, NUCLEAR POTENTIAL, NUCLEAR REACTIONS, NUCLEI, NUMERICAL DATA, OXYGEN ISOTOPES, POTENTIALS, SCATTERING, STABLE ISOTOPES, TARGETS, TRANSFER REACTIONS
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[en] Within the framework of meson exchange theory, the N-N interaction is derived by a classical field method from a chiral σ-ω model. The nuclear potential derived is similar to the ordinary one boson exchange potential
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BARYON-BARYON INTERACTIONS, BARYONS, BOSON-EXCHANGE MODELS, ELEMENTARY PARTICLES, FERMIONS, HADRON-HADRON INTERACTIONS, HADRONS, HYPERONS, INTERACTIONS, MATHEMATICAL MODELS, OMEGA BARYONS, PARTICLE INTERACTIONS, PARTICLE MODELS, PARTICLE PROPERTIES, PERIPHERAL MODELS, POTENTIALS, STRANGE PARTICLES, SYMMETRY
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[en] Resonant structures appeared in the excitation functions for the 16O + 20Ne elastic scattering have been studied by the nuclear molecular orbital theory. The theoretical results agree will with the experimental data
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[en] As two skyrmions overlap, a molecular-like binding may arise. This may be one of the main sources of missing intermediate range attraction in NN interaction. The attraction is found to be strong enough to form bound state of two nucleons. It seems then that one no longer needs to introduce phenomenologically scalar meson which has never been observed
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[en] In the excitation function for the elastic scattering between an α-conjugate target and projectile, there often exist intermediate structures which cannot be interpreted easily either by conventional optical potential model or statistical theory. A nuclear molecular-orbital approximation theory for the α-transfer mechanism has been formulated and applied to the 24Mg(16O,12C)28Si reaction. The excitation function at θc.m. = 00 and differential cross section in the whole angle region at three different energies Ec.m. = 27.8, 30.8 and 36.2 MeV are calculated. The calculations reproduce well these experimental curves with a common set of parameters. The intermediate structures shown naturally in the excitation function and the anomalous oscillatory structures appear in the whole angle region of the differential cross section. (orig.)
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ALPHA-TRANSFER REACTIONS, ANGULAR DISTRIBUTION, CARBON 12, CENTRAL POTENTIAL, COUPLED CHANNEL THEORY, DIFFERENTIAL CROSS SECTIONS, ELASTIC SCATTERING, ENERGY DEPENDENCE, EXCITATION FUNCTIONS, FOUR-NUCLEON TRANSFER REACTION, GAUSS POTENTIAL, HAMILTONIANS, HEAVY ION REACTIONS, MAGNESIUM 24 TARGET, MEV RANGE 10-100, MOLECULAR ORBITAL METHOD, MULTI-NUCLEON TRANSFER REACTIO, NUCLEAR MOLECULES, NUCLEAR STRUCTURE, OPTICAL MODELS, OXYGEN 16 REACTIONS, SILICON 28, THEORETICAL DATA, WAVE FUNCTIONS, WOODS-SAXON POTENTIAL
CARBON ISOTOPES, CROSS SECTIONS, DATA, DIRECT REACTIONS, DISTRIBUTION, ENERGY RANGE, EVEN-EVEN NUCLEI, FUNCTIONS, INFORMATION, ISOTOPES, LIGHT NUCLEI, MATHEMATICAL MODELS, MATHEMATICAL OPERATORS, MEV RANGE, NUCLEAR POTENTIAL, NUCLEAR REACTIONS, NUCLEI, NUCLEON-NUCLEON POTENTIAL, NUMERICAL DATA, POTENTIALS, QUANTUM OPERATORS, SCATTERING, SILICON ISOTOPES, STABLE ISOTOPES, TARGETS, TRANSFER REACTIONS
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[en] Based on the scattering theory of KMT and FGH we calculate the nucleon-nucleus optical potentials of 4He, 16O and 40Ca from the Paris N-N potential given by M. Lacombe et al. The real part Vsub(R)(r) of our optential has the form of Woods-Saxon when the kinetic energy E of the incident nucleon is low. The depth of Vsub(R)(r) will decrease as E increases, and it turns into positive in the interior of nucleus when E approx.= 300 MeV. The repulsive effect in the interior of nucleus increases rapidly as E increases even more, butthere always exists some attractive effect at the surface of nucleus. Therefore, Vsub(R)(r) has generally the wine-bottle bottom shape. We also calculate the quatity Jv/N = (4π/N)∫sub(0)sub(infinity)Vsub(R)(r)r2dr. Our results are basically in acordance with those of M.Jaminon et al's relativistic Hatree calculation as well as the experimental results. In this work we also calculate the imaginary part of optical potential and its variation with the kinetic energy of the incident nucleon
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Chinese Journal of Nuclear Physics; CODEN YTHLD; v. 6(3); p. 234-244
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[en] The mechanism of transfering a cluster of nucleons between two colliding nuclei is considered to explain the backward angle oscillatory rise in the differential cross section of the elastic scattering between certain nuclei, such as 16O + 24Mg or 20Ne + 24Mg. The nuclear molecular orbit approximation theory is applied. For one-step transfer, if the parameter involved is assumed to be adjustable, the numerical calculations can be made to fit the experimental results naturally
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Phys. Energ. Fortis Phys. Nucl; CODEN KNWLD; v. 9(1); p. 101-107
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[en] A phenomenological parity-dependent potential has been obtained for analysing resonant structure in the 16O+20Ne system with a deep optical potential and is compared with the potential from the linear combination of nuclear orbital model. This potential agrees in both sign and magnitude in the tail region with the calculation, and the former is roughly an envelope curve of the latter. (orig.)
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ANGULAR DISTRIBUTION, ARGON 36, CENTRAL POTENTIAL, DIFFERENTIAL CROSS SECTIONS, ENERGY DEPENDENCE, EXCITATION FUNCTIONS, HIGH SPIN STATES, MEV RANGE 10-100, NEON 20, NEON 20 TARGET, NUCLEAR MODELS, OPTICAL MODELS, OXYGEN 16, OXYGEN 16 REACTIONS, PARITY, POTENTIAL SCATTERING, RESONANCE, ROTATIONAL STATES, THEORETICAL DATA, WOODS-SAXON POTENTIAL
ARGON ISOTOPES, CROSS SECTIONS, DATA, DISTRIBUTION, ELASTIC SCATTERING, ENERGY LEVELS, ENERGY RANGE, EVEN-EVEN NUCLEI, EXCITED STATES, HEAVY ION REACTIONS, INFORMATION, ISOTOPES, LIGHT NUCLEI, MATHEMATICAL MODELS, MEV RANGE, NEON ISOTOPES, NUCLEAR POTENTIAL, NUCLEAR REACTIONS, NUCLEI, NUMERICAL DATA, OXYGEN ISOTOPES, PARTICLE PROPERTIES, POTENTIALS, SCATTERING, STABLE ISOTOPES, TARGETS
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