Ultraviolet suppression and nonlocality in optical model potentials for nucleon-nucleus scattering

نویسندگان

چکیده

We investigate the role of high momentum components optical model potentials for nucleon-nucleus scattering and its incidence on their nonlocal structure in coordinate space. The study covers closed-shell nuclei with mass number range $$4 \le A 208$$ , nucleon energies from tens MeV up to 1 GeV. To this purpose microscopic were calculated using density-dependent off-shell g matrices Brueckner-Hartree-Fock approximation based Argonne $$v_{18}$$ as well chiral 2N force next-to-next-to-next-to-leading order. confirm that gradual suppression high-momentum contributions potential results quite different coordinate-space counterparts, all them accounting same observables. infer a minimum cutoff Q, function target energy process, filters out irrelevant ultraviolet potential. find when is applied Perey-Buck or local Woods-Saxon potentials, they result similar those obtained models examine transversal nonlocality, quantity makes comparable intrinsic nonlocality any regardless representation. conclude meaningful comparisons features alternative require components.

برای دانلود رایگان متن کامل این مقاله و بیش از 32 میلیون مقاله دیگر ابتدا ثبت نام کنید

اگر عضو سایت هستید لطفا وارد حساب کاربری خود شوید

منابع مشابه

Microscopic optical potentials for nucleon - nucleus scattering

Microscopic optical potentials for nucleon-nucleus (NA) scattering obtained from the folding of the effective g matrices, solutions of the Bruckner-BetheGoldstone equation, with the densities of the target, are applied to the case of neutron-nucleus scattering. Given that the optical potentials are specified in all two-body angular momentum, spin and isospin channels available to the NA scatter...

متن کامل

Microscopic Optical Potentials for Elastic Nucleon-Nucleus Scattering

The theoretical approach to the elastic scattering of a nucleon from a nucleus, pioneered by Watson [1], made familiar by Kerman, McManus, and Thaler (KMT) [2] and further developed as the spectator expansion [3, 4, 5, 6] is now being applied with striking success. In a similar vein, a slightly di erent approach to the multiple scattering expansion within the KMT framework is being pursued by t...

متن کامل

Comparison of Dirac and microscopic Schrödinger optical model potentials for nucleon - nucleus scattering

Detailed comparisons are made between results of calculations for intermediate energy nucleon– 208 Pb scattering using optical potentials obtained from Dirac phenomenology and a microscopic Schrödinger model. The two approaches yield quite similar results for all of the observables with each projectile , including spin observables, suggesting the two models are physically equivalent. A new phen...

متن کامل

Non - localities in nucleon - nucleus potentials and their effects in nucleon - nucleus scattering

Two causes of non-locality inherent in nucleon-nucleus scattering are considered. They are the results of two-nucleon antisymmetry of the projectile with each nucleon in the nucleus and the dynamic polarization potential representation of channel coupling. For energies ∼ 40− 300 MeV, a g-folding model of the optical potential is used to show the influence of the knock-out process that is a resu...

متن کامل

Full-Folding Optical Potentials for Elastic Nucleon-Nucleus Scattering based on Realistic Densities

Optical model potentials for elastic nucleon nucleus scattering are calculated for a number of target nuclides from a full-folding integral of two different realistic target density matrices together with full off-shell nucleonnucleon t-matrices derived from two different Bonn meson exchange models. Elastic proton and neutron scattering observables calculated from these full-folding optical pot...

متن کامل

ذخیره در منابع من


  با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید

ژورنال

عنوان ژورنال: The European Physical Journal A

سال: 2021

ISSN: ['1434-6001', '1434-601X']

DOI: https://doi.org/10.1140/epja/s10050-020-00328-0