S. Yu. Mezhevych, O. A. Ponkratenko, N. Keeley, Yu. S. Roznyuk, O. M. Povoroznyk, O. K. Gorpinich, V. I. Grantsev, O. O. Jachmenjov, K. K. Kisurin, S. E. Omelchuk, B. A. Rudenko, L. I. Slyusarenko, B. G. Struzhko, I. I. Vertegel
{"title":"Analysis of the angular distribution for the elastic scattering of \\(\\alpha \\) particles from tritium at an energy of 84.2 MeV","authors":"S. Yu. Mezhevych, O. A. Ponkratenko, N. Keeley, Yu. S. Roznyuk, O. M. Povoroznyk, O. K. Gorpinich, V. I. Grantsev, O. O. Jachmenjov, K. K. Kisurin, S. E. Omelchuk, B. A. Rudenko, L. I. Slyusarenko, B. G. Struzhko, I. I. Vertegel","doi":"10.1140/epja/s10050-025-01683-6","DOIUrl":null,"url":null,"abstract":"<div><p>New experimental angular distribution data are reported for the <span>\\(\\alpha \\)</span>+t elastic scattering at <span>\\(E_\\textrm{lab}(\\alpha ) = 84.2\\)</span> MeV (<span>\\(E_\\textrm{cm} = 36.09\\)</span> MeV) covering both forward and backward scattering angles. An analysis was carried out using the coupled-reaction-channels (CRC) formalism including the transfer of a proton between the two triton cores. Automatic searches on the parameters of the <span>\\(\\alpha \\)</span>+t optical model potential of volume Woods-Saxon form, together with the spectroscopic factor (SF), were performed using the code SFRESCO. The inclusion of a proper core-core (t+t) potential was found to be important and led to slightly higher values of the SF being obtained. The deduced value of the SF for the <span>\\(\\alpha \\)</span> <span>\\(\\rightarrow \\)</span> t+p overlap (1.33 ± 0.05) agrees very well with that found earlier for the mirror system <span>\\(^3\\)</span>He+n. However, both are lower than the value of 2.0 predicted by the shell model. The asymptotic normalization coefficient (ANC) was also deduced and the variations of the SF and <span>\\(\\text {ANC}^2\\)</span> as a function of the radius of the t+p binding potential appear to be different, that of the SF being almost linear while the <span>\\(\\text {ANC}^2\\)</span> increases approximately exponentially with increasing binding potential radius. Nevertheless, the best fit value of the <span>\\(\\text {ANC}^2\\)</span> = 45.5 ± 1.8 <span>\\(\\text {fm}^{-1}\\)</span> was found to be close to those obtained theoretically by Monte Carlo calculations.</p></div>","PeriodicalId":786,"journal":{"name":"The European Physical Journal A","volume":"61 9","pages":""},"PeriodicalIF":2.8000,"publicationDate":"2025-09-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"The European Physical Journal A","FirstCategoryId":"4","ListUrlMain":"https://link.springer.com/article/10.1140/epja/s10050-025-01683-6","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"PHYSICS, NUCLEAR","Score":null,"Total":0}
引用次数: 0
Abstract
New experimental angular distribution data are reported for the \(\alpha \)+t elastic scattering at \(E_\textrm{lab}(\alpha ) = 84.2\) MeV (\(E_\textrm{cm} = 36.09\) MeV) covering both forward and backward scattering angles. An analysis was carried out using the coupled-reaction-channels (CRC) formalism including the transfer of a proton between the two triton cores. Automatic searches on the parameters of the \(\alpha \)+t optical model potential of volume Woods-Saxon form, together with the spectroscopic factor (SF), were performed using the code SFRESCO. The inclusion of a proper core-core (t+t) potential was found to be important and led to slightly higher values of the SF being obtained. The deduced value of the SF for the \(\alpha \)\(\rightarrow \) t+p overlap (1.33 ± 0.05) agrees very well with that found earlier for the mirror system \(^3\)He+n. However, both are lower than the value of 2.0 predicted by the shell model. The asymptotic normalization coefficient (ANC) was also deduced and the variations of the SF and \(\text {ANC}^2\) as a function of the radius of the t+p binding potential appear to be different, that of the SF being almost linear while the \(\text {ANC}^2\) increases approximately exponentially with increasing binding potential radius. Nevertheless, the best fit value of the \(\text {ANC}^2\) = 45.5 ± 1.8 \(\text {fm}^{-1}\) was found to be close to those obtained theoretically by Monte Carlo calculations.
期刊介绍:
Hadron Physics
Hadron Structure
Hadron Spectroscopy
Hadronic and Electroweak Interactions of Hadrons
Nonperturbative Approaches to QCD
Phenomenological Approaches to Hadron Physics
Nuclear and Quark Matter
Heavy-Ion Collisions
Phase Diagram of the Strong Interaction
Hard Probes
Quark-Gluon Plasma and Hadronic Matter
Relativistic Transport and Hydrodynamics
Compact Stars
Nuclear Physics
Nuclear Structure and Reactions
Few-Body Systems
Radioactive Beams
Electroweak Interactions
Nuclear Astrophysics
Article Categories
Letters (Open Access)
Regular Articles
New Tools and Techniques
Reviews.