Nuclear-matter distribution in the proton-rich nuclei $^7$Be and $^8$B from intermediate energy proton elastic scattering in inverse kinematics

التفاصيل البيبلوغرافية
العنوان: Nuclear-matter distribution in the proton-rich nuclei $^7$Be and $^8$B from intermediate energy proton elastic scattering in inverse kinematics
المؤلفون: Dobrovolsky, A. V., Korolev, G. A., Inglessi, A. G., Alkhazov, G. D., Colò, G., Dillmann, I., Egelhof, P., Estradé, A., Farinon, F., Geissel, H., Ilieva, S., Ke, Y., Khanzadeev, A. V., Kiselev, O. A., Kurcewicz, J., Le, X. C., Litvinov, Yu. A., Petrov, G. E., Prochazka, A., Scheidenberger, C., Sergeev, L. O., Simon, H., Takechi, M., Tang, S., Volkov, V., Vorobyov, A. A., Weick, H., Yatsoura, V. I.
سنة النشر: 2019
المجموعة: Nuclear Experiment
Nuclear Theory
مصطلحات موضوعية: Nuclear Experiment, Nuclear Theory
الوصف: Absolute differential cross sections for elastic $p^7$Be and $p^8$B small-angle scattering were measured in inverse kinematics at an energy of 0.7 GeV/u at GSI Darmstadt. The hydrogen-filled ionization chamber IKAR was used as an active target to detect the recoil protons. The projectile tracking and isotope identification were performed with multi-wire proportional chambers and scintillation detectors. The measured cross sections were analysed using the Glauber multiple-scattering theory. The root-mean-square (rms) nuclear matter radii $R_{\rm m} = 2.42 (4)$ fm for $^7$Be and $R_{\rm m} = 2.58 (6)$ fm for $^8$B were obtained. The radial density distribution deduced for $^8$B exhibits a proton halo structure with the rms halo radius $R_{\rm h} = 4.24 (25)$ fm. A comparison of the deduced experimental radii is displayed with existing experimental and theoretical data.
Comment: 18 pages, 6 figures. arXiv admin note: text overlap with arXiv:1803.02044
نوع الوثيقة: Working Paper
DOI: 10.1016/j.nuclphysa.2019.05.012
URL الوصول: http://arxiv.org/abs/1905.11399
رقم الأكسشن: edsarx.1905.11399
قاعدة البيانات: arXiv
الوصف
DOI:10.1016/j.nuclphysa.2019.05.012