TY - JOUR
T1 - Magnetic-substate ionization of medium- and high-Zt elements induced by proton impact
AU - Liu, Yitong
AU - Qin, Jinrui
AU - Wang, Xing
AU - Xu, Zhongfeng
N1 - Publisher Copyright:
© 2025 Elsevier B.V.
PY - 2025/5/5
Y1 - 2025/5/5
N2 - Magnetic-substate ionization of L3-subshell and the consequent atomic alignment of molybdenum, cadmium, indium and gold ions are reported for proton impact with low incident velocity range (0.147∼0.232)vL3, (0.124∼0.196)vL3, (0.120∼0.191)vL3, (0.067∼0.107)vL3, respectively. Here, vL3 is the classical orbital velocity of an electron in the L3-subshell of the target atom. It is demonstrated that the Lβ2 and Lα X-ray lines present spatially non-isotropic emission. Coster-Kronig calibration factors as well as anisotropy coefficients are calculated to derive the alignment parameter A20. Unifying A20 and the cross section σL3 in direct ionization, a novel methodology to determine the cross sections [Formula presented] and [Formula presented] for magnetic substate ionization is introduced. The results manifest that both cross sections exhibit positive correlation with the incident energy and inverse correlation with atomic number of the target. The cross section [Formula presented] is found to be greater than [Formula presented], and the tendency of the ratio [Formula presented] varies regularly and gradually as the atomic number increases for the four targets. Particularly, it also implies that the ionization cross section for high-Zt targets exhibits a more remarkable increase rate with the increase of incident energy. Experimental results are well understood by taking account of probability density distribution of the orbital electrons.
AB - Magnetic-substate ionization of L3-subshell and the consequent atomic alignment of molybdenum, cadmium, indium and gold ions are reported for proton impact with low incident velocity range (0.147∼0.232)vL3, (0.124∼0.196)vL3, (0.120∼0.191)vL3, (0.067∼0.107)vL3, respectively. Here, vL3 is the classical orbital velocity of an electron in the L3-subshell of the target atom. It is demonstrated that the Lβ2 and Lα X-ray lines present spatially non-isotropic emission. Coster-Kronig calibration factors as well as anisotropy coefficients are calculated to derive the alignment parameter A20. Unifying A20 and the cross section σL3 in direct ionization, a novel methodology to determine the cross sections [Formula presented] and [Formula presented] for magnetic substate ionization is introduced. The results manifest that both cross sections exhibit positive correlation with the incident energy and inverse correlation with atomic number of the target. The cross section [Formula presented] is found to be greater than [Formula presented], and the tendency of the ratio [Formula presented] varies regularly and gradually as the atomic number increases for the four targets. Particularly, it also implies that the ionization cross section for high-Zt targets exhibits a more remarkable increase rate with the increase of incident energy. Experimental results are well understood by taking account of probability density distribution of the orbital electrons.
KW - Angular distribution
KW - Atomic alignment
KW - Characteristic radiation
KW - Magnetic-substate ionization cross section
KW - Proton-atom collision
UR - https://www.scopus.com/pages/publications/86000157896
U2 - 10.1016/j.physleta.2025.130417
DO - 10.1016/j.physleta.2025.130417
M3 - 文章
AN - SCOPUS:86000157896
SN - 0375-9601
VL - 541
JO - Physics Letters, Section A: General, Atomic and Solid State Physics
JF - Physics Letters, Section A: General, Atomic and Solid State Physics
M1 - 130417
ER -