Multipole mixing effects on the angular distribution and polarization of dielectronic hypersatellite lines from highly charged helium-like ions

• Published in: Physics letters. A 2023-07, Vol.475, p.128852, Article 128852
• Main Authors: Ma, Kun, Wang, Shu-Xing, Zhu, Lin-Fan, Tang, Zhi-Ming, Xie, Lu-You
• Format: Article
• Language: English
• Subjects: Angular distribution; Dielectronic recombination; Multipole mixing; Polarization
• ISSN: 0375-9601; 1873-2429
• DOI: 10.1016/j.physleta.2023.128852

The angular distribution and the degree of linear polarization of the dielectronic hypersatellite lines of highly charged helium-like ions are studied by using the multiconfiguration Dirac-Fock method and density matrix theory with a focus on the multipole mixing effects. Detailed calculations have been carried out for the emission of characteristic X-rays from the (2s2p)P1,23 and P11 resonant states decay to the (1s2s)S13 state following the KLL dielectronic recombination of initial hydrogen-like ions with atomic nuclear charge from Z=22 to Z=100. It is shown that the mixing of electric dipole (E1) and magnetic quadrupole (M2) radiations significantly alters the angular distribution and the degree of linear polarization, in which the shifts are dependent on the resonant capture states and the atomic nuclear charges. The E1+M2 mixing has opposite effects for the (2s2p)P23 and (2s2p)P11 resonant states, except for the (2s2p)P11 resonance of the heavy ions with Z≳90, where the profile of angular distribution is reversed by strong mixing effects due to the contribution of the M2 term and its interference with the E1 radiative channel. The results should be of particular interest to the diagnosis of anisotropic plasmas and the test of fundamental physics in few-electron heavy ions. •Angular distribution and the degree of linear polarization of the dielectronic hypersatellite lines are studied.•Multipole mixing effects significantly alter the angular distribution and the degree of linear polarization.•Multipole mixing effects are dependent on resonant states and the atomic nuclear charge.