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Parametrization of the angular correlation and degree of linear polarization in two-photon decays of hydrogenlike ions

P. Amaro, F. Fratini, S. Fritzsche, P. Indelicato, J. P. Santos, and A. Surzhykov
Phys. Rev. A 86, 042509 – Published 16 October 2012

Abstract

The spontaneous two-photon emission in hydrogenlike ions is investigated within the framework of second-order perturbation theory and Dirac's equation. Special attention is paid to the angular correlation of the emitted photons as well as to the degree of linear polarization of one of the two photons, if the second is just observed under arbitrary angles. Expressions for the angular correlation and the degree of linear polarization are expanded in powers of cosine functions of the two-photon opening angle, whose coefficients depend on the atomic number and the energy sharing of the emitted photons. The effects of including higher (electric and magnetic) multipoles upon the emitted photon pairs beyond the electric-dipole approximation are also discussed. Calculations of the coefficients are performed for the transitions 2s1/21s1/2, 3d3/21s1/2, and 3d5/21s1/2, along the entire hydrogen isoelectronic sequence (1Z100).

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  • Received 29 July 2012

DOI:https://doi.org/10.1103/PhysRevA.86.042509

©2012 American Physical Society

Authors & Affiliations

P. Amaro1,2,*, F. Fratini1,3,4, S. Fritzsche3,4, P. Indelicato5, J. P. Santos2, and A. Surzhykov1,3

  • 1Physikalisches Institut, Universität Heidelberg, D-69120 Heidelberg, Germany
  • 2Centro de Física Atómica, CFA, Departamento de Física, Faculdade de Ciências e Tecnologia, FCT, Universidade Nova de Lisboa, 2829-516 Caparica, Portugal
  • 3GSI Helmholtzzentrum für Schwerionenforschung, D-64291 Darmstadt, Germany
  • 4Department of Physics, P.O. Box 3000, Fin—90014 University of Oulu, Finland
  • 5Laboratoire Kastler Brossel, École Normale Supérieure, CNRS, Université P. et M. Curie–Paris 6, Case 74, 4, place Jussieu, 75252 Paris CEDEX 05, France

  • *pamaro@physi.uni-heidelberg.de

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Issue

Vol. 86, Iss. 4 — October 2012

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Images

  • Figure 1
    Figure 1
    Geometry of the two-photon decay. The z axis is collinear with the first photon momentum vector k1. The plane zx contains the second photon momentum vector k2 The angle θ is the opening angle between the direction of the two photons.Reuse & Permissions
  • Figure 2
    Figure 2
    Values of the parameters ai defined in Eq. (9), for the 2s1/21s1/2 transition as a function of Z. The values obtained in this work, which correspond to different energy shares y=0.1, 0.25, and 0.5, are represented by a black-solid, red-dashed, and green-dot-dashed curve, respectively. With exception of a0 (given in s1), all parameters are dimensionless. The same energy shares values given by Au [17] are represented by a blue dotted line (y=0.5), a cyan dot-dot-dashed line (y=0.25), and by the purple short dashed line (y=0.1). The parameters a2 of Ref. [17] are always equal to one, as represented by the purple dotted line. On the bottom right plot, the blue dotted line refers to values of the total decay rate obtained from the parametrization of Ref. [17]. The black line represents the total decay values obtained from our current parametrization. The dark green dashed line contains the values provided by Refs. [18, 19]. The level of precision of the plot does not allow one to distinguish differences between these references. Values of parameters bi can be obtained from this figure using the relations b0a0, b1a3, and b4a4.Reuse & Permissions
  • Figure 3
    Figure 3
    Values of the parameters ai defined in Eq. (9), for the 2d3/21s1/2 transition as function of Z. The different energy shares y=0.1, 0.25, 0.5 are represented by a black-solid, red-dashed, and green-dot-dashed curve, respectively. With exception of a0 (given in s1), all parameters are dimensionless. Values for parameters bi can be obtained from this figure (within its resolution) using the relations b0a0/13 and b113a3.Reuse & Permissions
  • Figure 4
    Figure 4
    Values of the parameters ai defined in Eq. (9), for the 2d5/21s1/2 transition as a function of Z. The different energy shares y=0.1, 0.25, 0.5 are represented by a black-solid, red-dashed, and green-dot-dashed curve, respectively. With exception of a0 (given in s1), all parameters are dimensionless.Reuse & Permissions
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