Interference, post-collision interaction and exchange effects in angular distribution patterns of resonant photo double-ionization in neon for equal electron energies

Angle-resolved patterns of the fivefold-differential cross section in neon are calculated ab initio for the case of resonant photo double-ionization under the condition of equal energies of the ejected electrons. The patterns reveal the important role of direct and indirect processes as well as post-collision interaction (PCI), interference and exchange effects. Comparison with available experimental data shows that some of these effects are readily confirmed, but the angular range with dramatic PCI effects still awaits experimental verification.

[1]  V. Schmidt,et al.  Postcollision Interaction in the Coincident Emission of Photoelectrons and Auger Electrons at Small Relative Angles , 1999 .

[2]  U. Heinzmann,et al.  Complete description of the Xe 4d photoionization by spin-resolved photoelectron and Auger spectroscopy , 1999 .

[3]  I. Bray,et al.  Application of the CCC method to the calculation of helium double-photoionization triply differential cross sections , 1998 .

[4]  J. Ullrich,et al.  Absolute triple differential cross sections for photo-double ionization of helium - experiment and theory , 1998 .

[5]  T. Reddish,et al.  2e) cross section measurements of and He , 1998 .

[6]  P. Lablanquie,et al.  LETTER TO THE EDITOR: Interference effects in inner-shell double photoionization of xenon , 1998 .

[7]  O. Gessner,et al.  Interference Effects between Auger and Photoelectron Studied by Subnatural Linewidth Auger-Photoelectron Coincidence Spectroscopy , 1998 .

[8]  J. Ullrich,et al.  Photo-double-ionization of He: Fully differential and absolute electronic and ionic momentum distributions , 1998 .

[9]  P. V. Kampen,et al.  Matrix elements for photoionization in xenon derived from coincidence electron spectrometry , 1997 .

[10]  V. Schmidt,et al.  PCI and interference effects in the energy and angular correlation between the photoelectron and the Auger electron for equal electron energies , 1997 .

[11]  P. Lablanquie,et al.  Double photoionization: II. Analysis of experimental triple differential cross sections in helium and neon , 1997 .

[12]  A. Malcherek,et al.  Triply differential cross sections for the photo-double ionization of neon , 1996 .

[13]  B. Krassig,et al.  State dependence of angular correlation patterns in double photoionization , 1996 .

[14]  V. Schmidt,et al.  Interference effects in the angular correlation between the photoelectron and the Auger electron of the same kinetic energy in the ionization of xenon , 1996 .

[15]  V. Schmidt,et al.  Interference effects in angular patterns of resonant double photoionization in neon , 1996 .

[16]  Briggs,et al.  Angular distributions for double photoionization of helium: Discrepancies between theory and experiment. , 1996, Physical review. A, Atomic, molecular, and optical physics.

[17]  Kazansky,et al.  Electron correlation in double photoionization: Comparative study of secondary structure for Ne and Xe. , 1995, Physical Review A. Atomic, Molecular, and Optical Physics.

[18]  V. Schmidt,et al.  Experimental determination of the absolute value of the triple differential cross section for double photoionization in helium , 1995 .

[19]  Kazansky,et al.  Wannier-ridge theory of angular distribution. , 1995, Physical Review A. Atomic, Molecular, and Optical Physics.

[20]  L. Avaldi,et al.  Near threshold TDCS for photo-double ionization of helium , 1995 .

[21]  Pont,et al.  Absolute triply differential cross sections for double photoionization of helium at 10, 20, and 52.9 eV above threshold. , 1995, Physical review. A, Atomic, molecular, and optical physics.

[22]  Sellés,et al.  Effect of electron energy sharing on the double photoionization of helium near threshold. , 1995, Physical review letters.

[23]  J. Briggs,et al.  Selection rules for transitions to two-electron continuum states , 1995 .

[24]  Macek,et al.  Coherences in the decay of autoionizing states in photoionization. I. Exchange effect between photo- and Auger electrons. , 1994, Physical review. A, Atomic, molecular, and optical physics.

[25]  J. Briggs,et al.  Double photoionization in the case of unequal energy sharing , 1994 .

[26]  S. Sheinerman,et al.  PCI influence on angular distribution of Auger and autoionization electrons , 1994 .

[27]  B. Krassig,et al.  Energy- and angle-resolved double photoionization in argon leading to the 3p-2 1De final ionic state , 1993 .

[28]  J. Briggs,et al.  Angular distribution of electrons following double photoionization , 1993 .

[29]  Schmidt,et al.  Energy- and angle-resolved double photoionization in helium. , 1993, Physical review letters.

[30]  B. Kammerling,et al.  Predictions for complete fragmentation patterns of 4d5/2 photoelectrons and N5-O23O23 1S0 Auger electrons of xenon based on experimental data at 94.5 eV photon energy , 1993 .

[31]  V. Schmidt Photoionization of atoms using synchrotron radiation , 1992 .

[32]  N. Kabachnik Angular correlation between photoelectron and Auger electron in two-step double photoionization of atoms , 1992 .

[33]  Schmidt,et al.  Complete fragmentation pattern for two-step double photoionization in xenon. , 1991, Physical review letters.

[34]  S. Sheinerman,et al.  Post-collision interaction in atomic processes , 1989 .

[35]  J. Briggs,et al.  Triply-differential cross sections for ionisation of hydrogen atoms by electrons and positrons , 1989 .

[36]  S. Sheinerman,et al.  Resonant scattering with low-velocity outgoing charged particles , 1988 .

[37]  T. Åberg A Scattering Approach to the Decay of Metastable States , 1980 .

[38]  H. P. Kelly,et al.  Double photoionization of neon and argon , 1977 .

[39]  R. T. Poe,et al.  Double photoionization of neon , 1975 .

[40]  I. I. Sobelʹman Introduction to the theory of atomic spectra , 1972 .