Comparison of different quantum mechanical methods for inner atomic shell photo-ionization followed by Auger decay

A numerical time-dependent quantum mechanical approach was developed previously for simulating the process of photoionization followed by Auger decay for cases where the photoelectron energy is not very large; the method accurately calculates the interaction between the two active electrons, but simplifies their interaction with the core electrons. More established theoretical methods, which take account of postcollision interaction effects, allow an accurate description of this process when the photoelectron energy is not too low. We demonstrate that using the time-dependent method (although with some simplifications that are needed for its numerical implementation) for low energy photoelectrons and more established methods for higher energy allows accurate calculations for nearly all possible combinations of electron energy. This is confirmed by performing calculations of the photoelectron energy and angular distributions for the 1 s photoionization of Ne, with a subsequent KLL Auger transition. By computing the energy and angular distributions for energies where the two groups of methods should agree and where they should disagree, we demonstrate their consistency and range of accuracy. For the regions where the methods disagree, we discuss the reasons for any discrepancies and the trends in the differences. In addition, some of our calculations are compared with existing experimental data for the same system. The agreement found in the comparison confirms the reliability of the theoretical approaches.

[1]  V. D. Mur,et al.  Current progress in developing the nonlinear ionization theory of atoms and ions , 2015 .

[2]  M. Schöffler,et al.  Calculated and measured angular correlation between photoelectrons and Auger electrons from K-shell ionization , 2012 .

[3]  D. Hochstuhl,et al.  Time-dependent restricted-active-space configuration-interaction method for the photoionization of many-electron atoms , 2012, 1207.5693.

[4]  F. Robicheaux Time propagation of extreme two-electron wavefunctions , 2012 .

[5]  M. Piancastelli,et al.  Ultrafast dynamics in postcollision interaction after multiple auger decays in argon 1s photoionization. , 2012, Physical review letters.

[6]  L. Gerchikov Post-collision-interaction distortion of low-energy photoelectron spectra associated with double Auger decay , 2011 .

[7]  D. Hochstuhl,et al.  Two-photon ionization of helium studied with the multiconfigurational time-dependent Hartree-Fock method. , 2010, The Journal of chemical physics.

[8]  T. Kaneyasu,et al.  PCI effects in argon 2p double Auger decay probed by multielectron coincidence methods , 2010 .

[9]  M. Schöffler,et al.  Angular correlation between photoelectrons and auger electrons from K-shell ionization of neon. , 2009, Physical review letters.

[10]  P. Lablanquie,et al.  Multi-coincidence in cascade Auger decay processes , 2008 .

[11]  D. C. Griffin,et al.  The time-dependent close-coupling method for atomic and molecular collision processes , 2007 .

[12]  K. Ito,et al.  Electron correlation in Xe 4d Auger decay studied by slow photoelectron–Auger electron coincidence spectroscopy , 2006 .

[13]  R. Feifel,et al.  Multielectron spectroscopy: the xenon 4d hole double auger decay. , 2005, Physical review letters.

[14]  K. Ueda,et al.  A study of photoelectron recapture due to post-collision interaction in Ne at the 1s photoionization threshold , 2005 .

[15]  S. Sheinerman PCI effects in resonant processes of photo double electron emission near the Ne 1s threshold , 2005 .

[16]  H. Tanaka,et al.  Investigation of valence inter-multiplet Auger transitions in Ne following 1s photoelectron recapture , 2005 .

[17]  Hiroshi Tanaka,et al.  Photoelectron recapture as a tool for the spectroscopy of ionic Rydberg states , 2004 .

[18]  V. Schmidt,et al.  Angle-dependent decrease of transition probability in sequential photo double-ionization , 2004 .

[19]  S. Sheinerman Capture and re-emission of slow photoelectrons in Ar 2p6-subshell photoionization processes , 2003 .

[20]  L. Avaldi,et al.  Experimental observation of post-collision interaction and interference effects in resonant double photoionization processes. , 2001, Physical review letters.

[21]  V. Schmidt,et al.  Interference, post-collision interaction and exchange effects in angular distribution patterns of resonant photo double-ionization in neon for equal electron energies , 1999 .

[22]  P. Feulner,et al.  Substrate Mediated Suppression of Postcollision Interaction Effects , 1998 .

[23]  J. Levin,et al.  POSTCOLLISION-INTERACTION RECAPTURE OF PHOTOELECTRONS AND ZERO-KINETIC-ENERGY ELECTRON EMISSION : A QUANTUM MODEL , 1997 .

[24]  Bolognesi,et al.  Observation of Angle Dependent Postcollision Interaction in the Electron Impact Ionization of Xe 4d5/2. , 1995, Physical review letters.

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

[26]  B. Kammerling,et al.  Angle-dependent post-collision interaction in inner-shell photoionization of xenon , 1993 .

[27]  M. Keane,et al.  Observation of anisotropic PCI effects at high excess energies , 1992 .

[28]  Berg,et al.  Quantum approach to photoelectron recapture in post-collision interaction. , 1990, Physical review. A, Atomic, molecular, and optical physics.

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

[30]  Whitfield,et al.  Photoelectron recapture through post-collision interaction. , 1988, Physical review. A, General physics.

[31]  F. Koike Theory of post-collision interaction at high excess energies , 1988 .

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

[33]  A. Niehaus,et al.  Angular dependent post-collision interaction in auger processes , 1988 .

[34]  B. Crasemann,et al.  Quantum theory of post-collision interaction in inner-shell photoionization: Final-state interaction between two continuum electrons. , 1987 .

[35]  B. Crasemann,et al.  Quantum theory of post-collision interaction in inner-shell photoionization , 1987, Physical review. A, General physics.

[36]  W. Mehlhorn,et al.  Post-collision interaction and the Auger lineshape , 1986 .

[37]  S. Sheinerman,et al.  The post collision interaction in the inner-shell photoionisation of Ar and Xe , 1985 .

[38]  J. Mizuno,et al.  Energy exchange between two outgoing electrons in the post-collision interaction process , 1985 .

[39]  G. Ogurtsov Auger line shift due to the post-collision interaction at large excess energies , 1983 .

[40]  K. Siegbahn,et al.  An Improved Model for Post-Collision Interaction (PCI) and High Resolution Ar LMM Auger Spectra Revealing New PCI Effects , 1983 .

[41]  R. L. Watson,et al.  Post-collision interaction in the selenium L/sub 2/M/sub 4,5/M/sub 4,5/ Auger spectrum following photoionization , 1979 .

[42]  S. Sheinerman,et al.  Inter-shell correlations in the formation of singly charged ions near the Ar L-shell ionisation threshold , 1977 .

[43]  A. Niehaus Analysis of post-collision interactions in Auger processes following near-threshold inner-shell photoionization , 1977 .

[44]  F. Wuilleumier,et al.  Post-Collision Interaction in the Xenon N 4,5 -OO Auger Spectrum Excited by Photon Impact , 1977 .

[45]  M. V. D. Wiel,et al.  Post-collision interaction in L-shell ionization of Ar , 1976 .

[46]  F. Read Displaced electron energies and the "shake-down" effect. , 1975, Radiation research.

[47]  F. H. Read,et al.  Structure near autoionizing energies in the excitation of bound states of helium, neon and argon by electron impact , 1975 .

[48]  H. W. Berry,et al.  Electron Energy Distributions from Ionizing Collisions of Helium and Neon Ions with Helium , 1966 .