Export citation

Export citation

Choose format for download:

Download Citation
  • Access by Xinjiang University

Multielectron coincidence spectroscopy of the Ar2+(2p2) double-core-hole decay

Maximilian Mailhiot1,7,*, Kari Jänkälä1, Marko Huttula1, Minna Patanen1, Klemen Bučar2, Matjaž Žitnik2, Denis Cubaynes3, Fabian Holzmeier4,†, Raimund Feifel5 et al.

Denis Céolin6, Lidija Andric7, Renaud Guillemin7, Iyas Ismail7, Jerome Palaudoux7, Francis Penent7, and Pascal Lablanquie7

  • 1Nano and Molecular Systems Research Unit (NANOMO), Faculty of Science, University of Oulu, P.O. Box 3000, FIN-90014 Oulu, Finland
  • 2J. Stefan Institute, Jamova 39, SI-1000 Ljubljana, Slovenia
  • 3Institut des Sciences Moléculaires d’Orsay, Centre National de la Recherche Scientifique, Bâtiment 520 Université Paris-Sud and Paris-Saclay, F-91405 Orsay Cedex, France
  • 4Dipartimento di Fisica, Politecnico di Milano, I-20133 Milano, Italy
  • 5University of Gothenburg, Department of Physics, SE-41258 Gothenburg, Sweden
  • 6Synchrotron SOLEIL, L'Orme des Merisiers, Départementale 128, F-91190 Saint-Aubin, France
  • 7Laboratoire de Chimie Physique Matière et Rayonnement, Sorbonne Université and Centre National de la Recherche Scientifique, F-75005 Paris, France

  • *Corresponding author: maximilian.mailhiot@oulu.fi
  • Present address: Imec, Kapeldreef 75, BE-3001 Leuven, Belgium.

Phys. Rev. A 107, 063108 – Published 23 June, 2023

DOI: https://doi.org/10.1103/PhysRevA.107.063108

Abstract

The dominant decay pathways of argon 2p2 double-core-hole states have been investigated using synchrotron radiation and a magnetic-bottle-type spectrometer coupled with an ion time-of-flight spectrometer. This experiment allows for efficient multi-electron-ion coincidence measurements, and thus for following the Auger cascade step by step in detail. Dominant decay pathways leading to Ar4+ final states via Ar3+ intermediate states have been assigned with the help of theoretical ab initio calculations. The weak correlated decay of the two core holes by emission of a single Auger electron, leading to Ar3+ final states, has been observed at 458.5-eV kinetic energy. Compared to the total decay of the 2p2 double core vacancies, this two-electron–one-electron process was measured to have a branching ratio of 1.9×103±1.0×103. Furthermore, the remaining decay paths of the Ar1+(1s1) core hole to higher charge states and their respective contributions to the total yield have been analyzed and show very good agreement with theoretical results.

Physics Subject Headings (PhySH)

Article Text

References (71)

  1. G. Charpak, Experimental study of the double ionization of the K shell of 55Mn in the disintegration of 55Fe by K-capture, C. R. Acad. Sci. 237, 243 (1953).
  2. J. Hoszowska, J. C. Dousse, W. Cao, K. Fennane, Y. Kayser, M. Szlachetko, J. Szlachetko, and M. Kavčič, Double K-shell photoionization and hypersatellite x-ray transitions of 12 ≤ Z ≤ 23 atoms, Phys. Rev. A 82, 063408 (2010).
  3. L. S. Cederbaum, F. Tarantelli, A. Sgamellotti, and J. Schirmer, On double vacancies in the core, J. Chem. Phys. 85, 6513 (1986).
  4. P. Lablanquie et al., Properties of Hollow Molecules Probed by Single-Photon Double Ionization, Phys. Rev. Lett. 106, 063003 (2011).
  5. M. Nakano et al., Single Photon K2 and K1K1 Double Core Ionization in C2H2n (N=13 ), CO, and N2 As a Potential New Tool for Chemical Analysis, Phys. Rev. Lett. 110, 163001 (2013).
  6. L. Hedin, M. Tashiro, P. Linusson, J. H. D. Eland, M. Ehara, K. Ueda, V. Zhaunerchyk, L. Karlsson, K. Pernestål, and R. Feifel, N1s and O1s double ionization of the NO and N2O molecules, J. Chem. Phys. 140, 44309 (2014).
  7. M. Tashiro, M. Nakano, M. Ehara, F. Penent, L. Andric, J. Palaudoux, K. Ito, Y. Hikosaka, N. Kouchi, and P. Lablanquie, Auger decay of molecular double core-hole and its satellite states: Comparison of experiment and calculation, J. Chem. Phys. 137, 224306 (2012).
  8. S. Carniato et al., Double-core ionization photoelectron spectroscopy of C6H6: Breakdown of the “intuitive” ortho-meta-para binding energy ordering of K1K1 states, J. Chem. Phys. 151, 214303 (2019).
  9. S. Carniato et al., Single photon simultaneous K-shell ionization/excitation in C6H6: experiment and theory, J. Phys. B 53, 244010 (2020).
  10. L. S. Cederbaum, F. Tarantelli, A. Sgamellotti, and J. Schirmer, Double vacancies in the core of benzene, J. Chem. Phys. 86, 2168 (1987).
  11. F. Penent et al., Double core hole spectroscopy with synchrotron radiation, J. Electron. Spectros. Relat. Phenom. 204, 303 (2015).
  12. P. Lablanquie, F. Penent, and Y. Hikosaka, Multi-electron coincidence spectroscopy: Double photoionization from molecular inner-shell orbitals, J. Phys. B 49, 182002 (2016).
  13. M. Nakano, P. Selles, P. Lablanquie, Y. Hikosaka, F. Penent, E. Shigemasa, K. Ito, and S. Carniato, Near-Edge X-Ray Absorption Fine Structures Revealed in Core Ionization Photoelectron Spectroscopy, Phys. Rev. Lett. 111, 123001 (2013).
  14. S. Carniato et al., Single photon simultaneous K-shell ionization and K-shell excitation. I. Theoretical model applied to the interpretation of experimental results on H2O, J. Chem. Phys. 142, 014307 (2015).
  15. S. Carniato et al., Single photon simultaneous K-shell ionization and K-shell excitation. II. Specificities of hollow nitrogen molecular ions, J. Chem. Phys. 142, 014308 (2015).
  16. S. Carniato et al., Photon-energy dependence of single-photon simultaneous core ionization and core excitation in CO2, Phys. Rev. A 94, 013416 (2016).
  17. L. Journel, D. Cubaynes, J.-M. Bizau, S. Al Moussalami, B. Rouvellou, F. J. Wuilleumier, L. VoKy, P. Faucher, and A. Hibbert, First Experimental Determination and Theoretical Calculation of Partial Photoionization Cross Sections of Lithium over the Energy Region of Hollow Atomic States, Phys. Rev. Lett. 76, 30 (1996).
  18. S. Diehl et al., Hollow-atom-hollow-ion decay routes of triply excited lithium: First Auger results and a comparison with R-matrix calculations, J. Phys. B 30, L595 (1997).
  19. S. Diehl, D. Cubaynes, J. M. Bizau, F. J. Wuilleumier, E. T. Kennedy, J. P. Mosnier, and T. J. Morgan, New high-resolution measurements of doubly excited states of Li+, J. Phys. B 32, 4193 (1999).
  20. L. M. Kiernan, E. T. Kennedy, J.-P. Mosnier, J. T. Costello, and B. F. Sonntag, First Observation of a Photon-Induced Triply Excited State in Atomic Lithium, Phys. Rev. Lett. 72, 2359 (1994).
  21. G. Goldsztejn et al., Double-Core-Hole States in Neon: Lifetime, Post-Collision Interaction, and Spectral Assignment, Phys. Rev. Lett. 117, 133001 (2016).
  22. G. Goldsztejn et al., Experimental and theoretical study of the double-core-hole hypersatellite Auger spectrum of Ne, Phys. Rev. A 96, 012513 (2017).
  23. R. Püttner et al., Argon 1s2 Auger hypersatellites, J. Phys. B 54, 024001 (2020).
  24. D. Koulentianos et al., KL double core hole pre-edge states of HCl, Phys. Chem. Chem. Phys. 20, 2724 (2018).
  25. A. Perry-Sassmannshausen et al., Multiple Photodetachment of Carbon Anions Via Single and Double Core-Hole Creation, Phys. Rev. Lett. 124, 083203 (2020).
  26. S. Schippers, A. Hamann, A. Perry-Sassmannshausen, T. Buhr, A. Müller, M. Martins, S. Reinwardt, F. Trinter, and S. Fritzsche, Multiple photodetachment of oxygen anions via K-Shell excitation and ionization: direct double-detachment processes and subsequent deexcitation cascades, Phys. Rev. A 106, 013114 (2022).
  27. A. Müller, M. Martins, A. Borovik, T. Buhr, A. Perry-Sassmannshausen, S. Reinwardt, F. Trinter, S. Schippers, S. Fritzsche, and A. S. Kheifets, Role of L-Shell Single and Double Core-Hole Production and Decay in m-Fold (1m6) Photoionization of the Ar+ Ion, Phys. Rev. A 104, 033105 (2021).
  28. N. Berrah et al., Double-core-hole spectroscopy for chemical analysis with an intense x-ray femtosecond laser, Proc. Natl. Acad. Sci. USA 108, 16912 (2011).
  29. L. Young et al., Femtosecond electronic response of atoms to ultra-intense x-rays, Nature (London) 466, 56 (2010).
  30. P. Salén et al., Experimental Verification of the Chemical Sensitivity of Two-Site Double Core-Hole States Formed by an x-Ray Free-Electron Laser, Phys. Rev. Lett. 108, 153003 (2012).
  31. L. J. Frasinski et al., Dynamics of Hollow Atom Formation in Intense X-Ray Pulses Probed by Partial Covariance Mapping, Phys. Rev. Lett. 111, 073002 (2013).
  32. L. Asplund, P. Kelfve, B. Blomster, H. Siegbahn, and K. Siegbahn, Argon KLL and KLM Auger electron spectra, Phys. Scr. 16, 268 (1977).
  33. G. Omar and Y. Hahn, Final charge state distribution in the production and decay of hollow Ar, Z. Phys. D 25, 41 (1992).
  34. R. Guillemin, C. Bomme, T. Marin, L. Journel, T. Marchenko, R. K. Kushawaha, N. Trcera, M. N. Piancastelli, and M. Simon, Complex decay patterns in atomic core photoionization disentangled by ion-recoil measurements, Phys. Rev. A 84, 063425 (2011).
  35. R. Guillemin, S. Sheinerman, C. Bomme, L. Journel, T. Marin, T. Marchenko, R. K. Kushawaha, N. Trcera, M. N. Piancastelli, and M. Simon, Ultrafast Dynamics in Postcollision Interaction after Multiple Auger Decays in Argon 1s Photoionization, Phys. Rev. Lett. 109, 013001 (2012).
  36. R. Guillemin et al., Interplay of complex decay processes after argon 1s ionization, Phys Rev A 97, 013418 (2018).
  37. X. L. Wang, B. X. Liu, G. H. Zhang, P. Y. Wang, L. W. Liu, and X. Y. Li, Theoretical studies on the cascade decay processes of 1s-core-hole state of Ar ion, J. Electron. Spectros. Relat. Phenom. 250, 147083 (2021).
  38. A. O. G. Wallis, H. I. B. Banks, and A. Emmanouilidou, Traces in ion yields and electron spectra of the formation of Ar inner-shell hollow states by free-electron lasers, Phys. Rev. A 91, 063402 (2015).
  39. T. D. Thomas, Single and double core-hole ionization energies in molecules, J. Phys. Chem. A 116, 3856 (2012).
  40. J. P. Rueff, J. M. Ablett, D. Céolin, D. Prieur, T. Moreno, V. Balédent, B. Lassalle-Kaiser, J. E. Rault, M. Simon, and A. Shukla, The GALAXIES beamline at the SOLEIL synchrotron: Inelastic x-ray scattering and photoelectron spectroscopy in the hard x-ray range, J. Synchrotron Radiat. 22, 175 (2015).
  41. D. Céolin et al., Hard x-ray photoelectron spectroscopy on the GALAXIES beamline at the SOLEIL synchrotron, J. Electron. Spectros. Relat. Phenom. 190, 188 (2013).
  42. J. H. D. Eland, O. Vieuxmaire, T. Kinugawa, P. Lablanquie, R. I. Hall, and F. Penent, Complete Two-Electron Spectra in Double Photoionization: The Rare Gases Ar, Kr, and Xe, Phys. Rev. Lett. 90, 053003 (2003).
  43. F. Penent, J. Palaudoux, P. Lablanquie, L. Andric, R. Feifel, and J. H. D. Eland, Multielectron Spectroscopy: The Xenon 4d Hole Double Auger Decay, Phys. Rev. Lett. 95, 083002 (2005).
  44. I. Ismail et al., A modified magnetic bottle electron spectrometer for the detection of multiply charged ions in coincidence with all correlated electrons: Decay pathways to Xe3+ above xenon-4d ionization threshold, Phys. Chem. Chem. Phys. 24, 20219 (2022).
  45. K. Ito, F. Penent, Y. Hikosaka, E. Shigemasa, I. H. Suzuki, J. H. D. Eland, and P. Lablanquie, Application of a simple asynchronous mechanical light chopper to multielectron coincidence spectroscopy, Rev. Sci. Instrum. 80, 123101 (2009).
  46. M. Breinig, M. H. Chen, G. E. Ice, F. Parente, B. Crasemann, and G. S. Brown, Atomic inner-shell level energies determined by absorption spectrometry with synchrotron radiation, Phys Rev A 22, 520 (1980).
  47. H. Pulkkinen, S. Aksela, O.-P. Sairanen, A. Hiltunen, and H. Aksela, Correlation effects in the L 2,3-MM Auger transitions of Ar, J. Phys. B: At. Mol. Opt. Phys. 29, 3033 (1996).
  48. K. Bučar and M. Žitnik, Auger electron–ion coincidence spectrometry after electronic excitation of L-shell in argon, Radiat. Phys. Chem. 76, 487 (2007).
  49. M. F. Gu, The flexible atomic code, Can. J. Phys. 86, 675 (2008).
  50. K. G. Dyall, I. P. Grant, C. T. Johnson, F. A. Parpia, and E. P. Plummer, GRASP: A general-purpose relativistic atomic structure program, Comput. Phys. Commun. 55, 425 (1989).
  51. S. Fritzsche, C. F. Fischer, and G. Gaigalas, RELCI: A program for relativistic configuration interaction calculations☆☆this program can be downloaded from the CPC program library under catalogue identifier: http://Cpc.Cs.Qub.Ac.Uk/Summaries/ADQH, Comput. Phys. Commun. 148, 103 (2002).
  52. S. H. Southworth, T. LeBrun, Y. Azuma, and K. G. Dyall, Argon KM photoelectron satellites, J. Electron. Spectros. Relat. Phenom. 94, 33 (1998).
  53. P. Lablanquie, L. Andric, J. Palaudoux, U. Becker, M. Braune, J. Viefhaus, J. H. D. Eland, and F. Penent, and Multielectron spectroscopy: Auger decays of the argon 2p hole, J. Electron. Spectros. Relat. Phenom. 156, 51 (2007).
  54. R. Püttner et al., Argon KLL Auger spectrum: Initial states, core-hole lifetimes, shake, and knock-down processes, Phys. Rev. A 102, 052832 (2020).
  55. M. O. Krause, Atomic radiative and radiationless yields for K and L shells, J. Phys. Chem. Ref. Data 8, 307 (1979).
  56. F. von Busch, U. Kuetgens, J. Doppelfeld, and S. Fritzsche, L23[L23]MM[L23] and L23[M2]MM[M2] Auger vacancy satellite spectra of argon, Phys. Rev. A 59, 2030 (1999).
  57. R. D. Deslattes, E. G. Kessler, Jr., P. Indelicato, L. de Billy, E. Lindroth, J. Anton, J. S. Coursey, D. J. Schwab, C. Chang, R. Sukumar, K. Olsen, and R. A. Dragoset, X-ray transition energies ver. 1.2, http://physics.nist.gov/XrayTrans.
  58. M. H. Chen, B. Crasemann, and H. Mark, Relativistic radiationless transition probabilities for atomic K- and L-shells, At. Data Nucl. Data Tables 24, 13 (1979).
  59. J. C. Levin, C. Biedermann, N. Keller, L. Liljeby, C.-S. O, R. T. Short, R. T. Short, I. A. Sellin, and D. W. Lindle, Argon-Photoion–Auger-Electron Coincidence Measurements Following K-Shell Excitation by Synchrotron Radiation, Phys. Rev. Lett. 65, 988 (1990).
  60. S. M. Huttula, P. Lablanquie, L. Andric, J. Palaudoux, M. Huttula, S. Sheinerman, E. Shigemasa, Y. Hikosaka, K. Ito, and F. Penent, Decay of a 2p Inner-Shell Hole in an Ar+ Ion, Phys. Rev. Lett. 110, 113002 (2013).
  61. A. G. Kochur, Final-ion-charge spectra produced by cascading decay of hollow argon and krypton atoms, J. Electron. Spectros. Relat. Phenomena 114, 81 (2001).
  62. M. Žitnik et al., Two-to-one Auger decay of a double L vacancy in argon, Phys Rev A 93, 021401(R) (2016).
  63. F. von Busch, J. Doppelfeld, C. Gunther, and E. Hartmann, Argon L23-MM Auger satellite spectrum emitted after K ionization, J. Phys. B 27, 2151 (1994).
  64. P. Linusson, S. Fritzsche, J. H. D. Eland, M. Mucke, and R. Feifel, Single-photon multiple ionization forming double vacancies in the 2p subshell of argon, Phys. Rev. A 87, 043409 (2013).
  65. A. Kramida, Y. Ralchenko, J. Reader and NIST ASD Team (2022), NIST Atomic Spectra Database Ver. 5.8 (National Institute of Standards and Technology, Gaithersburg, MD, 2023), https://physics.nist.gov/asd.
  66. E. B. Saloman, Energy levels and observed spectral lines of ionized argon, Ar II through Ar XVIII, J. Phys. Chem. Ref. Data 39, 033101 (2010).
  67. I. Velchev, W. Hogervorst, and W. Ubachs, Precision VUV spectroscopy of Ar I at 105 Nm, J. Phys. B 32, L511 (1999).
  68. J. E. Sansonetti and W. C. Martin, Handbook of basic atomic spectroscopic data, J. Phys. Chem. Ref. Data 34, 1559 (2005).
  69. V. Kaufman and W. Whaling, Improved wavelengths and energy levels of doubly-ionized argon (Ar III), J. Res. Natl. Inst. Stand. Technol. 101, 691 (1996).
  70. E. Biémont, Y. Frémat, and P. Quinet, Ionization potentials of atoms and ions from lithium to tin (Z=50), At. Data Nucl. Data Tables 71, 117 (1999).
  71. S. Bashkin and J. O. Stoner, Atomic Energy Levels and Grotrian Diagrams: Hydrogen I–Phosphorus XV (Elsevier, Amsterdam, 2013).

Outline

Information

Sign In to Your Journals Account

Filter

Filter

Article Lookup

Enter a citation