N1s and O1s double ionization of the NO and N2O molecules.

Single-site N1s and O1s double core ionisation of the NO and N2O molecules has been studied using a magnetic bottle many-electron coincidence time-of-flight spectrometer at photon energies of 1100 eV and 1300 eV. The double core hole energies obtained for NO are 904.8 eV (N1s(-2)) and 1179.4 eV (O1s(-2)). The corresponding energies obtained for N2O are 896.9 eV (terminal N1s(-2)), 906.5 eV (central N1s(-2)), and 1174.1 eV (O1s(-2)). The ratio between the double and single ionisation energies are in all cases close or equal to 2.20. Large chemical shifts are observed in some cases which suggest that reorganisation of the electrons upon the double ionization is significant. Δ-self-consistent field and complete active space self-consistent field (CASSCF) calculations were performed for both molecules and they are in good agreement with these results. Auger spectra of N2O, associated with the decay of the terminal and central N1s(-2) as well as with the O1s(-2) dicationic states, were extracted showing the two electrons emitted as a result of filling the double core holes. The spectra, which are interpreted using CASSCF and complete active space configuration interaction calculations, show atomic-like character. The cross section ratio between double and single core hole creation was estimated as 1.6 × 10(-3) for nitrogen at 1100 eV and as 1.3 × 10(-3) for oxygen at 1300 eV.

[1]  C. Bostedt,et al.  Experimental verification of the chemical sensitivity of two-site double core-hole states formed by an x-ray free-electron laser. , 2012, Physical review letters.

[2]  Masahiro Ehara,et al.  Double-core-hole spectroscopy for chemical analysis with an intense X-ray femtosecond laser , 2011, Proceedings of the National Academy of Sciences.

[3]  M. Ehara,et al.  Auger decay of molecular double core-hole state. , 2011, The Journal of chemical physics.

[4]  R. Feifel,et al.  Structure sensitivity of double inner-shell holes in sulfur-containing molecules , 2011 .

[5]  M. Zitnik,et al.  Properties of hollow molecules probed by single-photon double ionization. , 2011, Physical review letters.

[6]  M. Ehara,et al.  Double core hole creation and subsequent Auger decay in NH3 and CH4 molecules. , 2010, Physical review letters.

[7]  M. Ehara,et al.  Double core–hole electron spectroscopy for open-shell molecules: Theoretical perspective , 2010, 1007.0530.

[8]  Masahiro Ehara,et al.  Molecular double core-hole electron spectroscopy for chemical analysis , 2010, 1004.3092.

[9]  R. Santra,et al.  X-ray two-photon photoelectron spectroscopy: a theoretical study of inner-shell spectra of the organic para-aminophenol molecule. , 2009, Physical review letters.

[10]  J. Eland,et al.  Double photoionisation spectra of small molecules and a new empirical rule for double ionisation energies , 2007 .

[11]  R. Feifel,et al.  Complete valence double photoionization of SF6. , 2005, The Journal of chemical physics.

[12]  P. Lablanquie,et al.  Complete two-electron spectra in double photoionization: the rare gases Ar, Kr, and Xe. , 2003, Physical review letters.

[13]  M. Mitani,et al.  Theoretical molecular Auger spectra with electron population analysis , 2003 .

[14]  J. Tennyson,et al.  The UK molecular R-matrix codes , 1998 .

[15]  T. H. Dunning Gaussian basis sets for use in correlated molecular calculations. I. The atoms boron through neon and hydrogen , 1989 .

[16]  Lorenz S. Cederbaum,et al.  On double vacancies in the core , 1986 .

[17]  P. Knowles,et al.  A second order multiconfiguration SCF procedure with optimum convergence , 1985 .

[18]  P. Knowles,et al.  An efficient second-order MC SCF method for long configuration expansions , 1985 .

[19]  Pieter Kruit,et al.  Magnetic field paralleliser for 2π electron-spectrometer and electron-image magnifier , 1983 .

[20]  W. L. Jolly,et al.  A table of absolute core-electron binding-energies for gaseous atoms and molecules , 1980 .

[21]  G. Wentzel Über strahlungslose Quantensprünge , 1927 .