@article {471,
	title = {Theoretical Auger electron spectra of polymers by density functional theory calculations using model dimers},
	journal = {Journal of Computational Chemistry},
	volume = {23},
	number = {3},
	year = {2002},
	note = {ISI Document Delivery No.: 516HWTimes Cited: 2Cited Reference Count: 36},
	month = {Feb},
	pages = {394-401},
	type = {Article},
	abstract = {We propose a new approach for analysis of Auger electron spectra (AES) of polymers by density functional theory (DFT) calculations with the Slater{\textquoteright}s transition-state concept. Simulated AES and X-ray photoelectron spectra (XPS) of four polymers [(CH2CH2)(n) (PE), (CH2CH(CH3))(n) (PP), (CH2CH(OCH3))(n) (PVME), and (CH2CH(COCH3))(n) (PVMK)] by DFT calculations using model dimers are in a good accordance with the experimental ones. The experimental AES of the polymers can be classified in each range of ls-2p2p, 1s-2s2p, and 1s-2s2s transitions for CKVV and OKVV spectra, and in individual contributions of the functional groups from the theoretical analysis. (C) 2002 John Wiley Sons, Inc.},
	keywords = {AES, APPROXIMATION, BINDING-ENERGIES, C1S SPECTRA, DFT calculations, LINE-SHAPES, MOLECULES, OLIGOMERS, polymer, RAY PHOTOELECTRON-SPECTRA, SIO2, XPS},
	isbn = {0192-8651},
	url = {<Go to ISI>://000173548700008},
	author = {Otsuka, T. and Koizumi, S. and Endo, K. and Kawabe, H. and Chong, D. P.}
}
@article {5058,
	title = {Analysis of XPS and XES of diamond and graphite by DFT calculations using model molecules},
	journal = {Journal of Computational Chemistry},
	volume = {22},
	number = {1},
	year = {2001},
	note = {ISI Document Delivery No.: 384EGTimes Cited: 6Cited Reference Count: 31},
	month = {Jan},
	pages = {102-108},
	type = {Article},
	abstract = {X-ray photoelectron and emission spectra (XPS and XES) of diamond and graphite have been analyzed by deMon density-functional theory (DFT) calculations using the model adamantane derivative (C10H12(CH3)(4)) and pyrene (C16H10) molecules, respectively. The theoretical valence photoelectron and C K alpha X-ray emission spectra for the allotrope are in good accordance with the experimental ones. The combined analysis of the valence XPS and C K alpha XES enables us to divide the valence electronic distribution into the individual contributions for p sigma-, and p pi -bonding MOs of the diamond and graphite, respectively. (C) 2000 John Wiley \& Sons, Inc.},
	keywords = {APPROXIMATION, carbon allotrope, combined analysis of XPS and XES, DENSITY-FUNCTIONAL CALCULATION, DFT calculations, ELECTRON BINDING-ENERGIES, POLYMERS, RAY PHOTOELECTRON-SPECTRA, SILICON},
	isbn = {0192-8651},
	url = {<Go to ISI>://000165929000009},
	author = {Endo, K. and Koizumi, S. and Otsuka, T. and Suhara, M. and Morohasi, T. and Kurmaev, E. Z. and Chong, D. P.}
}
@article {5059,
	title = {Theoretical X-ray photoelectron and emission spectra of Si- and S-containing polymers by density-functional theory calculations using model molecules},
	journal = {Journal of Molecular Structure},
	volume = {561},
	number = {1-3},
	year = {2001},
	note = {ISI Document Delivery No.: 420KQTimes Cited: 5Cited Reference Count: 29},
	month = {Apr},
	pages = {17-28},
	type = {Article},
	abstract = {The X-ray photoelectron and emission spectra (XPS and XES) of Si- and S-containing polymers [(-Si{-CH2-}(3))(n) (PCS), (-Si(CH3)(OH)-O-)(n) (PMHSO), (-Si(C6H5)(OH)-O-)(n) (PTES), (-Si(C6H5)(OH)-O-Si(CH3)(OH)-O-)(n) (PPMHSO), (-C6H4-O-C6H4-SO2-)(n) (PES)] were simulated by the deMon density-functional theory (DFT) calculations using the model molecules. The theoretical valence photoelectron and C K alpha X-ray emission spectra showed good accordance with some experimental ones. The combined analysis of the valence XPS and C and O K alpha XES enables us to divide the observed valence electronic distribution into the individual contributions for p sigma-, p pi- and non-bonding MOs of the polymers. (C) 2001 Elsevier Science B.V. All rights reserved.},
	keywords = {APPROXIMATION, C1S SPECTRA, CK alpha XES, DFT calculations, ELECTRONIC STATES, ENERGY, FILMS, FLUORESCENCE, OLIGOMERS, POLYMERS, SPECTROSCOPY, XPS},
	isbn = {0022-2860},
	url = {<Go to ISI>://000168004500002},
	author = {Endo, K. and Shimada, S. and Ida, T. and Suhara, M. and Kurmaev, E. Z. and Moewes, A. and Chong, D. P.}
}
@article {4391,
	title = {Valence orbital electron momentum distributions for oxygen: comparison of EMS measurements with theory},
	journal = {Chem. Phys.},
	volume = {230},
	number = {2-3},
	year = {1998},
	note = {ISI Document Delivery No.: ZR243Times Cited: 19Cited Reference Count: 72},
	month = {May},
	pages = {153-186},
	type = {Article},
	abstract = {<p>The valence shell binding energy spectra and orbital electron momentum profiles of O-2 have been measured by energy dispersive multichannel electron momentum spectroscopy at an impact energy of 1200 eV + binding energy. The effects of electron correlation on the valence binding energy spectrum are investigated using multi-reference singles and doubles configuration interaction calculations. The presently reported experimental momentum profiles of O-2 display considerably improved statistics compared with previously published EMS results. The measured momentum profiles are compared with cross sections calculated using both unrestricted and restricted open shell Hartree-Fock methods with basis sets ranging from minimal to near Hartree-Fock limit in quality. In addition, the effects of correlation and relaxation on the calculated momentum profiles are investigated using multi-reference singles and doubles configuration interaction calculations of the full ion-neutral overlap distributions. Electron correlation effects in the ground state are further examined using several density functional approaches for the momentum profiles. The present EMS measurements and MRSD-CI calculations clearly show that the binding energy peak at similar to 27.3 eV has significant contributions from both (4) Sigma(u)(-) and (2) Sigma(u)(-) processes in contrast to earlier assignments which have attributed this peak to the C-2 Sigma(u)(-) State alone. Similarly, the binding energy peak at 33 eV is shown to be due to (2) Sigma(u)(-) rather than earlier assignments of (2) Pi(u) character. (C) 1998 Elsevier Science B.V. All rights reserved.</p>},
	keywords = {CALCULATIONS, CONFIGURATION-INTERACTION CALCULATIONS, CORRELATED MOLECULAR, CORRELATION ENERGIES, DENSITY-FUNCTIONAL THEORY, DFT calculations, GAUSSIAN-BASIS SETS, HARTREE-FOCK LIMIT, OPEN-SHELL MOLECULES, PHOTOELECTRON-SPECTROSCOPY, PHOTOIONIZATION CROSS-SECTIONS},
	isbn = {0301-0104},
	url = {<Go to ISI>://000073954600002},
	author = {Rolke, J. and Zheng, Y. and C. E. Brion* and Wang, Y. A. and Davidson, E. R.}
}
