001     29175
005     20180210134034.0
024 7 _ |2 DOI
|a 10.1016/0009-2614(03)00770-X
024 7 _ |2 WOS
|a WOS:000183945900028
037 _ _ |a PreJuSER-29175
041 _ _ |a eng
082 _ _ |a 540
084 _ _ |2 WoS
|a Chemistry, Physical
084 _ _ |2 WoS
|a Physics, Atomic, Molecular & Chemical
100 1 _ |a Antol, I.
|b 0
|0 P:(DE-HGF)0
245 _ _ |a Valence and Rydberg states of protonated formaldehyde
260 _ _ |a Amsterdam [u.a.]
|b Elsevier
|c 2003
300 _ _ |a 587 - 593
336 7 _ |a Journal Article
|0 PUB:(DE-HGF)16
|2 PUB:(DE-HGF)
336 7 _ |a Output Types/Journal article
|2 DataCite
336 7 _ |a Journal Article
|0 0
|2 EndNote
336 7 _ |a ARTICLE
|2 BibTeX
336 7 _ |a JOURNAL_ARTICLE
|2 ORCID
336 7 _ |a article
|2 DRIVER
440 _ 0 |a Chemical Physics Letters
|x 0009-2614
|0 1200
|v 374
500 _ _ |a Record converted from VDB: 12.11.2012
520 _ _ |a MR-CISD and MR-CISD + Q calculations have been performed for the vertical excitations of protonated formaldehyde in comparison to formaldehyde. Singlet and triplet states have been investigated. It is shown that the protonation causes the Rydberg states to be shifted to higher energies by several eV. This finding is discussed by means of the Rydberg formula in terms of quantum defects for the two lowest vertical ionization energies. For protonated formaldehyde the pi-pi(*) valence state is energetically the second lowest state at 9.80 eV, about 1.50 eV below the first Rydberg n-3s state. This finding is in strong contrast to the case of formaldehyde where the pi-pi(*) state is embedded within a series of Rydberg states. (C) 2003 Elsevier Science B.V. All rights reserved.
536 _ _ |a Betrieb und Weiterentwicklung des Höchstleistungsrechners
|c I03
|2 G:(DE-HGF)
|0 G:(DE-Juel1)FUEK254
|x 0
588 _ _ |a Dataset connected to Web of Science
650 _ 7 |a J
|2 WoSType
700 1 _ |a Eckert-Maksic, M.
|b 1
|0 P:(DE-HGF)0
700 1 _ |a Müller, T.
|b 2
|u FZJ
|0 P:(DE-Juel1)132204
700 1 _ |a Dallos, M.
|b 3
|0 P:(DE-HGF)0
700 1 _ |a Lischka, H.
|b 4
|0 P:(DE-HGF)0
773 _ _ |a 10.1016/0009-2614(03)00770-X
|g Vol. 374, p. 587 - 593
|p 587 - 593
|q 374<587 - 593
|0 PERI:(DE-600)1466293-0
|t Chemical physics letters
|v 374
|y 2003
|x 0009-2614
856 7 _ |u http://dx.doi.org/10.1016/0009-2614(03)00770-X
909 C O |o oai:juser.fz-juelich.de:29175
|p VDB
913 1 _ |k I03
|v Betrieb und Weiterentwicklung des Höchstleistungsrechners
|l Wissenschaftliches Rechnen
|b Information
|0 G:(DE-Juel1)FUEK254
|x 0
914 1 _ |y 2003
915 _ _ |0 StatID:(DE-HGF)0010
|a JCR/ISI refereed
920 1 _ |k ZAM
|l Zentralinstitut für Angewandte Mathematik
|d 31.12.2007
|g ZAM
|0 I:(DE-Juel1)VDB62
|x 0
970 _ _ |a VDB:(DE-Juel1)25408
980 _ _ |a VDB
980 _ _ |a ConvertedRecord
980 _ _ |a journal
980 _ _ |a I:(DE-Juel1)JSC-20090406
980 _ _ |a UNRESTRICTED
981 _ _ |a I:(DE-Juel1)JSC-20090406


LibraryCollectionCLSMajorCLSMinorLanguageAuthor
Marc 21