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Volumn 113, Issue 7, 2009, Pages 1308-1317

Structure, bonding, and relative stability of the ground and low-lying electronic states of CuO2. the role of exact exchange

Author keywords

[No Author keywords available]

Indexed keywords

CCSD; COMPLETE BASIS SET LIMITS; DENSITY FUNCTIONALS; DFT METHODS; EXACT EXCHANGES; FUNCTIONALS; HARTREE-FOCK; LOW-LYING ELECTRONIC STATE; LOW-LYING STATE; RELATIVE ENERGIES; RELATIVE STABILITIES; STANDARD DEVIATIONS;

EID: 63849286577     PISSN: 10895639     EISSN: None     Source Type: Journal    
DOI: 10.1021/jp8031379     Document Type: Article
Times cited : (18)

References (93)
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    • Frisch, M. J.; Trucks, G. W.; Schlegel, H. B.; Scuseria, G. E.; Robb, M. A.; Cheeseman, J. R.; Montgomery J. A., Jr.; Vreven, T.; Kudin, K. N.; Burant, J. C.; Millam, J. M.; Iyengar, S. S.; Tomasi, J.; Barone, V.; Mennucci, B.; Cossi, M.; Scalmani, G.; Rega, N.; Petersson, G. A.; Nakatsuji, H.; Hada, M.; Ehara, M.; Toyota, K.; Fukuda, R.; Hasegawa, J.; Ishida, M.; Nakajima, T.; Honda, Y.; Kitao, O.; Nakai, H.; Klene, M.; Li, X.; Knox, J. E.; Hratchian, H. P.; Cross, J. B.; Bakken, V.; Adamo, C.; Jaramillo, J.; Gomperts, R.; Stratmann, R. E.; Yazyev, O.; Austin, A. J.; Cammi, R.; Pomelli, C; Ochterski, J. W.; Ayala, P. Y.; Morokuma, K.; Voth, G. A.; Salvador, P.; Dannenberg, J. J.; Zakrzewski, G.; Dapprich, S.; Daniels, A. D.; Strain, M. C.; Farkas, O.; Malick, D. K.; Rabuck, A. D.; Raghavachari, K.; Foresman, J. B.; Ortiz, J. V.; Cui, Q.; Baboul, A. G.; Clifford, S.; Cioslowski, J.; Stefanov, B. B.; Liu, G.; Liashenko, A.; Piskorz, P.; Komaromi, I.; Martin, R. L.; Fox, D. J.; Keith, T.; Al-Laham, M. A.; Peng, C. Y.; Nanayakkara, A.; Challacombe, M.; Gill, P. M. W.; Johnson, B.; Chen, W.; Wong, M. W.; Gonzalez, C.; Pople, J. A. Gaussian 03, revision C.01; Gaussian, Inc.: Pittsburgh, PA, 2003.
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    • Werner, H.-J, Knowles, P. J, Lindh, R, Manby, F. R, Schütz, M. MOLPRO, version 2006.1, a package of ab initio programs, 2006
    • Werner, H.-J.; Knowles, P. J.; Lindh, R.; Manby, F. R.; Schütz, M. MOLPRO, version 2006.1, a package of ab initio programs, 2006.
  • 67
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    • In the Gaussian 03 implementation of the Cu basis set, the s and p functions come from Wachter's optimization for the Cu atom in its 2S state, while the d functions come from Wachter's optimization for the Cu atom in its 2D state. In addition, we have checked that with the B3LYP method the Gaussian 03 internal basis set provides more reasonable results for the relative energies among the different analyzed states than the basis set with the d functions coming from Wachter's optimization for the Cu atom in its 2D state
    • 2D state.
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.