Computational Evidence of Inversion of (1)La and (1)Lb-Derived Excited States in Naphthalene Excimer Formation from ab Initio Multireference Theory with Large Active Space: DMRG-CASPT2 Study.
暂无分享,去创建一个
Takeshi Yanai | Yuki Kurashige | T. Yanai | S. Shirai | Yuki Kurashige | Soichi Shirai | Takeshi Yanai | Soichi Shirai
[1] Frank Neese,et al. The ORCA program system , 2012 .
[2] U. Nagashima,et al. Geometrical structure of benzene and naphthalene: ultrahigh-resolution laser spectroscopy and ab initio calculation. , 2011, The Journal of chemical physics.
[3] S. Shirai,et al. Ab initio studies of aromatic excimers using multiconfiguration quasi-degenerate perturbation theory. , 2011, The journal of physical chemistry. A.
[4] S. McGlynn,et al. Energy of Excimer Luminescence. II. Configuration Interaction between Molecular Exciton States and Charge Resonance States , 1964 .
[5] Allan L. L. East,et al. Naphthalene dimer: Electronic states, excimers, and triplet decay , 2000 .
[6] John R. Platt,et al. Classification of Spectra of Cata-Condensed Hydrocarbons , 1949 .
[7] Robert Häner,et al. A highly sensitive, excimer-controlled molecular beacon. , 2010, Angewandte Chemie.
[8] S. McGlynn,et al. Energy of Excimer Luminescence. I. A Reconsideration of Excimer Processes , 1964 .
[9] Martin Schütz,et al. Molpro: a general‐purpose quantum chemistry program package , 2012 .
[10] S. McGlynn,et al. Energy of Excimer Luminescence. III. Group Theoretical Considerations of Molecular Exciton and Charge Resonance States , 1965 .
[11] Henrik Koch,et al. Coupled cluster response functions , 1990 .
[12] Juyoung Yoon,et al. Unique blue shift due to the formation of static pyrene excimer: highly selective fluorescent chemosensor for Cu2+ , 2006 .
[13] J. Birks,et al. ‘Excimer’ fluorescence VII. Spectral studies of naphthalene and its derivatives , 1965, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.
[14] Ryan M. Richard,et al. Time-Dependent Density-Functional Description of the (1)La State in Polycyclic Aromatic Hydrocarbons: Charge-Transfer Character in Disguise? , 2011, Journal of chemical theory and computation.
[15] Takeshi Yanai,et al. Second-order perturbation theory with a density matrix renormalization group self-consistent field reference function: theory and application to the study of chromium dimer. , 2011, The Journal of chemical physics.
[16] T. Dunning,et al. Electron affinities of the first‐row atoms revisited. Systematic basis sets and wave functions , 1992 .
[17] S. Inagaki,et al. Light harvesting by a periodic mesoporous organosilica chromophore. , 2009, Angewandte Chemie.
[18] B. Roos. The Complete Active Space Self‐Consistent Field Method and its Applications in Electronic Structure Calculations , 2007 .
[19] Debashree Ghosh,et al. Orbital optimization in the density matrix renormalization group, with applications to polyenes and beta-carotene. , 2007, The Journal of chemical physics.
[20] J. Bok,et al. A Fluoride‐Selective PCT Chemosensor Based on Formation of a Static Pyrene Excimer. , 2006 .
[21] Björn O. Roos,et al. Second-order perturbation theory with a complete active space self-consistent field reference function , 1992 .
[22] J. Murrell,et al. The theory of the electronic spectra of aromatic hydrocarbon dimers , 1964 .
[23] T. H. Dunning. Gaussian basis sets for use in correlated molecular calculations. I. The atoms boron through neon and hydrogen , 1989 .
[24] Takeshi Yanai,et al. Complete active space second-order perturbation theory with cumulant approximation for extended active-space wavefunction from density matrix renormalization group. , 2014, The Journal of chemical physics.
[25] White,et al. Density matrix formulation for quantum renormalization groups. , 1992, Physical review letters.
[26] Stefan Grimme,et al. Substantial errors from time-dependent density functional theory for the calculation of excited states of large pi systems. , 2003, Chemphyschem : a European journal of chemical physics and physical chemistry.
[27] N. Handy,et al. A new hybrid exchange–correlation functional using the Coulomb-attenuating method (CAM-B3LYP) , 2004 .
[28] B. Stevens. Evidence for the Photo-Association of Aromatic Hydrocarbons in Fluid Media , 1961, Nature.
[29] J. Brédas,et al. Closely stacked oligo(phenylene ethynylene)s: effect of π-stacking on the electronic properties of conjugated chromophores. , 2012, Journal of the American Chemical Society.
[30] B. Roos,et al. A theoretical study of the electronic spectrum of naphthalene , 1994 .
[31] Manabu Oumi,et al. A doubles correction to electronic excited states from configuration interaction in the space of single substitutions , 1994 .
[32] Kwang Soo Kim,et al. Aromatic Excimers: Ab Initio and TD-DFT Study. , 2013, Journal of chemical theory and computation.
[33] Th. Förster,et al. Ein Konzentrationsumschlag der Fluoreszenz des Pyrens , 1954, Zeitschrift für Elektrochemie, Berichte der Bunsengesellschaft für physikalische Chemie.
[34] Marcel Nooijen,et al. Obtaining the two-body density matrix in the density matrix renormalization group method. , 2008, The Journal of chemical physics.
[35] M. Head‐Gordon,et al. Long-range corrected hybrid density functionals with damped atom-atom dispersion corrections. , 2008, Physical chemistry chemical physics : PCCP.
[36] K. Man,et al. Excitation of naphthalene by electron impact , 1992 .
[37] Th. Förster. Elektronenspektren gekoppelter Moleküle , 1962 .
[38] J. Tanaka. The Electronic Spectra of Aromatic Molecular Crystals. II. The Crystal Structure and Spectra of Perylene , 1963 .
[39] Wataru Mizukami,et al. Density matrix renormalization group for ab initio calculations and associated dynamic correlation methods: A review of theory and applications , 2015 .
[40] Th. Förster,et al. Ein Konzentrationsumschlag der Fluoreszenz des Pyrens , 1955 .
[41] D. Casanova. Theoretical investigations of the perylene electronic structure: Monomer, dimers, and excimers , 2015 .
[42] E. C. Lim,et al. Excimer Formation in van der Waals Dimers and Clusters of Aromatic Molecules , 1996 .
[43] John F. Stanton,et al. The equation of motion coupled‐cluster method. A systematic biorthogonal approach to molecular excitation energies, transition probabilities, and excited state properties , 1993 .
[44] J. B. Birks,et al. Excimers , 2018, Laser Materials Processing.
[45] Leeor Kronik,et al. Charge-Transfer-Like π→π* Excitations in Time-Dependent Density Functional Theory: A Conundrum and Its Solution. , 2011, Journal of chemical theory and computation.
[46] G. C. Morris,et al. The intensity of absorption of naphthalene from 30 000 cm−1 to 53 000 cm−1 , 1968 .
[47] Kimihiko Hirao,et al. Theoretical study of the valence π→π* excited states of polyacenes: Benzene and naphthalene , 1996 .