Excited-state singly substituted

Although variational methods are quite general and any CSF with the required quantum numbers may be included in an expansion, it is extremely helpful to follow a computational model for the inclusion of correlation in an efficient manner such as single (S) and double (D) substitutions from a multireference set of CSFs. These substitutions are often referred to as excitations but when the state under consideration is an excited state, some substitutions may be to CSFs with a lower energy and the term is misleading. An example would be a calculation for the 3p 2P° ASF of aluminum. The substitution 3p 3s is a de-excitation and ensures that the excited state is orthogonal to a lower state of the same symmetry. For some properties, such as hyperfine constants [2], it may be necessary to include selected triple (T) and quadruple (Q) substitutions. Such expansions increase in size rapidly with the size of the orbital set. 

Organic dye nanoparticles of DHIA and DHBIA (the chemical structures are shown in Fig. 1) have been synthesized in THF/water mixed solvent by a reprecipitation method [32]. These dye molecules possess a 2-(2-hydroxyphenyl) benzothiazole (HBT) unit, which is known to be more stable as an enol imine form in the ground state and as a keto amine form in the excited state [32, 33] (Fig. 6). The nanoparticles exhibited the AIEE phenomenon mainly due to a restricted intramolecular motion, that is, impediment to free rotation of two end-substituted HBT units around single bonds. It is interesting to note that the... 

A number of methods have been proposed for calculations of the geometries of molecules in excited states. These include CIS (Configuration Interaction Singles) and variations on CIS to account for the effect of double substitutions, as well as so-called time dependent density functional models. Except for CIS (the simplest of the methods) there is very little practical experience. There is also very little solid experimental data on the geometries of excited-state molecules. 

Abstract. We present a quantum-classieal determination of stable isomers of Na Arii clusters with an electronically excited sodium atom in 3p P states. The excited states of Na perturbed by the argon atoms are obtained as the eigenfunctions of a single-electron operator describing the electron in the field of a Na Arn core, the Na and Ar atoms being substituted by pseudo-potentials. These pseudo-potentials include core-polarization operators to account for polarization and correlation of the inert part with the excited electron . The geometry optimization of the excited states is carried out via the basin-hopping method of Wales et al. The present study confirms the trend for small Na Arn clusters in 3p states to form planar structures, as proposed earlier by Tutein and Mayne within the framework of a first order perturbation theory on a "Diatomics in Molecules" type model. 

A survey of many such reactions suggests that there is no single, simple pattern that can be used to predict the outcome of photochemical nucleophilic substitutions, but rather a situation in which oneof at least three mechanisms may operate, and this has been borne out by more detailed mechanistic studies. One approach to rationalizing the preferred orientation in the excited-state reactions is to calculate electron densities at the various ring carbon atoms for a particular pattern of substituents, and to assume that preferential attack by a nucleophile will take place at the position of lowest electron density. This static reactivity leads to the prediction that a nitro group is meta-directing for direct nucleophilic attack in the excited state,... 

The photodissociation of aromatic molecules does not always take place at the weakest bond. It has been reported that in a chlorobenzene, substituted with an aliphatic chain which holds a far-away Br atom, dissociation occurs at the aromatic C-Cl bond rather than at the much weaker aliphatic C-Br bond (Figure 4.30). This is not easily understood on the basis of a simple picture of the crossing to a dissociative state, and it is probable that the reaction takes place in the tt-tt Si excited state which is localized on the aromatic system. There are indeed cases in which the dissociation is so fast (< 10-12 s) that it competes efficiently with internal conversion. 1-Chloromethyl-Np provides a clear example of this behaviour, its fluorescence quantum yield being much smaller when excitation populates S2 than when it reaches Figure 4.31 shows a comparison of the fluorescence excitation spectrum and the absorption spectrum of this compound. This is one of the few well-documented examples of an upper excited state reaction of an organic molecule which has a normal pattern of energy levels (e.g. unlike azulene or thioketones). This unusual behaviour is related of course to the extremely fast dissociation, within a single vibration very probably. We must now... 

In two recent publications we have tried to characterize the excited state properties of 1 and 3 in order to facilitate their detection by LIF-spectroscopy. Our main tool in this effort has been equation of motion coupled cluster theory (EOM-CC). The EOM-CCSD method, which is equivalent to linear response CCSD, has been shown to provide an accurate description of both valence and excited states even in systems where electron correlation effects play an important role [39]. Computed transition energies for excitations that are of mainly single substitution character are generally accurate to within 0.1 eV. We have found the EOM-CCSD method to perform particularly well in combination with the doubly-augmented cc-pVDZ (d-aug-cc-pVDZ) basis set. This basis seems to provide equally balanced descriptions of ground and excited states,... 

Rico RJ, Head-Gordon M (1993) Single-reference theories of molecular excited states with single and double substitutions. Chem Phys Lett 213 224—232. 

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