Electronic and vibrational properties of a MOF-5 metal-organic framework: ZnO quantum dot behaviour.

UV-Vis DRS and photoluminescence (PL) spectroscopy, combined with excitation selective Raman spectroscopy, allow us to understand the main optical and vibrational properties of a metal-organic MOF-5 framework. A O(2-)Zn(2+)[rightward arrow] O(-)Zn(+) ligand to metal charge transfer transition (LMCT) at 350 nm, testifies that the Zn(4)O(13) cluster behaves as a ZnO quantum dot (QD). The organic part acts as a photon antenna able to efficiently transfer the energy to the inorganic ZnO-like QD part, where an intense emission at 525 nm occurs.

Vibrational structure of titanium silicate catalysts. A spectroscopic and theoretical study.

A thorough analysis of the vibrational features of the titanium silicalite-1 (TS-1) catalyst is presented, based on quantitative IR measurements, Raman and resonant Raman experiments, quantitative XANES, and quantum chemical calculations on cluster and periodic models. The linear correlation of the intensity of the IR and Raman bands located at 960 and 1125 cm(-1) and the XANES peak at 4967 eV with the amount of tetrahedral Ti are quantitatively demonstrated. Raman and resonant Raman spectra of silicalite and TS-1 with variable Ti content are presented, showing main features at 960 and 1125 cm(-1) associated with titanium insertion into the zeolite framework. The enhancement of the intensity of the 1125 cm(-1) feature and the invariance of the 960 cm(-1) feature in UV-Raman experiments, are discussed in terms of resonant Raman selection rules. Quantum chemical calculations on cluster models Si[OSi(OH)(3)](4) and Ti[OSi(OH)(3)](4) at the B3LYP/6-31G(d) level of theory provide the basis for the assignment of the main vibrational contributions and for the understanding of Raman enhancement. The resonance-enhanced 1125 cm(-1) mode is unambiguously associated with a totally symmetric vibration of the TiO(4) tetrahedron, achieved through in-phase antisymmetric stretching of the four connected Ti-O-Si bridges. This vibration can also be described as a totally symmetric stretching of the four Si-O bonds pointing toward Ti. The resonance enhancement of this feature is explained in terms of the electronic structure of the Ti-containing moiety. Asymmetric stretching modes of TO(4) units show distinct behavior when (i) T is occupied by Si as in perfect silicalite, (ii) T is occupied by Ti as in TS-1, or (iii) the oxygen atom belongs to an OH group, such as in terminal tetrahedra of cluster models and in real defective zeolites. Asymmetric SiO(4) and TiO(4) stretching modes appear above and below 1000 cm(-1), respectively, when they are achieved through antisymmetric stretching of the T-O-Si bridges, and around 800 cm(-1) (in both SiO(4) and TiO(4)) when they involve symmetric stretching of the T-O-Si units. In purely siliceous models, the transparency gap between the main peaks at 800 and 1100 cm(-1) contains only vibrational features associated with terminal Si-OH groups, while in Ti-containing models it contains also the above-mentioned asymmetric TiO(4) modes, which in turn are strongly coupled with Si-OH stretching modes. Calculations on periodic models of silicalite and TS-1 free of OH groups using the QMPOT embedding method correctly reproduce the transparency gap of silicalite and the appearance of asymmetric TiO(4) vibrations at 960 cm(-1) in TS-1. Finally, we demonstrate, for the first time, that the distortion of the tetrahedral symmetry around Ti caused by water adsorption quenches the UV-Raman enhancement of the 1125 cm(-1) band.

An NMR and molecular mechanics study of squalene and squalene derivatives.

Various squalene derivatives, including squalene, squalene 2,3-epoxide (monoepoxide, SQME), squalene 2,3;22,23-diepoxide (SQDE), 2-aza-2,3-dihydrosqualene (SQN) and 2-aza-2,3-dihydrosqualene N-oxide (SQNO), were studied in chloroform solutions using ID high-resolution 1H spectra and 13C longitudinal relaxation studies, 2D proton NOESY and COSY and 2D proton-carbon HETCOR spectroscopy. A full interpretation of the 1H and 13C-NMR spectra is presented. Staggered conformations along the C11-C12 bond are favoured and a relatively rigid structure of the central part of the chain is indicated in relaxation and coupling data, while further away from the central part the molecular mobility grows. A detected NOE dipolar interaction between terminal and central parts of the molecule indicates the presence of dynamically folded structures in solution. The proposed model also explains the selective reactivity of the mobile chain endings with respect to the central part which is protected by these moving ends. Different solvents at different concentrations induce some variations in this molecular model with a shortening or a lengthening of the mean path covered by the tail endings. Molecular mechanics and molecular dynamics calculations on the free squalene molecule indicate that the mobility of the chain is almost equivalent in all its isoprenic moieties, and the greater mobility of the chain ends may be ascribed to co-operative movements from the center to the tails. The solvent probably plays an important role in hindering the motion of the central part of the molecule.