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Tetraspanins function as organizers of the cell surface by recruiting specific partner proteins into tetraspanin-enriched microdomains, which regulate processes such as cell adhesion, signalling and intracellular trafficking. Endothelial cells appear to express at least 23 of the 33 human tetraspanins, and a number of recent studies have demonstrated their importance in endothelial cell biology. Tetraspanin CD151 is essential for pathological angiogenesis, which may in part be due to regulation of its main partner proteins, the laminin-binding integrins α3β1, α6β1 and α6β4. CD9 and CD151 are essential for leucocyte recruitment during an inflammatory response, through the formation of pre-assembled nano-platforms containing the adhesion molecules ICAM-1 (intercellular adhesion molecule 1) and VCAM-1 (vascular cell adhesion molecule 1), which ultimately coalesce to form docking structures around captured leucocytes. Tetraspanin CD63 also facilitates leucocyte capture by promoting clustering of the adhesion molecule P-selectin. Finally, Tspan12 is required for blood vessel development in the eye, through regulation of Norrin-induced Frizzled-4 signalling, such that Tspan12 mutations can lead to human disease. Future studies on these and other endothelial tetraspanins are likely to provide further novel insights into angiogenesis and inflammation. [ABSTRACT FROM AUTHOR]

Electronic structure calculations at the level of second-order Møller−Plesset perturbation theory have been performed on anionic water clusters, (H 2O) n−, in the n= 14−33 size regime. The contribution to the electron binding energy that arises from electron correlation is found to be significantly larger for cavity-bound electrons than it is for surface-bound electrons, even for surface states with electron binding energies well above 1 eV. A decomposition of the correlation energy into interactions between pairs of Boys-localized molecular orbitals is used to demonstrate that the larger correlation energy found in the cavity isomers arises from electron−water dispersion interactions, and that the dispersion interaction is larger in cavity-bound isomers because the unpaired electron penetrates well beyond the first solvation shell. In contrast, a surface-bound electron exhibits virtually no penetration into the interior of the cavity. To obtain a qualitatively accurate picture of this phenomenon, one must plot molecular orbitals using isoprobability surfaces rather than arbitrarily-selected isocontours. [ABSTRACT FROM AUTHOR]

The lowest few electronic excitations of a π-stacked adenine dimer in its B-DNA geometry are investigated, in the gas phase and in a water cluster, using a long-range-corrected version of time-dependent density functional theory (TD-DFT) that asymptotically incorporates Hartree−Fock exchange. Long-range correction is shown to eliminate the catastrophic underestimation of charge-transfer (CT) excitation energies that plagues conventional TD-DFT, at the expense of introducing one adjustable parameter, μ, that determines the length scale on which Hartree−Fock exchange is turned on. This parameter allows us to interpolate smoothly between hybrid density functionals and time-dependent Hartree−Fock theory. Excitation energies for CT states (in which an electron is transferred from one adenine molecule to the other) are found to increase dramatically as a function of μ. Uncorrected hybrid functionals underestimate the CT excitation energies, placing them well below the valence excitations, while time-dependent Hartree−Fock calculations place these states well above the valence states. Values for μ determined from certain benchmark calculations place the CT states well above the valence ππ* and nπ* states at the Franck−Condon point. [ABSTRACT FROM AUTHOR]