After the discovery of fullerene-C60, it took almost two decades for the possibility of boron-based fullerene structures to be considered. So far, there has been no experimental evidence for these nanostructures, in spite of the progress made in theoretical investigations of their structure and bonding. Here we report the observation, by photoelectron spectroscopy, of an all-boron fullerene-like cage cluster at B40(-) with an extremely low electron-binding energy. Theoretical calculations show that this arises from a cage structure with a large energy gap, but that a quasi-planar isomer of B40(-) with two adjacent hexagonal holes is slightly more stable than the fullerene structure. In contrast, for neutral B40 the fullerene-like cage is calculated to be the most stable structure. The surface of the all-boron fullerene, bonded uniformly via delocalized σ and π bonds, is not perfectly smooth and exhibits unusual heptagonal faces, in contrast to C60 fullerene.

An elementary molecular process can be characterized by the flow of particles (i.e., electrons and nuclei) that compose the system. The flow, in turn, is quantitatively described by the flux (i.e., the time-sequence of maps of the rate of flow of particles though specified surfaces of observation) or, in more detail, by the flux density. The quantum theory of concerted electronic and nuclear fluxes (CENFs) associated with electronically adiabatic intramolecular processes is presented. In particular, it is emphasized how the electronic continuity equation can be employed to circumvent the failure of the Born-Oppenheimer approximation, which always predicts a vanishing electronic flux density (EFD). It is also shown that all CENFs accompanying coherent tunnelling between equivalent "reactant" and "product" configurations of isolated molecules are synchronous. The theory is applied to three systems of increasing complexity. The first application is to vibrating, aligned H2(+)((2)Σg(+)), or vibrating and dissociating H2(+)((2)Σg(+), J = 0, M = 0). The EFD maps manifest a rich and surprising structure in this simplest of systems; for example, they show that the EFD is not necessarily synchronous with the nuclear flux density and can alternate in direction several times over the length of the molecule. The second application is to coherent tunnelling isomerization in the model inorganic system B4, in which all CENFs are synchronous. The contributions of core and valence electrons to the EFD are separately computed and it is found that core electrons flow with the nuclei, whereas the valence electrons flow obliquely to the core electrons in distinctive patterns. The third application is to the Cope rearrangement of semibullvalene, which also involves coherent tunnelling. An especially interesting discovery is that the so-called "pericyclic" electrons do not behave in the manner typically portrayed by the traditional Lewis structures with appended arrows. Indeed, it is found that only about 3 pericyclic electrons flow, in contrast to the 6 predicted by the Lewis picture. It is remarkable that the time scales of these three processes vary by 18 orders of magnitude: femtoseconds (H2(+)((2)Σg(+))); picoseconds (B4); kilosceconds (semibullvalene). It is emphasized that results presented herein are appearing in the literature for the first time.

A new homocysteine-selective sensor based on the iridium(III) complex Ir(pba)2(acac) (Hpba = 4-(2-pyridyl)benzaldehyde; acac = acetylacetone) was synthesized, and its' photophysical properties were studied. Upon the addition of homocysteine (Hcy) to a semi-aqueous solution of Ir(pba)2(acac), a color change from orange to yellow and a luminescent variation from deep red to green were evident to the naked eye. The blue-shift of the absorption spectrum and enhancement of the phosphorescence emission upon the addition of Hcy can be attributed to the formation of a thiazinane group by selective reaction of the aldehyde group of Ir(pba)2(acac) with Hcy, which was confirmed by 1H NMR studies. Importantly, Ir(pba)2(acac) shows uniquely luminescent recognition of Hcy over other amino acids (including cysteine) and thiol-related peptides (reduced glutathione), in agreement with the higher luminescent quantum yield of the adduct of Ir(pba)2(acac) with Hcy (0.038) compared with that of the adduct with Cys (~0.002). Both surface charge analysis and the electrochemical measurement indicated that a photoinduced electron-transfer process for Ir(pba)2(acac)-Cys might be responsible for the high specificity of Ir(pba)2(acac) toward Hcy over Cys.

Homocysteine (Hcy) and cysteine (Cys) are crucial to the physiological balance in living systems. Specific detection of intracellular Hcy and Cys is of growing importance. Herein, we demonstrated phosphorescence imaging of intracellular Hcy and Cys using a cationic iridium(III) complex Ir(pba)(2)(bpy)(+).PF(6)(-) [pba = 4-(2-pyridyl)benzaldehyde, bpy = bipyridine] containing aldehyde groups as a luminescent probe. Upon addition of Hcy or Cys to a semiaqueous solution of Ir(pba)(2)(bpy)(+), a change in luminescence from yellow to red was visible to the naked eye. The successful chemical reaction of the aldehyde in Ir(pba)(2)(bpy)(+) with Hcy and Cys to form thiazinane and thiazolidine was confirmed by (1)H NMR. Moreover, complexation with Hcy and Cys disturbed the p-pi conjugation between the aldehyde group and the bpy moiety, and led to the excited states switching to [dpi(Ir)-pi(N(wedge)N)*] (3)MLCT and [pi(C(wedge)N)-pi(N(wedge)N)*] (3)LLCT from (pi-pi*)(pba(-)) (3)IL. Furthermore, the MTT assay was used to determine that the probe has low cytotoxicity. Importantly, cell imaging experiments demonstrated that the probe is membrane permeable and can monitor the changes of Hcy/Cys within living cells in a ratiometric mode.