Size-selected, ligand-free gold clusters with diameters less than 2 nm can be routinely generated in the gas phase. The pronounced size dependence of their physical and chemical properties is one of their most important features. Surfacedeposited gold clusters are particularly interesting for applications in nanotechnology and heterogeneous catalysis. [1][2][3][4][5][6][7] One prerequisite for such applications is a detailed knowledge of the cluster structures.The extensive literature on theoretical studies of gold clusters has been surveyed in recent reviews. [8,9] In principle, quantum-chemical methods allow many properties of small gold clusters to be predicted with high accuracy. However, for larger clusters, the large number of possible isomers impedes the search for a global energy minimum. Often, only a small set of the possible structures can be considered, without any guarantee that the global minimum is included in the set. Consequently, progress in the intermediate size regime can only be made through the joint use of experiment and theory.In this fashion, the structures of small gold cluster anions and cations with up to 13 atoms have been inferred through a comparison of theoretical and experimental collision cross sections from ion-mobility measurements. [10,11] A remarkable finding in this study was that the 2D!3D structural transition for Au n À occurs at the surprisingly large cluster sizes of n = 11 and 12. This result was later confirmed through a comparison of photoelectron spectroscopy (PES) data with calculated density of states (DOS) curves.[12] For Au n À with n = 16-18 and 21-24, experimental and theoretical evidence for hollow cage-like structures has been reported. [13][14][15] Au 20 À possesses a tetrahedral structure, [16] which corresponds to a fragment of the face-centered cubic (fcc) structure of bulk gold; the cluster consists only of surface atoms and does not contain any inner atoms.It has been suggested, on the basis of quantum-chemical calculations, that medium-sized gold clusters, such as Au n with n = 32-35, [17,18] 42, [19] , and 50, [20] also have cage-like structures. In contrast, in a recent study, Au 32 À was assigned an amorphous, but dense, structure on the basis of a comparison of data from PES and the calculated DOS.[21] Low-symmetry "disordered" structures have also been proposed by Garzón et al. for Au 28 and Au 55 .[22] These results were supported by a combined PES and theoretical study by Häkkinen et al., which excluded high-symmetry structures for Au 55 À (whereas Ag 55 À and Cu 55 À have icosahedral structures).[23]The PE spectra of several Au n À clusters, notably for n = 14, 20, 34, and 58, show prominent band gaps, [24] reflecting the large gaps between the highest occupied molecular orbital (HOMO) and the lowest unoccupied molecular orbital (LUMO) in the corresponding neutral clusters. The associated valence-electron counts correlate with the sequence of jellium-shell closings obtained from a simple free-electron model invoking (volume-filling) spherical ...

The structures of mass selected silver cluster cations Ag19 +, Ag38 +, Ag55 +, Ag59 +, Ag75 +, and Ag79 + have been probed at a temperature of 100 K by trapped ion electron diffraction. The structure assignment is carried out by comparison of the experimental scattering intensity with theoretical scattering functions of calculated candidate structures obtained by density functional theory. For the cluster sizes studied the resulting experimental data are invariably best described by structures based on the icosahedral motif, while closed packed structures can be ruled out.

Ultrafast pump-probe spectroscopic studies on the hydrated 7-azaindole monomer are presented. The experiments provide evidence that excited-state proton transfer in the gas-phase hydrated 7-azaindole monomer may be possible, as predicted by theory, and can occur by means of a water proton bridge. As explained in the text, full tautomerization may not be occurring, but rather the transfer of a proton from the 7-azaindole monomer to the solvating water molecules. A calculated geometry for the structure of 7-azaindole clustered with four waters is presented and used to explain the rate increase observed in this species compared to the 7-azaindole monomer clustered with two and three waters. Experimental SectionHydrated clusters of 7Aza were formed by means of supersonic expansion into a vacuum. Vapor from 7Aza (Sigma), † Part of the special issue "C. Bradley Moore Festschrift".

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We present a comparative study on the structural properties of the coinage metal icosamers Cu(20)(+/-), Ag(20)(+/-), and Au(20)(+/-). Using trapped ion electron diffraction measurements in combination with density functional structure calculations we find distinct structural differences depending on the cluster material and the charge state: Cu(20)(-), Cu(20)(+), as well as Ag(20)(+) prefer icosahedral structures. Ag(20)(-) adopts a rearranged, distorted icosahedral structure. While Au(20)(-) is tetrahedral, Au(20)(+) cannot be described satisfyingly by a single isomer alone. Here a mixture of tetrahedral and distorted icosahedral structures is suggested. The influence of material and charge on the structural properties of the coinage metal icosamers is discussed.

Hardware from a commercial-off-the-shelf (COTS) ion mobility spectrometry (IMS) based explosive trace detector (ETD) has been interfaced to an AB/SCIEX API 2000 triple quadrupole mass spectrometer. To interface the COTS IMS based ETD to the API 2000, the faraday plate of the IMS instrument and the curtain plate of the mass spectrometer were removed from their respective systems and replaced by a custom faraday plate, which was fabricated with a hole for passing the ion beam to the mass spectrometer, and a custom interface flange, which was designed to attach the IMS instrument onto the mass spectrometer. Additionally, the mass spectrometer was modified to increase the electric field strength and decrease the pressure in the differentially pumped interface, causing a decrease in the effect of collisional focusing and permitting a mobility spectrum to be measured using the mass spectrometer. The utility of the COTS-ETD/API 2000 configuration for the characterization of the gas phase ion chemistry of COTS-ETD equipment was established by obtaining mass and tandem mass spectra in the continuous ion flow and selected mobility monitoring operating modes and by obtaining mass-selected ion mobility spectra for the explosive standard 2,4,6 trinitrotoluene (TNT). This analysis confirmed that the product ion for TNT is [TNT - H](-), the predominant collision-induced dissociation pathway for [TNT- H](-) is the loss of NO and NO(2), and the reduced mobility value for [TNT - H](-) is 1.54 cm(2)V(-1) s(-1). Moreover, this analysis was attained for sample amounts of 1 ng and with a resolving power of 37. The objective of the research is to advance the operational effectiveness of COTS IMS based ETD equipment by developing a platform that can facilitate the understanding of the ion chemistry intrinsic to the equipment.

The highly pyramidalized alkene, pentacyclo[4.3.0.0(2,4).0(3,8).0(5,7)]non-4-ene (9), has been generated via treatment of 4,5-diiodopentacyclo[4.3.0.0(2,4).0(3,8).0(5,7)]nonane (12) with n-butyllithium and tert-butyllithium. The title alkene has also been trapped as its Diels-Alder adduct with 1,3-diphenylisobenzofuran, 2,5-dimethylfuran, and spiro[2.4]hepta-4,6-diene. Products resulting from alkyllithium addition to the pyramidalized double bond of 9 have been isolated and fully characterized spectroscopically. The geometry, olefin strain energy, heat of hydrogenation, and relative HOMO/LUMO energies of 9 have been obtained by ab initio calculations at the MP2 and B3LYP levels using the 6-31G* basis set.

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