The gas-phase reactivity of lanthanide (Ln+ = La+−Lu+), group 2 (Ca+, Sr+, and Ba+), and group 3 (Sc+ and Y+) cations, and of their corresponding monoxide ions MO+, with pentamethylcyclopentadiene (C5Me5H) was studied by Fourier transform ion cyclotron resonance mass spectrometry. The reactivity of Eu+, Tm+, Yb+, and the alkaline earth metal ions was similar to that observed previously for Sm+, namely formation of the fulvenide ion M(C5Me4CH2)+ as the main primary product and the metallocene ion M(C5Me5)2 + as the main secondary product. With Sc+, Y+, and the remaining lanthanide series ions, several other species were observed in the primary reactions, corresponding to single and multiple losses of neutral molecules such as H2 and CH4. These differences in reactivity appear to correlate with the accessibility of reactive excited state electron configurations of the metal ions. In the case of the metal oxide cations MO+, the reactivity with pentamethylcyclopentadiene appears to be determined by the strength of the M+−O bonds. The ions with the strongest bonds, LaO+, CeO+, PrO+, and NdO+, formed M(C5Me5)(OH)+ as the sole primary product, which reacted further, eliminating water, to give the metallocene ion M(C5Me5)2 +. ScO+, YO+, and the lanthanide series ions SmO+, GdO+−TmO+, and LuO+ yielded MO(C5Me4CH2)+ and M(C5Me4CH2)+ as the primary products in addition to M(C5Me5)(OH)+. These metal oxides gave M(C5Me4CH2)2 + and M(C5Me5)2 + as secondary products. The ions with the weakest M+−O bonds, EuO+, YbO+, CaO+, SrO+, and BaO+, formed MOH+ as a primary product and M(C5Me5)+ as a secondary product.
The gas phase chemistry of bis(pentamethylcyclopentadienyl)samarium, (C5Me5)2Sm, was studied by Fourier transform ion cyclotron resonance mass spectrometry (FTICR/MS). Positive electron impact (EI) spectra showed the formation of (C5Me5)2Sm+, (C5Me5)Sm+, and Sm+. All three ions reacted with (C5Me5)2Sm by charge transfer, as verified by double-resonance techniques, and (C5Me5)Sm+ also formed the (C5Me5)3Sm2 + ion in a condensation reaction with neutral (C5Me5)2Sm. The laser desorption/ionization (LDI) spectra showed, in addition to (C5Me5)2Sm+, (C5Me5)Sm+, and Sm+, the formation of (C5Me4H)Sm+ and (C5Me4CH2)Sm+. The latter species most probably involves a tetramethylfulvenide ligand. Access to all of the ionic species cited here could also be obtained by reacting laser-desorbed Sm+ ions with pentamethylcyclopentadiene, C5Me5H. (C5Me4CH2)Sm+, (C5Me4H)Sm+, and (C5Me5)Sm+ were formed as primary products, and the metallocene ion (C5Me5)2Sm+ resulted from the rapid addition of C5Me5H to (C5Me4CH2)Sm+.
We report the polarized infrared reflectance spectra and optical conductivity of β‘ ‘-(ET)2SF5RSO3 superconducting (R = CH2CF2), metallic (R = CHF), and metal−insulator (R = CHFCF2) mixed crystal materials. Incorporation of chiral counterions in the superconducting matrix allows us to tune the physical and spectroscopic properties over the composition range by modulating the anion potential. We conclude that the two low-energy electronic excitations at ≈5200 and 9600 cm-1 are spectral manifestations of charge localization in the ET stack, made manifest by both local (anion pocket) and spatial (positional) disorder.
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