The detection of ionic species in a polymeric planar electrophoresis device by contactless conductivity measurement is described. To our knowledge this is the first report of such measurements carried out with external electrodes which are part of the holder rather than the separation chip itself. The approach allows the use of bare devices as used for optical measurements, which greatly simplifies the method. The use of a sine wave of 100 kHz of a high amplitude of 500 V for cell excitation assures high sensitivity which is demonstrated with electropherograms for alkali and heavy metal ions as well as inorganic anions and carboxylates at concentrations between 10 and 50 µM. The determination of underivatized amino acids was also possible by using a buffer in the alkaline region where these species are present in anionic form. Detection limits were found to be in the order of 1-5 µM for the inorganic ions and between about 5 and 50 µM for the organic species.
A gain in detection sensitivity of more than 3 orders of magnitude has been achieved in high-resolution
solid-state 13C NMR of monocrystalline fluorene doped with acridine by applying optical nuclear polarization
(ONP) via excited triplet states to protons and transferring this proton polarization to the 13C nuclei. This
sensitivity gain was utilized to measure the angular dependence (rotation pattern) of the 13C NMR lines. In
this way the principal values and orientations of all 13C chemical shielding tensors were determined. While
the 13C shielding tensor of the bridging methylene group exhibits only a small anisotropy, at the aromatic
carbon positions the typical strong anisotropy is observed. All tensors belonging to the same molecule have
one principal axis, perpendicular to the molecular plane, in common, showing that in the crystal lattice the
fluorene molecule is in a planar configuration. The experimental data are compared to ab initio calculations
employing optimized geometries and gauge included atomic orbitals density functional theory (GIAO DFT).
The orientations of all calculated tensors are in excellent agreement with the experimental data. On an absolute
scale the calculated shielding parameters reproduce the experimental values reasonably well. A significant
improvement of the calculated eigenvalues is achieved by shifting the tensors employing data from calculations
of benzene and methane.
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