8 research outputs found
Effect of Proton Substitution by Alkali Ions on the Fluorescence Emission of Rhodamine B Cations in the Gas Phase
The
photophysics of chromophores is strongly influenced by their
environment. Solvation, charge state, and adduct formation significantly
affect ground and excited state energetics and dynamics. The present
study reports on fluorescence emission of rhodamine B cations (RhBH<sup>+</sup>) and derivatives in the gas phase. Substitution of the acidic
proton of RhBH<sup>+</sup> by alkali metal cations, M<sup>+</sup>,
ranging from lithium to cesium leads to significant and systematic
blue shifts of the emission. The gas-phase structures and singlet
transition energies of RhBH<sup>+</sup> and RhBM<sup>+</sup>, M =
Li, Na, K, Rb, and Cs, were investigated using HartreeâFock
theory, density functional methods, second-order MøllerâPlesset
perturbation theory, and the second-order approximate coupled-cluster
model CC2. Comparison of experimental and theoretical results highlights
the need for improved quantum chemical methods, while the hypsochromic
shift observed upon substitution appears best explained by the Stark
effect due to the inhomogeneous electric field generated by the alkali
ions
From Planar to Cage in 15 Easy Steps: Resolving the C<sub>60</sub>H<sub>21</sub>F<sub>9</sub><sup>â</sup> â C<sub>60</sub><sup>â</sup> Transformation by Ion Mobility Mass Spectrometry
A combination
of mass spectrometry, collision-induced dissociation,
ion mobility mass spectrometry (IM-MS), and density functional theory
(DFT) has been used to study the evolution of anionic species generated
by laser-desorption of the near-planar, fluorinated polycyclic aromatic
hydrocarbon (PAH), C<sub>60</sub>H<sub>21</sub>F<sub>9</sub> (s).
The dominant decay process for isolated, thermally activated C<sub>60</sub>H<sub>21</sub>F<sub>9</sub><sup>â</sup> species comprises
a sequence of multiple regioselective cyclodehydrofluorination and
cyclodehydrogenation reactions (eliminating HF and H<sub>2</sub>,
respectively, while forming additional pentagons and/or hexagons).
The DFT calculations allow us to set narrow bounds on the structures
of the resulting fragment ions by fitting structural models to experimentally
determined collision cross sections. These show that the transformation
of the precursor anion proceeds via a series of intermediate structures
characterized by increasing curvature, ultimately leading to the closed-shell
fullerene cage C<sub>60</sub><sup>â</sup> as preprogrammed
by the precursor structure
Gas-Phase Photoluminescence Characterization of Stoichiometrically Pure Nonanuclear Lanthanoid Hydroxo Complexes Comprising Europium or Gadolinium
Gas-phase
photoluminescence measurements involving mass-spectrometric techniques
enable determination of the properties of selected molecular systems
with knowledge of their exact composition and unaffected by matrix
effects such as solvent interactions or crystal packing. The resulting
reduced complexity facilitates a comparison with theory. Herein, we
provide a detailed report of the intrinsic luminescence properties
of nonanuclear europiumÂ(III) and gadoliniumÂ(III) 9-hydroxyÂphenalen-1-one
(HPLN) hydroxo complexes. Luminescence spectra of [Eu<sub>9</sub>(PLN)<sub>16</sub>(OH)<sub>10</sub>]<sup>+</sup> ions reveal an europium-centered
emission dominated by a 4-fold split Eu<sup>III</sup> hypersensitive
transition, while photoluminescence lifetime measurements for both
complexes support an efficient europium sensitization via a PLN-centered
triplet-state manifold. The combination of gas-phase measurements
with density functional theory computations and ligand-field theory
is used to discuss the antiprismatic core structure of the complexes
and to shed light on the energy-transfer mechanism. This methodology
is also employed to fit a new set of parameters, which improves the
accuracy of ligand-field computations of Eu<sup>III</sup> electronic
transitions for gas-phase species
Vibronic Coupling Analysis of the Ligand-Centered Phosphorescence of Gas-Phase Gd(III) and Lu(III) 9âOxophenalen-1-one Complexes
The gas-phase laser-induced
photoluminescence of cationic mononuclear
gadolinium and lutetium complexes involving two 9-oxophenalen-1-one
ligands is reported. Performing measurements at a temperature of 83
K enables us to resolve vibronic transitions. Via comparison to FranckâCondon
computations, the main vibrational contributions to the ligand-centered
phosphorescence are determined to involve rocking, wagging, and stretching
of the 9-oxophenalen-1-oneâlanthanoid coordination in the low-energy
range, intraligand bending, and stretching in the medium- to high-energy
range, rocking of the carbonyl and methine groups, and CâH
stretching beyond. Whereas FranckâCondon calculations based
on density-functional harmonic frequency computations reproduce the
main features of the vibrationally resolved emission spectra, the
absolute transition energies as determined by density functional theory
are off by several thousand wavenumbers. This discrepancy is found
to remain at higher computational levels. The relative energy of the
GdÂ(III) and LuÂ(III) emission bands is only reproduced at the coupled-cluster
singles and doubles level and beyond
Characterization of Nonanuclear Europium and Gadolinium Complexes by Gas-Phase Luminescence Spectroscopy
Gas-phase measurements
using mass-spectrometric techniques allow
determination of the luminescence properties of selected molecular
systems with knowledge of their exact composition. Furthermore, isolated
luminophores are unaffected by matrix effects like solvent interactions
or crystal packing. As a result, the system complexity is reduced
relative to the condensed phase and a direct comparison with theory
is facilitated. Herein, we report the intrinsic luminescence properties
of nonanuclear europiumÂ(III) and gadoliniumÂ(III) 9-hydroxyphenalen-1-one
(HPLN)âhydroxo complexes. Luminescence spectra of [Eu<sub>9</sub>(PLN)<sub>16</sub>(OH)<sub>10</sub>]<sup>+</sup> ions reveal an europium-centered
emission dominated by a 4-fold split EuÂ(III) hypersensitive transition.
The corresponding GdÂ(III) complex, [Gd<sub>9</sub>(PLN)<sub>16</sub>(OH)<sub>10</sub>]<sup>+</sup>, shows a broad emission from a ligand
based triplet state with an onset of about 1000 wavenumbers in excess
of the europium emission. As supported by photoluminescence lifetime
measurements for both complexes, we deduce an efficient europium sensitization
via PLN-based triplet states. The luminescence spectra of the complexes
are discussed in terms of a square antiprismatic europium/gadolinium
core structure as suggested by density functional computations
Gas-Phase Photoluminescence and Photodissociation of Silver-Capped Hexagold Clusters
We
report on the radiative and nonradiative deactivation pathways
of selected charge states of the stoichiometric hexagold phosphine-stabilized
ionic clusters, [(C)Â(AuDppy)<sub>6</sub>Ag<sub>2</sub>¡(BF<sub>4</sub>)<sub><i>x</i></sub>]<sup>(4â<i>x</i>)+</sup> with <i>x</i> = 2 and 3 (Dppy = diphenylphosphino-2-pyridine),
combining gas-phase photoluminescence and photodissociation with quantum
chemical computations. These clusters possess an identical isostructural
core made of a hyper-coordinated carbon at their center octahedrally
surrounded by six gold ions, and two silver ions at their apexes.
Their luminescence and fragmentation behavior upon photoexcitation
was investigated under mass and charge control in an ion trap. The
experimental and computational results shed light on the electronic
states involved in the optical transitions as well as on their core,
ligand, or charge transfer character. Gas-phase results are discussed
in relation with condensed phase measurements, as well as previous
observations in solution and on metalâorganic frameworks. The
monocationic species (<i>x</i> = 3) is found to be less
stable than the dicationic one (<i>x</i> = 2). In the luminescence
spectrum of the monocationic species, a shoulder at short wavelength
can be observed and is assigned to fragment emission. This fragment
formation appears to be favored for the monocation by the existence
of a low lying singlet state energetically overlapping with the triplet
state manifold, which is populated quickly after photoexcitation
Photoluminescence Spectroscopy of Mass-Selected Electrosprayed Ions Embedded in Cryogenic Rare-Gas Matrixes
An
apparatus is presented which combines nanoelectrospray ionization
for isolation of large molecular ions from solution, mass-to-charge
ratio selection in gas-phase, low-energy-ion-beam deposition into
a (co-condensed) inert gas matrix and UV laser-induced visible-region
photoluminescence (PL) of the matrix isolated ions. Performance is
tested by depositing three different types of lanthanoid diketonate
cations including also a dissociation product species not directly
accessible by chemical synthesis. For these strongly photoluminescent
ions, accumulation of some femto- to picomoles in a neon matrix (over
a time scale of tens of minutes to several hours) is sufficient to
obtain well-resolved dispersed emission spectra. We have ruled out
contributions to these spectra due to charge neutralization or fragmentation
during deposition by also acquiring photoluminescence spectra of the
same ionic species in the gas phase
Ion Mobility Spectrometry, Infrared Dissociation Spectroscopy, and ab Initio Computations toward Structural Characterization of the Deprotonated Leucine-Enkephalin Peptide Anion in the Gas Phase
Although
the sequencing of protonated proteins and peptides with
tandem mass spectrometry has blossomed into a powerful means of characterizing
the proteome, much less effort has been directed at their deprotonated
analogues, which can offer complementary sequence information. We
present a unified approach to characterize the structure and intermolecular
interactions present in the gas-phase pentapeptide leucine-enkephalin
anion by several vibrational spectroscopy schemes as well as by ion-mobility
spectrometry, all of which are analyzed with the help of quantum-chemical
computations. The picture emerging from this study is that deprotonation
takes place at the C terminus. In this configuration, the excess charge
is stabilized by strong intramolecular hydrogen bonds to two backbone
amide groups and thus provides a detailed picture of a potentially
common charge accommodation motif in peptide anions