19 research outputs found
Inorganic and Organozinc Fluorocarboxylates: Synthesis, Structure and Materials Chemistry
The organozinc fluorocarboxylates
RZnO<sub>2</sub>CR<sub>f</sub> and RZnO<sub>2</sub>CR<sub>f</sub>Ā·TMEDA,
along with ZnĀ(O<sub>2</sub>CR<sub>f</sub>)<sub>2</sub>Ā·TMEDA
(R = Me, Et; R<sub>f</sub> = C<sub>2</sub>F<sub>5</sub>, C<sub>3</sub>F<sub>7</sub>) have been synthesized. The structures of EtZnO<sub>2</sub>C<sub>2</sub>F<sub>5</sub> (<b>5</b>), EtZnO<sub>2</sub>C<sub>3</sub>F<sub>7</sub> (<b>7</b>), EtĀZnĀO<sub>2</sub>C<sub>2</sub>F<sub>5</sub>Ā·TMEDA (<b>11</b>), ZnĀ(O<sub>2</sub>C<sub>2</sub>F<sub>5</sub>)<sub>2</sub>Ā·TMEDA (<b>13</b>), along with products from the adventitious reaction with
either O<sub>2</sub> or H<sub>2</sub>O, Zn<sub>10</sub>Me<sub>4</sub>(OMe)<sub>4</sub>(O<sub>2</sub>CC<sub>2</sub>F<sub>5</sub>)<sub>12</sub> (<b>2</b>), Zn<sub>9</sub>ĀEt<sub>2</sub>Ā(O<sub>2</sub>ĀCC<sub>2</sub>F<sub>5</sub>)<sub>12</sub>(O)<sub>2</sub> (<b>6</b>), Zn<sub>8</sub>Et<sub>4</sub>(OEt)<sub>4</sub>(O<sub>2</sub>CC<sub>3</sub>F<sub>7</sub>)<sub>6</sub>(O) (<b>8</b>), [ZnĀ(O<sub>2</sub>CC<sub>3</sub>F<sub>7</sub>)<sub>2</sub>Ā·TMEDA]<sub>2</sub>Ā·H<sub>2</sub>O (<b>15</b>) have been determined.
Thin films of oriented ZnO have been deposited on glass substrates
by low-pressure chemical vapor deposition (LPCVD) using <b>3</b> and <b>10</b> as precursors, though no fluorine incorporation
in the films was noted. LPCVD using <b>13</b> as precursor also
yielded fluorine-free ZnO, but lacking the oriented growth observed
using <b>3</b>, <b>10</b>. However, <b>5</b>, which
exhibits short intermolecular ZnĀ·Ā·Ā·F contacts in the
solid state, thermally decomposes to bulk ZnF<sub>2</sub>
Unnatural Amino Acid Mutagenesis Reveals Dimerization As a Negative Regulatory Mechanism of VHRās Phosphatase Activity
<i>Vaccinia</i> H1-related
(VHR) phosphatase is a dual
specificity phosphatase that is required for cell-cycle progression
and plays a role in cell growth of certain cancers. Therefore, it
represents a potential drug target. VHR is structurally and biochemically
well characterized, yet its regulatory principles are still poorly
understood. Understanding its regulation is important, not only to
comprehend VHRās biological mechanisms and roles but also to
determine its potential and druggability as a target in cancer. Here,
we investigated the functional role of the unique āvariable
insertā region in VHR by selectively introducing the photo-cross-linkable
amino acid <i>para-</i>benzoylphenylalanine (<i>p</i>BPA) using the amber suppression method. This approach led to the
discovery of VHR dimerization, which was further confirmed using traditional
chemical cross-linkers. Phe68 in VHR was discovered as a residue involved
in the dimerization. We demonstrate that VHR can dimerize inside cells,
and that VHR catalytic activity is reduced upon dimerization. Our
results suggest that dimerization could occlude the active site of
VHR, thereby blocking its accessibility to substrates. These findings
indicate that the previously unknown transient self-association of
VHR acts as a means for the negative regulation of its catalytic activity
How To Arrive at Accurate Benchmark Values for Transition Metal Compounds: Computation or Experiment?
With
the objective of analyzing which kind of reference data is
appropriate for benchmarking quantum chemical approaches for transition
metal compounds, we present the following, (a) a collection of 60
transition metal diatomic molecules for which experimentally derived
dissociation energies, equilibrium distances, and harmonic vibrational
frequencies are known and (b) a composite computational approach based
on coupled-cluster theory with basis set extrapolation, inclusion
of coreāvalence correlation, and corrections for relativistic
and multireference effects. The latter correction was obtained from
internally contracted multireference coupled-cluster (icMRCC) theory.
This composite approach has been used to obtain the dissociation energies
and spectroscopic constants for the 60 molecules in our data set.
In accordance with previous studies on a subset of molecules, we find
that multireference corrections are rather small in many cases and
CCSDĀ(T) can provide accurate reference values, if the complete basis
set limit is explored. In addition, the multireference correction
improves the results in cases where CCSDĀ(T) is not a good approximation.
For a few cases, however, strong deviations from experiment persist,
which cannot be explained by the remaining error in the computational
approach. We suggest that these experimentally derived values require
careful revision. This also shows that reliable reference values for
benchmarking approximate computational methods are not always easily
accessible via experiment and accurate computations may provide an
alternative way to access them. In order to assess how the choice
of reference data affects benchmark studies, we tested 10 DFT functionals
for the molecules in the present data set against experimental and
calculated reference values. Despite the differences between these
two sets of reference values, we found that the ranking of the relative
performance of the DFT functionals is nearly independent of the chosen
reference
Intramolecular Charge-Transfer Excited-State Processes in 4ā(<i>N</i>,<i>N</i>āDimethylamino)benzonitrile: The Role of Twisting and the ĻĻ* State
The
structural processes leading to dual fluorescence of 4-(diĀmethylĀamino)ĀbenzoĀnitrile
in the gas phase and in acetonitrile solvent were investigated using
a combination of multireference configuration interaction (MRCI) and
the second-order algebraic diagrammatic construction (ADC(2)) methods.
Solvent effects were included on the basis of the conductor-like screening
model. The MRCI method was used for computing the nonadiabatic interaction
between the two lowest excited ĻĻ* states (S<sub>2</sub>(L<sub>a</sub>, CT) and S<sub>1</sub>(L<sub>b</sub>, LE)) and the
corresponding minimum on the crossing seam (MXS) whereas the ADC(2)
calculations were dedicated to assessing the role of the ĻĻ*
state. The MXS structure was found to have a twisting angle of ā¼50Ā°.
The branching space does not contain the twisting motion of the diĀmethylĀamino
group and thus is not directly involved in the deactivation process
from S<sub>2</sub> to S<sub>1</sub>. Polar solvent effects are not
found to have a significant influence on this situation. Applying <i>C<sub>s</sub></i> symmetry restrictions, the ADC(2) calculations
show that CCN bending leads to a strong stabilization and to significant
charge transfer (CT). Nevertheless, this structure is not a minimum
but converts to the local excitation (LE) structure on releasing the
symmetry constraint. These findings suggest that the main role in
the dynamics is played by the nonadiabatic interaction of the LE and
CT states and that the main source for the dual fluorescence is the
twisted internal charge-transfer state in addition to the LE state
New Polymorphs of Perylene:Tetracyanoquinodimethane Charge Transfer Cocrystals
We
report two hitherto unknown polymorphs of the charge transfer
(CT) cocrystal perylene:tetracyanoquinodimethane (TCNQ) grown by physical
vapor transport (PVT) in argon atmosphere. One of the polymorphs,
named Ī², has stoichiometry 1:1 and adds to the three known structures
with stoichiometry 1:1 (Ī±), 2:1, and 3:1. Interestingly, below
(280 Ā± 10) K the Ī² structure undergoes a phase transition
to what we refer to as the Ī³ polymorph, with halving of the
unit cell and reduction of symmetry from monoclinic to triclinic.
Both new crystal structures present two alternating stacks with different
intermolecular and intramolecular geometries. In stack SāI
the perylene molecules show substantial deviations from planarity,
with the angle between the naphthalene intramolecular moieties of
6.69Ā°, and with the perylene and TCNQ molecular centroids shifted
by 1.95 Ć
. In the second stack, S-II, the perylene is planar,
and the centroids almost coincident. Structural investigations on
bond length complemented by vibrational IR spectroscopy indicate that
in the new polymorphs the degree of charge transfer, Ļ, can
be 0 or 0.12. The higher value of ionicity to be due to donorāacceptor
pairs in the S-II, while molecules in S-I are closer to neutrality.
Thus, the ionicity of the donorāacceptor pair depends on the
stack and is comparable to that of the Ī± polymorph which we
redetermined as Ļ = 0.15 Ā± 0.05
Experimental Basicities of Phosphazene, Guanidinophosphazene, and Proton Sponge Superbases in the Gas Phase and Solution
Experimental
gas-phase superbasicity scale spanning 20 orders of
magnitude and ranging from bicyclic guanidine 7-methyl-1,5,7-triazabicyclo[4.4.0]Ādec-5-ene
to triguanidinophosphazenes and P<sub>3</sub> phosphazenes is presented
together with solution basicity data in acetonitrile and tetrahydrofuran.
The most basic compound in the scaleīøtriguanidinophosphazene
EtāNī»PĀ[Nī»CĀ(NMe<sub>2</sub>)<sub>2</sub>]<sub>3</sub>īøhas the highest experimental gas-phase basicity of
an organic base ever reported: 273.9 kcal mol<sup>ā1</sup>.
The scale includes besides the higher homologues of classical superbasic
phosphazenes and several guanidino-substituted phosphazenes also a
number of recently introduced bisphosphazene and bis-guanidino proton
sponges. This advancement was made possible by a newly designed Fourier
transform ion cyclotron resonance (ICR) mass spectrometry setup with
the unique ability to generate and control in the ICR cell sufficient
vapor pressures of two delicate compounds having low volatility, which
enables determining their basicity difference. The obtained experimental
gas-phase and solution basicity data are analyzed in terms of structural
and solvent effects and compared with data from theoretical calculations