12 research outputs found
New Polymorph of Dehydroepiandrosterone Obtained via Cryomodification
A new anhydrous polymorph of dehydroepiandrosterone
(DHEA) is detected
in cryomodified powder samples and designated as form VII. The crystal
structure of form VII is determined from multiphase X-ray powder diffraction
(XRPD) data. Additionally, the unknown crystal structures of anhydrous
form III and the new monohydrated DHEA form designated as form S5
are also determined from multiphase XRPD data. To validate the crystal
structures III, VII, and S5, energy minimization with dispersion-corrected
density functional theory is performed in VASP. An extended list of
the DHEA forms with the known crystal structures, which now covers
anhydrous forms I, II, III, VI, and VII and solvated forms S1, S2,
S4 and S5, allows quantification of DHEA solid-state transformations
to be carried out
Structural Properties and Phase Transition of Exfoliated-Restacked Molybdenum Disulfide
The
product of exfoliation and restacking of MoS<sub>2</sub> in
acidic conditions is studied in detail using X-ray powder diffraction,
transmission electron microscopy (TEM), thermogravimetric analysis
(TGA), and differential scanning calorimetry (DSC). The temperature
dependence of powder patterns reveals that the heating of exfoliated-restacked
MoS<sub>2</sub> is a way to a new nanostructured MoS<sub>2</sub>-based
layered material that remains nanosized even upon heating to 850 °C.
Previously this material has been described as 2H-MoS<sub>2</sub>,
but according to the X-ray diffraction (XRD) data, its structure cannot
be correctly described by any of the âusualâ MoS<sub>2</sub> polytypes. A model of the structure of the material describing
its XRD patterns and thermal behavior is discussed in detail
Synthesis of thiazolo[3,2-<i>a</i>]pyridines via an unusual Mannich-type cyclization
<p>The Mannich-type reaction of <i>N</i>-methylmorpholinium 4-aryl-3-cyano-6-oxo-1,4,5,6-tetrahydropyridine-2-thiolates with 3-(1,3-benzodioxol-5-yl)-2-methylpropanal (ocean propanal) and <i>p</i>-toluidine afforded 7-aryl-2-(1,3-benzodioxol-5-ylmethyl)-2-methyl-3-[(4-methylphenyl)amino]-5-oxo-2,3,6,7-tetrahydro-5<i>H</i>-thiazolo[3,2-<i>a</i>]pyridine-8-carbonitriles in modest (25â46%) yields. The structure of the key compound was confirmed by X-ray crystal structure analysis.</p> <p></p
Stabilization of 1T-MoS<sub>2</sub> Sheets by Imidazolium Molecules in Self-Assembling Hetero-layered Nanocrystals
We report a facile, room-temperature
assembly of MoS<sub>2</sub>-based hetero-layered nanocrystals (NCs)
containing embedded monolayers
of imidazolium (Im), 1-butyl-3-methylÂimidÂazolium (BuMeIm),
2-phenylÂimidÂazolium, and 2-methylÂbenzÂimidÂazolium
molecules. The NCs are readily formed in water solutions by self-organization
of the negatively charged, chemically exfoliated 0.6 nm thick MoS<sub>2</sub> sheets and corresponding cationic imidazole moieties. As
evidenced by transmission electron microscopy, the obtained NCs are
anisotropic in shape, with thickness varying in the range 5â20
nm and lateral dimensions of hundreds of nanometers. The NCs exhibit
almost turbostratic stacking of the MoS<sub>2</sub> sheets, though
the local order is preserved in the orientation of the imidazolium
molecules with respect to the sulfide sheets. The atomic structure
of NCs with BuMeIm molecules was solved from powder X-ray diffraction
data assisted by density functional theory calculations. The performed
studies evidenced that the MoS<sub>2</sub> sheets of the NCs are of
the nonconventional 1T-MoS<sub>2</sub> (metallically conducting) structure.
The sheetsâ puckered outer surface is formed by the S atoms
and the positioning of the BuMeIm molecules follows the sheet nanorelief.
According to thermal analysis data, the presence of the BuMeIm cations
significantly increases the stability of the 1T-MoS<sub>2</sub> modification
and raises the temperature for its transition to the conventional
2H-MoS<sub>2</sub> (semiconductive) counterpart by âź70 °C
as compared to pure 1T-MoS<sub>2</sub> (âź100 °C). The
stabilizing interaction energy between inorganic and organic layers
was estimated as 21.7 kcal/mol from the calculated electron density
distribution. The results suggest a potential for the design of few-layer
electronic devices exploiting the charge transport properties of monolayer
thin MoS<sub>2</sub>
Electrostatic Origin of Stabilization in MoS<sub>2</sub>âOrganic Nanocrystals
Negatively
charged molybdenum disulfide layers form stable organicâinorganic
layered nanocrystals when reacted with organic cations in solution.
The reasons why this self-assembly process leads to a single-phase
compound with a well-defined interlayer distance in given conditions
are, however, poorly understood to date. Here, for the first time,
we quantify the interactions determining the cation packing and stability
of the MoS<sub>2</sub>âorganic nanocrystals and find that the
main contribution arises from Coulomb forces. The study was performed
on the series of new layered compounds of MoS<sub>2</sub> with naphthalene
derivatives, forming several distinct phases depending on reaction
conditions. Starting with structural models derived from powder X-ray
diffraction data and TEM, we evaluate their cohesion energy by modeling
layer separation with periodic PW-DFT-D calculations. The results
provide a reliable approach for estimation of the stability of MoS<sub>2</sub>-based heterolayered compounds
Stabilization of 1T-MoS<sub>2</sub> Sheets by Imidazolium Molecules in Self-Assembling Hetero-layered Nanocrystals
We report a facile, room-temperature
assembly of MoS<sub>2</sub>-based hetero-layered nanocrystals (NCs)
containing embedded monolayers
of imidazolium (Im), 1-butyl-3-methylÂimidÂazolium (BuMeIm),
2-phenylÂimidÂazolium, and 2-methylÂbenzÂimidÂazolium
molecules. The NCs are readily formed in water solutions by self-organization
of the negatively charged, chemically exfoliated 0.6 nm thick MoS<sub>2</sub> sheets and corresponding cationic imidazole moieties. As
evidenced by transmission electron microscopy, the obtained NCs are
anisotropic in shape, with thickness varying in the range 5â20
nm and lateral dimensions of hundreds of nanometers. The NCs exhibit
almost turbostratic stacking of the MoS<sub>2</sub> sheets, though
the local order is preserved in the orientation of the imidazolium
molecules with respect to the sulfide sheets. The atomic structure
of NCs with BuMeIm molecules was solved from powder X-ray diffraction
data assisted by density functional theory calculations. The performed
studies evidenced that the MoS<sub>2</sub> sheets of the NCs are of
the nonconventional 1T-MoS<sub>2</sub> (metallically conducting) structure.
The sheetsâ puckered outer surface is formed by the S atoms
and the positioning of the BuMeIm molecules follows the sheet nanorelief.
According to thermal analysis data, the presence of the BuMeIm cations
significantly increases the stability of the 1T-MoS<sub>2</sub> modification
and raises the temperature for its transition to the conventional
2H-MoS<sub>2</sub> (semiconductive) counterpart by âź70 °C
as compared to pure 1T-MoS<sub>2</sub> (âź100 °C). The
stabilizing interaction energy between inorganic and organic layers
was estimated as 21.7 kcal/mol from the calculated electron density
distribution. The results suggest a potential for the design of few-layer
electronic devices exploiting the charge transport properties of monolayer
thin MoS<sub>2</sub>
Electrostatic Origin of Stabilization in MoS<sub>2</sub>âOrganic Nanocrystals
Negatively
charged molybdenum disulfide layers form stable organicâinorganic
layered nanocrystals when reacted with organic cations in solution.
The reasons why this self-assembly process leads to a single-phase
compound with a well-defined interlayer distance in given conditions
are, however, poorly understood to date. Here, for the first time,
we quantify the interactions determining the cation packing and stability
of the MoS<sub>2</sub>âorganic nanocrystals and find that the
main contribution arises from Coulomb forces. The study was performed
on the series of new layered compounds of MoS<sub>2</sub> with naphthalene
derivatives, forming several distinct phases depending on reaction
conditions. Starting with structural models derived from powder X-ray
diffraction data and TEM, we evaluate their cohesion energy by modeling
layer separation with periodic PW-DFT-D calculations. The results
provide a reliable approach for estimation of the stability of MoS<sub>2</sub>-based heterolayered compounds
Electronic Structure of Cesium Butyratouranylate(VI) as Derived from DFT-assisted Powder Xâray Diffraction Data
Investigation of chemical bonding
and electronic structure of coordination
polymers that do not form high-quality single crystals requires special
techniques. Here, we report the molecular and electronic structure
of the first cesium butyratouranylate, CsÂ[UO<sub>2</sub>(<i>n</i>-C<sub>3</sub>H<sub>7</sub>COO)<sub>3</sub>]Â[UO<sub>2</sub>(<i>n</i>-C<sub>3</sub>H<sub>7</sub>COO)Â(OH)Â(H<sub>2</sub>O)], as
obtained from DFT-assisted powder X-ray diffraction data because of
the low quality of crystalline sample. The topological analysis of
the charge distribution within the quantum theory of atoms-in-molecules
(QTAIM) space partitioning and the distribution of electron localization
function (ELF) is reported. The constancy of atomic domain of the
uraniumÂ(VI) atom at different coordination numbers (7 and 8) and the
presence of three ELF maxima in equatorial plane of an uranyl cation
attributed to the 6s and 6p electrons were demonstrated for the first
time. Details of methodologies applied for additional verification
of the correctness of powder XRD refinement (Voronoi atomic descriptors
and the Morse restraints) are discussed
Electronic Structure of Cesium Butyratouranylate(VI) as Derived from DFT-assisted Powder Xâray Diffraction Data
Investigation of chemical bonding
and electronic structure of coordination
polymers that do not form high-quality single crystals requires special
techniques. Here, we report the molecular and electronic structure
of the first cesium butyratouranylate, CsÂ[UO<sub>2</sub>(<i>n</i>-C<sub>3</sub>H<sub>7</sub>COO)<sub>3</sub>]Â[UO<sub>2</sub>(<i>n</i>-C<sub>3</sub>H<sub>7</sub>COO)Â(OH)Â(H<sub>2</sub>O)], as
obtained from DFT-assisted powder X-ray diffraction data because of
the low quality of crystalline sample. The topological analysis of
the charge distribution within the quantum theory of atoms-in-molecules
(QTAIM) space partitioning and the distribution of electron localization
function (ELF) is reported. The constancy of atomic domain of the
uraniumÂ(VI) atom at different coordination numbers (7 and 8) and the
presence of three ELF maxima in equatorial plane of an uranyl cation
attributed to the 6s and 6p electrons were demonstrated for the first
time. Details of methodologies applied for additional verification
of the correctness of powder XRD refinement (Voronoi atomic descriptors
and the Morse restraints) are discussed
Synthesis of Isomeric Isothiazolo[4â˛,3â˛:4,5]- and Isothiazolo[4â˛,5â˛:4,5]thieno[3,2â<i>b</i>]pyrano[2,3â<i>d</i>]pyridines by Combination of Domino Reactions
Isothiazolothienopyridines
have been prepared by a domino reaction
(the S<sub>N</sub>2 reaction â the ThorpeâZiegler reaction
â the ThorpeâGuareschi reaction type) from disodium
4-cyanoisothiazole-3,5-dithiolate. By changing the order of addition
of the alkylation reagents in the reaction with disodium 4-cyanoisothiazole-3,5-dithiolate
both possible isomers of the isothiazolothienopyridines are synthesized.
These isomers were further used in three-component domino reaction
(the Knoevenagel reaction â the Michael reaction â the
hetero-ThorpeâZiegler reaction type) to obtain wide range of
isomeric isothiazolothienopyranopyridines