3 research outputs found
Evidence for Point Transformations in Photoactive Molecular Crystals by the Photoinduced Creation of Diffuse Diffraction Patterns
Time-resolved diffuse X-ray scattering is one powerful
method for
monitoring the progression from the creation of local structural changes
inside a crystalline material up to the transformation of the whole
crystalline bulk. In this work, we study the mechanism of phototransformation
of a molecular crystal by time-resolved diffuse X-ray scattering.
Here, an optical excitation source, like a pulsed laser, initiates
structural transformations which are monitored by X-ray scattering
techniques. We have studied the dimerization process of the molecular
switch α-styrylpyrylium (trifluoromethanesulfonate) TFMS, in
particular for understanding whether cooperative effects influence
the changes of the structure in the bulk and its periodicity. Upon
illumination with optical light, α-styrylpyrylium TFMS instantaneously
photoswitches. Depending on the optical fluence, X-ray diffuse planes
are observed prior to phototransformation of the bulk. In the early
stages of transformation, the analysis reveals systems of randomly
distributed islands of product clusters with gradual growth in size
and amount. The degree of transformation follows the optical excitation
profile, i.e., the spatial absorption of the laser beam. In the present
studies, no influence of cooperativity on the photodimerization process
has been found
Materials Properties of Ultra-Incompressible Re<sub>2</sub>P
In situ high-pressure X-ray powder diffraction measurements
on
Re<sub>2</sub>P up to 37.0 GPa at ambient temperature in diamond-anvil
cells were carried out at two different synchrotron facilities (ESRF
and DESY). The compressibility of Re<sub>2</sub>P (<i>Pnma</i>, no. 62, <i>a</i> = 5.5464(17), <i>b</i> = 2.9421(8), <i>c</i> = 10.0483(35) Å, <i>V</i> = 163.97(9) Å<sup>3</sup>, <i>Z</i> = 4, <i>R</i><sub>p</sub> = 0.1008, <i>wR</i><sub>p</sub> =
0.1341 at ambient conditions) was investigated and resulted in a bulk
modulus of <i>B</i><sub>0</sub> = 320(10) GPa after fitting the experimental <i>p</i>–<i>V</i> data to a second- and third-order Birch–Murnaghan
equation of state. In addition, the determined bulk modulus is compared
to values obtained from an Eulerian strain versus normalized stress
plot with values ranging form 315(7) to 321(15) GPa. These experimental
findings are confirmed by density functional theory (DFT)-calculations
ranking Re<sub>2</sub>P among ultra-incompressible materials. However,
the Vickers hardness of a high-pressure sintered Re<sub>2</sub>P–Re<sub><i>x</i></sub>C<sub><i>y</i></sub> composite
material in the asymptotic hardness region was found to be of only
13(2) GPa. Electrical conductivity measurements indicate that metallic
Re<sub>2</sub>P exhibits Pauli-paramagnetism. Analysis of temperature-dependent
in situ X-ray diffractometry reveals an approximately isotropic expansion
of the lattice parameters with a thermal expansion coefficient of
(α(<i>V</i>) = 28.5–32.8(2)·10<sup>–6</sup> K<sup>–1</sup>)
High-Pressure Synthesis of β‑Ir<sub>4</sub>B<sub>5</sub> and Determination of the Compressibility of Various Iridium Borides
A new
iridium boride, β-Ir<sub>4</sub>B<sub>5</sub>, was
synthesized under high-pressure/high-temperature conditions of 10.5
GPa and 1500 °C in a multianvil press with a Walker-type module.
The new modification β-Ir<sub>4</sub>B<sub>5</sub> crystallizes
in a new structure type in the orthorhombic space group <i>Pnma</i> (no. 62) with the lattice parameters <i>a</i> = 10.772(2)
Å, <i>b</i> = 2.844(1) Å, and <i>c</i> = 6.052(2) Å with <i>R</i>1 = 0.0286, <i>wR</i>2 = 0.0642 (all data), and <i>Z</i> = 2. The structure
was determined by single-crystal X-ray and neutron powder diffraction
on samples enriched in <sup>11</sup>B. The compound is built up by
an alternating stacking of boron and iridium layers with the sequence
ABA′B′. Additionally, microcalorimetry, hardness, and
compressibility measurements of the binary iridium borides α-Ir<sub>4</sub>B<sub>5</sub>, β-Ir<sub>4</sub>B<sub>5</sub>, Ir<sub>5</sub>B<sub>4</sub>, hexagonal Ir<sub>4</sub>B<sub>3–<i>x</i></sub> and orthorhombic Ir<sub>4</sub>B<sub>3–<i>x</i></sub> were carried out and theoretical investigations
based on density function theory (DFT) were employed to complement
a comprehensive evaluation of structure–property relations.
The incorporation of boron into the structures does not enhance the
compressibility but leads to a significant reduction of the bulk moduli
and elastic constants in comparison to elemental iridium