8 research outputs found
Droplet‐target laser‐plasma source for proximity x‐ray lithography
A compact, high-brightness and practically debris-free laser-plasma soft x-ray source for proximity x-ray lithography is described. The target of the source is small liquid fluorocarbon droplets injected into vacuum with a piezoelectrically vibrated nozzle. Emission from helium- and hydrogenlike fluorine in the 1.2-1.7 nm wavelength range was determined to similar to 2X10(12) photons/(sr-pulse). which corresponds to a conversion efficiency of similar to 5% of the 70 mJ laser pulse. Exposure of a copolymer of PMMA-MAA confirms the measured photon flux. Debris production was approximately 70 pg/sr pulse. The applicability of the source for dedicated lithography systems is discussed. (C) 1996 American Institute of Physics
Synthesis, Photophysical, and Biological Evaluation of Sulfated Polyglycerol Dendronized Perylenebisimides (PBIs)A Promising Platform for Anti-Inflammatory Theranostic Agents?
A set of four water-soluble perylene
bisimides (PBI) based on sulfated
polyglycerol (PGS) dendrons were developed, their photophysical properties
determined via UV/vis and fluorescence spectroscopy, and their performance
as possible anti-inflammatory agents evaluated via biological in vitro
studies. It could be shown that in contrast to charge neutral PG–PBIs
the introduction of the additional electrostatic repulsion forces
leads to a decrease in the dendron generation necessary for aggregation
suppression, allowing the preparation of PBIs with fluorescence quantum
yields of >95% with a considerable decreased synthetic effort.
Furthermore,
the values determined for L-selectin binding down to the nanomolar
range, their limited impact on blood coagulation, and their minor
activation of the complement system renders these systems ideal for
anti-inflammatory purposes
Methanol-Mediated Formation of an Iridium(III) NHC/Azolato Chelate Complex: An Experimental and Theoretical Study
One equivalent of methanol-d4 reacts
with the iridium(III)-carbonato-NHC complex [Ir(Cp*)(NHC-theo)(O2CO)] [1] containing an N-heterocyclic carbene
ligand with an N-tethered C8-iodotheophylline group (NHC-theo) to
form the iridium(III) chelate complex [Ir(Cp*)(theophyllinato^NHC)I]
[2] that bears a theophyllinato^NHC chelate ligand, an
iodo ligand, and the pentamethylcyclopentadienyl ligand (Cp*). The
methanol-d4 solvent is oxidized to formaldehyde-d2 that was identified by a detailed LC–MS
study using the 2,4-dinitrophenylhydrazine (DNPH) method. A plausible
rearrangement involving the unusual oxidative addition of the C8–I
bond of the theophylline group to an iridium(III) center to give a
seven-coordinate iridium(V) intermediate is supported by density functional
theory calculations
Methanol-Mediated Formation of an Iridium(III) NHC/Azolato Chelate Complex: An Experimental and Theoretical Study
One equivalent of methanol-d4 reacts
with the iridium(III)-carbonato-NHC complex [Ir(Cp*)(NHC-theo)(O2CO)] [1] containing an N-heterocyclic carbene
ligand with an N-tethered C8-iodotheophylline group (NHC-theo) to
form the iridium(III) chelate complex [Ir(Cp*)(theophyllinato^NHC)I]
[2] that bears a theophyllinato^NHC chelate ligand, an
iodo ligand, and the pentamethylcyclopentadienyl ligand (Cp*). The
methanol-d4 solvent is oxidized to formaldehyde-d2 that was identified by a detailed LC–MS
study using the 2,4-dinitrophenylhydrazine (DNPH) method. A plausible
rearrangement involving the unusual oxidative addition of the C8–I
bond of the theophylline group to an iridium(III) center to give a
seven-coordinate iridium(V) intermediate is supported by density functional
theory calculations
Frozen in Time: Kinetically Stabilized Amorphous Solid Dispersions of Nifedipine Stable after a Quarter Century of Storage
Kinetically stabilized
amorphous solid dispersions are inherently
metastable systems. Therefore, such systems are generally considered
prone to recrystallization. In some cases, the formation of crystals
will impact the bioavailability of the active pharmaceutical ingredient
in these formulations. Recrystallization therefore may present a significant
risk for patients as it potentially lowers the effective dose of the
pharmaceutical formulation. This study indicates that such metastable
formulations may indeed remain fully amorphous even after more than
two decades of storage under ambient conditions. Different formulations
of nifedipine stored for 25 years were compared with freshly prepared
samples. A thorough physicochemical characterization including polarized
light microscopy, differential scanning calorimetry, X-ray powder
diffraction, and transmission Raman spectroscopy was undertaken. This
in-depth characterization indicates no signs of recrystallization
in the stored samples. The observations presented here prove that
long-term stability of amorphous solid dispersions much beyond the
typical shelf life for pharmaceutical formulations is indeed possible
by kinetic stabilization alone. These findings implicate a reevaluation
of the propensity to recrystallize for kinetically stabilized amorphous
solid dispersions
Structural–Functional Role of Chloride in Photosystem II
Chloride binding in photosystem II (PSII) is essential for photosynthetic water oxidation. However, the functional roles of chloride and possible binding sites, during oxygen evolution, remain controversial. This paper examines the functions of chloride based on its binding site revealed in the X-ray crystal structure of PSII at 1.9 Å resolution. We find that chloride depletion induces formation of a salt-bridge between D2-K317 and D1-D61 that could suppress proton transfer to the lumen
Lanthanide Sensitization in II−VI Semiconductor Materials: A Case Study with Terbium(III) and Europium(III) in Zinc Sulfide Nanoparticles
International audienceThis work explores the sensitization of luminescent lanthanide Tb3+ and Eu3+ cations by electronic structure of zinc sulfide (ZnS) semiconductor nanoparticles. Excitation spectra collected while monitoring the lanthanide emission bands reveal that the ZnS nanoparticles act as an antenna for the sensitization of Tb3+ and Eu3+. The mechanism of lanthanide ion luminescence sensitization is rationalized in terms of an energy and charge transfer between trap sites and is based on a semiempirical model, proposed by Dorenbos and co-workers (Dorenbos, P. J. Phys.: Condens Matter 2003, 15, 8417-8434; J. Lumin. 2004, 108, 301-305; J. Lumin. 2005, 111, 89-104. Dorenbos, P.; van der Kolk, E. Appl. Phys. Lett. 2006, 89, 061122-1-061122-3; Opt. Mater. 2008, 30, 1052-1057. Dorenbos, P. J. Alloys Compd. 2009, 488, 568-573; references 1-6.) to describe the energy level scheme. This model implies that the mechanisms of luminescence sensitization of Tb3+ and Eu3+ in ZnS nanoparticles are different; namely, Tb3+ acts as a hole trap, whereas Eu3+ acts as an electron trap. Further testing of this model is made by extending the studies from ZnS nanoparticles to other II-VI semiconductor materials; namely, CdSe, CdS, and ZnSe
Structural, Electronic, and Magnetic Properties of Quasi-1D Quantum Magnets [Ni(HF2)(pyz)(2)]X (pyz = pyrazine; X = PF6-, SbF6-) Exhibiting Ni-FHF-Ni and Ni-pyz-Ni Spin Interactions
[Ni(HF(2))(pyz)(2)]X {pyz = pyrazine; X = PF(6)(-) (1), SbF(6)(-) (2)} were structurally characterized by synchrotron X-ray powder diffraction and found to possess axially compressed NiN(4)F(2) octahedra. At 298 K, 1 is monoclinic (C2/c) with unit cell parameters, a = 9.9481(3), b = 9.9421(3), c = 12.5953(4) Å, and β = 81.610(3)° while 2 is tetragonal (P4/nmm) with a = b = 9.9359(3) and c = 6.4471(2) Å and is isomorphic with the Cu-analogue. Infinite one-dimensional (1D) Ni-FHF-Ni chains propagate along the c-axis which are linked via μ-pyz bridges in the ab-plane to afford three-dimensional polymeric frameworks with PF(6)(-) and SbF(6)(-) counterions occupying the interior sites. A major difference between 1 and 2 is that the Ni-F-H bonds are bent (∼157°) in 1 but are linear in 2. Ligand field calculations (LFT) based on an angular overlap model (AOM), with comparison to the electronic absorption spectra, indicate greater π-donation of the HF(2)(-) ligand in 1 owing to the bent Ni-F-H bonds. Magnetic susceptibility data for 1 and 2 exhibit broad maxima at 7.4 and 15 K, respectively, and λ-like peaks in dχT/dT at 6.2 and 12.2 K that are ascribed to transitions to long-range antiferromagnetic order (T(N)). Muon-spin relaxation and specific heat studies confirm these T(N)'s. A comparative analysis of χ vs T to various 1D Heisenberg/Ising models suggests moderate antiferromagnetic interactions, with the primary interaction strength determined to be 3.05/3.42 K (1) and 5.65/6.37 K (2). However, high critical fields of 19 and 37.4 T obtained from low temperature pulsed-field magnetization data indicate that a single exchange constant (J(1D)) alone is insufficient to explain the data and that residual terms in the spin Hamiltonian, which could include interchain magnetic couplings (J(⊥)), as mediated by Ni-pyz-Ni, and single-ion anisotropy (D), must be considered. While it is difficult to draw absolute conclusions regarding the magnitude (and sign) of J(⊥) and D based solely on powder data, further support offered by related Ni(II)-pyz compounds and our LFT and density-functional theory (DFT) results lead us to a consistent quasi-1D magnetic description for 1 and 2