4 research outputs found
A novel fluorescent indicator displacement assay for sensing the anticancer drug gefitinib
<p>Fluorescent indicator displacement assays have become popular for converting synthetic receptors into optical sensors. We have now shown that a 1:2 host–guest complex between cucurbit[8]uril (Q[8]) and proflavine (PF) can be used as a fluorescent indicator for sensing the anticancer drug gefitinib. The 2PF@Q[8] complex can be used to detect gefitinib with high selectivity using fluorescence spectrometry with a detection limit of 6.63 × 10<sup>−8</sup> mol<sup>−L</sup>. The proposed sensing mechanism was investigated using <sup>1</sup>H nuclear magnetic resonance spectroscopy (<sup>1</sup>H NMR), isothermal titration calorimetry and electrospray ionisation mass spectrometry. The 2PF@Q[8] complex was shown to be suitable for imaging gefitinib in prostate cancer (PC3) cells, which may help to elucidate relevant biological processes at the molecular level. We have developed a novel F-IDA to detect the anticancer drug GEF with high selectivity. The new indicator has excellent selectivity and a low detection limit for GEF. We have also demonstrated that the F-IDA can be used for the practical determination of drugs in living cells.</p
Giant Magnetoelastic Effect at the Opening of a Spin-Gap in Ba<sub>3</sub>BiIr<sub>2</sub>O<sub>9</sub>
As compared to 3d (first-row) transition metals, the
4d and 5d
transition metals have much more diffuse valence orbitals. Quantum
cooperative phenomena that arise due to changes in the way these orbitals
overlap and interact, such as magnetoelasticity, are correspondingly
rare in 4d and 5d compounds. Here, we show that the 6H-perovskite
Ba<sub>3</sub>BiIr<sub>2</sub>O<sub>9</sub>, which contains 5d Ir<sup>4+</sup> (<i>S</i> = 1/2) dimerized into isolated face-sharing
Ir<sub>2</sub>O<sub>9</sub> bioctahedra, exhibits a giant magnetoelastic
effect, the largest of any known 5d compound, associated with the
opening of a spin-gap at <i>T</i>* = 74 K. The resulting
first-order transition is characterized by a remarkable 4% increase
in Ir–Ir distance and 1% negative thermal volume expansion.
The transition is driven by a dramatic change in the interactions
among Ir 5d orbitals, and represents a crossover between two very
different, competing, ground states: one that optimizes direct Ir–Ir
bonding (at high temperature), and one that optimizes Ir–O–Ir
magnetic superexchange (at low temperature)
Giant Magnetoelastic Effect at the Opening of a Spin-Gap in Ba<sub>3</sub>BiIr<sub>2</sub>O<sub>9</sub>
As compared to 3d (first-row) transition metals, the
4d and 5d
transition metals have much more diffuse valence orbitals. Quantum
cooperative phenomena that arise due to changes in the way these orbitals
overlap and interact, such as magnetoelasticity, are correspondingly
rare in 4d and 5d compounds. Here, we show that the 6H-perovskite
Ba<sub>3</sub>BiIr<sub>2</sub>O<sub>9</sub>, which contains 5d Ir<sup>4+</sup> (<i>S</i> = 1/2) dimerized into isolated face-sharing
Ir<sub>2</sub>O<sub>9</sub> bioctahedra, exhibits a giant magnetoelastic
effect, the largest of any known 5d compound, associated with the
opening of a spin-gap at <i>T</i>* = 74 K. The resulting
first-order transition is characterized by a remarkable 4% increase
in Ir–Ir distance and 1% negative thermal volume expansion.
The transition is driven by a dramatic change in the interactions
among Ir 5d orbitals, and represents a crossover between two very
different, competing, ground states: one that optimizes direct Ir–Ir
bonding (at high temperature), and one that optimizes Ir–O–Ir
magnetic superexchange (at low temperature)
Key Role of Bismuth in the Magnetoelastic Transitions of Ba<sub>3</sub>BiIr<sub>2</sub>O<sub>9</sub> and Ba<sub>3</sub>BiRu<sub>2</sub>O<sub>9</sub> As Revealed by Chemical Doping
The key role played by bismuth in
an average intermediate oxidation state in the magnetoelastic spin-gap
compounds Ba<sub>3</sub>BiRu<sub>2</sub>O<sub>9</sub> and Ba<sub>3</sub>BiIr<sub>2</sub>O<sub>9</sub> has been confirmed by systematically
replacing bismuth with La<sup>3+</sup> and Ce<sup>4+</sup>. Through
a combination of powder diffraction (neutron and synchrotron), X-ray
absorption spectroscopy, and magnetic properties measurements, we
show that Ru/Ir cations in Ba<sub>3</sub>BiRu<sub>2</sub>O<sub>9</sub> and Ba<sub>3</sub>BiIr<sub>2</sub>O<sub>9</sub> have oxidation states
between +4 and +4.5, suggesting that Bi cations exist in an unusual
average oxidation state intermediate between the conventional +3 and
+5 states (which is confirmed by the Bi L<sub>3</sub>-edge spectrum
of Ba<sub>3</sub>BiRu<sub>2</sub>O<sub>9</sub>). Precise measurements
of lattice parameters from synchrotron diffraction are consistent
with the presence of intermediate oxidation state bismuth cations
throughout the doping ranges. We find that relatively small amounts
of doping (∼10 at%) on the bismuth site suppress and then completely
eliminate the sharp structural and magnetic transitions observed in
pure Ba<sub>3</sub>BiRu<sub>2</sub>O<sub>9</sub> and Ba<sub>3</sub>BiIr<sub>2</sub>O<sub>9</sub>, strongly suggesting that the unstable
electronic state of bismuth plays a critical role in the behavior
of these materials