6 research outputs found
Vapor-Induced Conversion of a Centrosymmetric Organic–Inorganic Hybrid Crystal into a Proton-Conducting Second-Harmonic-Generation-Active Material
Chemical responsivity in materials is essential to build
systems
with switchable functionalities. However, polarity-switchable materials
are still rare because inducing a symmetry breaking of the crystal
structure by adsorbing chemical species is difficult. In this study,
we demonstrate that a molecular organic–inorganic hybrid crystal
of (NEt4)2[MnN(CN)4] (1) undergoes polarity switching induced by water vapor and transforms
into a rare example of proton-conducting second-harmonic-generation-active
material. Centrosymmetric 1 transforms into noncentrosymmetric
polar 1·3H2O and 1·MeOH by accommodating water and methanol
molecules, respectively. However, only water vapor causes a spontaneous
single-crystal-to-single-crystal transition. Moreover, 1·3H2O shows proton conduction with
2.3 × 10–6 S/cm at 298 K and a relative humidity
of 80%
Employment Discrimination: Recent Developments in the Supreme Court (Symposium: The Supreme Court and Local Government Law: The 1992-93 Term)
At a symposium entitled, “The Supreme Court and Local Government Law; The 1992/93 Term”, Professor Eileen Kaufman spoke about the cases involving employment discrimination that were decided during that particular Term, Hazen Paper Company v. Biggins and St. Mary\u27s Honor Center v. Hicks. While Hazen is an age discrimination case and St. Mary\u27s is a Title VII case, they can be viewed as companion cases which serve to explain what an employment discrimination plaintiff must now establish when attempting to prove disparate treatment by indirect evidence. By way of preview, suffice it to say that plaintiff\u27s task has been made more difficult as a result of these decisions
Metal Dilution Effects on the Reverse Spin Transition in Mixed Crystals of Type [Co<sub>1–<i>x</i></sub>Zn<sub><i>x</i></sub>(C<sub>16</sub>-terpy)<sub>2</sub>](BF<sub>4</sub>)<sub>2</sub> (<i>x</i> = 0.1–0.7)
Metal dilution effects on reverse
spin transition (rST) in mixed crystals of type [Co<sub>1–<i>x</i></sub>Zn<sub><i>x</i></sub>Â(C<sub>16</sub>-terpy)<sub>2</sub>]Â(BF<sub>4</sub>)<sub>2</sub> (<i>x</i> = 0.1–0.7) were investigated by comparison with behavior
of [Co<sub>1–<i>x</i></sub>Fe<sub><i>x</i></sub>Â(C<sub>16</sub>-terpy)<sub>2</sub>]Â(BF<sub>4</sub>)<sub>2</sub> (<i>x</i> = 0.1–0.4). In the mixed crystals,
the Zn complexes increased rST temperatures linearly with increasing
values of <i>x</i>, without changing the hysteresis width,
while the Fe complexes decreased rST temperatures. Moreover, the strength
of the metal dilution effects in the CoZn mixed crystals is weaker
than what occurs in the CoFe mixed crystals
Metal Dilution Effects on the Reverse Spin Transition in Mixed Crystals of Type [Co<sub>1–<i>x</i></sub>Zn<sub><i>x</i></sub>(C<sub>16</sub>-terpy)<sub>2</sub>](BF<sub>4</sub>)<sub>2</sub> (<i>x</i> = 0.1–0.7)
Metal dilution effects on reverse
spin transition (rST) in mixed crystals of type [Co<sub>1–<i>x</i></sub>Zn<sub><i>x</i></sub>Â(C<sub>16</sub>-terpy)<sub>2</sub>]Â(BF<sub>4</sub>)<sub>2</sub> (<i>x</i> = 0.1–0.7) were investigated by comparison with behavior
of [Co<sub>1–<i>x</i></sub>Fe<sub><i>x</i></sub>Â(C<sub>16</sub>-terpy)<sub>2</sub>]Â(BF<sub>4</sub>)<sub>2</sub> (<i>x</i> = 0.1–0.4). In the mixed crystals,
the Zn complexes increased rST temperatures linearly with increasing
values of <i>x</i>, without changing the hysteresis width,
while the Fe complexes decreased rST temperatures. Moreover, the strength
of the metal dilution effects in the CoZn mixed crystals is weaker
than what occurs in the CoFe mixed crystals
Intermolecular Interaction Tuning of Spin-Crossover Iron(III) Complexes with Aromatic Counteranions
IronÂ(III) spin-crossover
(SCO) complexes [FeÂ(qsal)<sub>2</sub>]ÂBS·MeOH·H<sub>2</sub>O (<b>1</b>), [FeÂ(qsal)<sub>2</sub>]Â(NS)·MeOH (<b>2</b>), [FeÂ(qnal)<sub>2</sub>]Â(NS) (<b>3</b>), and [FeÂ(qnal)<sub>2</sub>]ÂPS·MeOH·CH<sub>2</sub>Cl<sub>2</sub> (<b>4</b>) (Hqsal, <i>N</i>-(8-quinolinyl)Âsalicylaldimine; Hqnal, <i>N</i>-(8-quinolinyl)-2-hydroxy-1-naphthaldimine; BS, benzenesulfonate;
NS, 1-naphthalenesulfonate; PS, 1-pyrenesulfonate) have been synthesized
and characterized by X-ray structure determinations and temperature-dependent
magnetic susceptibility measurements. The aromatic counteranions BS,
NS, and PS can be used for the tuning of intermolecular coupling through
a variety of weak interactions. All of the complexes show temperature-dependent
SCO behavior. but the light-induced excited spin-state trapping (LIESST)
effect was observed only for <b>1</b>, <b>3</b>, and <b>4</b> when the samples were illuminated (λ 808 nm) for 1
h at 5 K. In particular, 59% of the LS form of <b>1</b> was
converted to the metastable HS state by illumination, equal to the
highest degree of conversion yet known for LIESST in [FeÂ(qsal)<sub>2</sub>]<sup>+</sup> derivatives. The lack of a LIESST effect for <b>2</b> may be due to the relatively limited degree of interaction
between the cations and anions in the lattice, reflected in a much
longer minimum Fe···Fe separation in this complex in
comparison to the others
Super Dielectric Materials of Two-Dimensional TiO<sub>2</sub> or Ca<sub>2</sub>Nb<sub>3</sub>O<sub>10</sub> Nanosheet Hybrids with Reduced Graphene Oxide
High dielectric constants
(ε<sub>r</sub>) were observed in
two-dimensional composites obtained from stacking of reduced graphene
oxide (RGO) with Ca<sub>2</sub>Nb<sub>3</sub>O<sub>10</sub> and with
TiO<sub>2</sub> nanosheets. The relative dielectric permittivity values
of the composites were found to be higher than 10<sup>5</sup>, an
amazingly high value compared to that of similar GO composites and
other common dielectric materials. As a consequence, we considered
application of the hybrids as super dielectric materials in high capacitance
supercapacitors. The route to high capacitance involves the variation
of oxygen vacancies within the surface and in the closest bulk interior
of the hybrids. The effective charges generated throughout the metal
oxide and carbon–oxygen polar bonding systems within the graphene
skeleton appear to highly influence dielectric polarization. Moreover,
the replenishment of oxygen vacancies at the RGO and metal oxide interface
also contributes to polarizability