3 research outputs found
Study of Optical and Magnetic Properties of Graphene-Wrapped ZnO Nanoparticle Hybrids
In this work, we
report a one-step method for the preparation of
graphene-wrapped zinc oxide (ZnO) nanoparticle (NP) (ZnO@G) hybrids.
These hybrids are characterized by transmission electron microscopy,
X-ray diffraction, Raman spectroscopy, optical absorption measurements,
photoluminescence (PL) emission spectroscopy, and <i>M</i>ā<i>H</i> hysteresis measurements. All results reveal
that the ZnO NPs are entirely covered with graphene sheets. In the
PL spectra, the quenching of the band gap emission and the enhanced
green emission serve as evidence of the electron transfer from the
ZnO NPs to the graphene layer. The increase of the room-temperature
magnetization of the hybrid, compared to pure ZnO NPs, is due to the
increasing defect concentration. We suggest a band diagram model that
accounts for these observations. We present the simple wet-chemical
synthesis procedure to open a new way for the synthesis of NPāgraphene
hybrid systems having magnetic properties giving the large manifold
potential application
Structures, Magnetochemistry, Spectroscopy, Theoretical Study, and Catechol Oxidase Activity of Dinuclear and Dimer-of-Dinuclear Mixed-Valence Mn<sup>III</sup>Mn<sup>II</sup> Complexes Derived from a Macrocyclic Ligand
The
work in this paper presents syntheses, characterization, magnetic
properties (experimental and density functional theoretical), catecholase
activity, and electrospray ionization mass spectroscopic (ESI-MS positive)
studies of two mixed-valence dinuclear Mn<sup>III</sup>Mn<sup>II</sup> complexes, [Mn<sup>III</sup>Mn<sup>II</sup>LĀ(Ī¼-O<sub>2</sub>CMe)Ā(H<sub>2</sub>O)<sub>2</sub>]Ā(ClO<sub>4</sub>)<sub>2</sub>Ā·H<sub>2</sub>OĀ·MeCN (<b>1</b>) and [Mn<sup>III</sup>Mn<sup>II</sup>LĀ(Ī¼-O<sub>2</sub>CPh)Ā(MeOH)Ā(ClO<sub>4</sub>)]Ā(ClO<sub>4</sub>) (<b>2</b>), and a Mn<sup>III</sup>Mn<sup>II</sup>Mn<sup>II</sup>Mn<sup>III</sup> complex, [{Mn<sup>III</sup>Mn<sup>II</sup>LĀ(Ī¼-O<sub>2</sub>CEt)Ā(EtOH)}<sub>2</sub>(Ī¼-O<sub>2</sub>CEt)]Ā(ClO<sub>4</sub>)<sub>3</sub> (<b>3</b>), derived from the Robson-type
macrocycle H<sub>2</sub>L, which is the [2 + 2] condensation product
of 2,6-diformyl-4-methylphenol and 2,2-dimethyl-1,3-diaminopropane.
In <b>1</b> and <b>2</b> and in two Mn<sup>III</sup>Mn<sup>II</sup> units in <b>3</b>, the two metal centers are bridged
by a bisĀ(Ī¼-phenoxo)-Ī¼-carboxylate moiety. The two Mn<sup>II</sup> centers of the two Mn<sup>III</sup>Mn<sup>II</sup> units
in <b>3</b> are bridged by a propionate moiety, and therefore
this compound is a dimer of two dinuclear units. The coordination
geometry of the Mn<sup>III</sup> and Mn<sup>II</sup> centers are JahnāTeller
distorted octahedral and distorted trigonal prism, respectively. Magnetic
studies reveal weak ferro- or antiferromagnetic interactions between
the Mn<sup>III</sup> and Mn<sup>II</sup> centers in <b>1</b> (<i>J</i> = +0.08 cm<sup>ā1</sup>), <b>2</b> (<i>J</i> = ā0.095 cm<sup>ā1</sup>), and <b>3</b> (<i>J</i><sub>1</sub> = +0.015 cm<sup>ā1</sup>). A weak antiferromagnetic interaction (<i>J</i><sub>2</sub> = ā0.20 cm<sup>ā1</sup>) also exists between the Mn<sup>II</sup> centers in <b>3</b>. DFT methods properly reproduce
the nature of the exchange interactions present in such systems. A
magneto-structural correlation based on MnāO bridging distances
has been proposed to explain the different sign of the exchange coupling
constants. Utilizing 3,5-di-<i>tert</i>-butyl catechol (3,5-DTBCH<sub>2</sub>) as the substrate, catecholase activity of all the three
complexes has been checked in MeCN and MeOH, revealing that all three
are active catalysts with <i>K</i><sub>cat</sub> values
lying in the range 7.5ā64.7 h<sup>ā1</sup>. Electrospray
ionization mass (ESI-MS positive) spectra of the complexes <b>1</b>ā<b>3</b> have been recorded in MeCN solutions, and
the positive ions have been well characterized. ESI-MS positive spectrum
of complex <b>1</b> in presence of 3,5-DTBCH<sub>2</sub> has
also been recorded, and a positive ion, [Mn<sup>III</sup>Mn<sup>II</sup>LĀ(Ī¼-3,5-DTBC<sup>2ā</sup>)]<sup>+</sup>, having most
probably a bridging catecholate moiety has been identified
A Series of M<sup>II</sup>Cu<sup>II</sup><sub>3</sub> Stars (M = Mn, Ni, Cu, Zn) Exhibiting Unusual Magnetic Properties
The
work in this report describes the syntheses, electrospray ionization
mass spectromtery, structures, and experimental and density functional
theoretical (DFT) magnetic properties of four tetrametallic stars
of composition [M<sup>II</sup>(Cu<sup>II</sup>L)<sub>3</sub>]Ā(ClO<sub>4</sub>)<sub>2</sub> (<b>1</b>, M = Mn; <b>2</b>, M =
Ni; <b>3</b>, M = Cu; <b>4</b>, M = Zn) derived from a
single-compartment Schiff base ligand, <i>N</i>,<i>N</i>ā²-bisĀ(salicylidene)-1,4-butanediamine (H<sub>2</sub>L), which is the [2 + 1] condensation product of salicylaldehyde
and 1,4-diaminobutane. The central metal ion (Mn<sup>II</sup>, Ni<sup>II</sup>, Cu<sup>II</sup>, or Zn<sup>II</sup>) is linked with two
Ī¼<sub>2</sub>-phenoxo bridges of each of the three [Cu<sup>II</sup>L] moieties, and thus the central metal ion is encapsulated in between
three [Cu<sup>II</sup>L] units. The title compounds are rare or sole
examples of stars having these metal-ion combinations. In the cases
of <b>1</b>, <b>3</b>, and <b>4</b>, the four metal
ions form a centered isosceles triangle, while the four metal ions
in <b>2</b> form a centered equilateral triangle. Both the variable-temperature
magnetic susceptibility and variable-field magnetization (at 2ā10
K) of <b>1</b>ā<b>3</b> have been measured and
simulated contemporaneously. While the Mn<sup>II</sup>Cu<sup>II</sup><sub>3</sub> compound <b>1</b> exhibits ferromagnetic interaction
with <i>J</i> = 1.02 cm<sup>ā1</sup>, the Ni<sup>II</sup>Cu<sup>II</sup><sub>3</sub> compound <b>2</b> and Cu<sup>II</sup>Cu<sup>II</sup><sub>3</sub> compound <b>3</b> exhibit
antiferromagnetic interaction with <i>J</i> = ā3.53
and ā35.5 cm<sup>ā1</sup>, respectively. Variable-temperature
magnetic susceptibility data of the Zn<sup>II</sup>Cu<sup>II</sup><sub>3</sub> compound <b>4</b> indicate very weak antiferromagnetic
interaction of ā1.4 cm<sup>ā1</sup>, as expected. On
the basis of known correlations, the magnetic properties of <b>1</b>ā<b>3</b> are unusual; it seems that ferromagnetic
interaction in <b>1</b> and weak/moderate antiferromagnetic
interaction in <b>2</b> and <b>3</b> are possibly related
to the distorted coordination environment of the peripheral copperĀ(II)
centers (intermediate between square-planar and tetrahedral). DFT
calculations have been done to elucidate the magnetic properties.
The DFT-computed <i>J</i> values are quantitatively (for <b>1</b>) or qualitatively (for <b>2</b> and <b>3</b>) matched well with the experimental values. Spin densities and magnetic
orbitals (natural bond orbitals) correspond well with the trend of
observed/computed magnetic exchange interactions