26 research outputs found
Modulation of Ligand-Field Parameters by Heme Ruffling in Cytochromes <i>c</i> Revealed by EPR Spectroscopy
Electron paramagnetic resonance (EPR) spectra of variants
of <i>Hydrogenobacter thermophilus</i> cytochrome <i>c</i><sub>552</sub> (<i>Ht c</i>-552) and <i>Pseudomonas
aeruginosa</i> cytochrome <i>c</i><sub>551</sub> (<i>Pa c</i>-551) are analyzed to determine the effect of heme ruffling
on ligand-field parameters. Mutations introduced at positions 13 and
22 in <i>Ht c</i>-552 were previously demonstrated to influence
hydrogen bonding in the proximal heme pocket and to tune reduction
potential (<i>E</i><sub>m</sub>) over a range of 80 mV [Michel,
L. V.; Ye, T.; Bowman, S. E. J.; Levin, B. D.; Hahn, M. A.; Russell,
B. S.; Elliott, S. J.; Bren, K. L. <i>Biochemistry</i> <b>2007</b>, <i>46</i>, 11753ā11760]. These mutations
are shown here to also increase heme ruffling as <i>E</i><sub>m</sub> decreases. The primary effect on electronic structure
of increasing heme ruffling is found to be a decrease in the axial
ligand-field term Ī/Ī», which is proposed to arise from
an increase in the energy of the d<sub><i>xy</i></sub> orbital.
Mutations at position 7, previously demonstrated to influence heme
ruffling in <i>Pa c</i>-551 and <i>Ht c</i>-552,
are utilized to test this correlation between molecular and electronic
structure. In conclusion, the structure of the proximal heme pocket
of cytochromes <i>c</i> is shown to play a role in determining
heme conformation and electronic structure
Fe<sub>3</sub>O<sub>4</sub> Nanocrystals Tune the Magnetic Regime of the Fe/Ni Molecular Magnet: A New Class of Magnetic Superstructures
A new
class of organometallicāinorganic magnetic material
was engineered by a sonochemically assisted self-assembly process
between magnetite nanoparticles (biogenic Fe<sub>3</sub>O<sub>4</sub>, hard constituent) functionalized with isonicotinic acid and a metamagnetic
organometallic complex ([NiĀ(en)<sub>2</sub>]<sub>3</sub>[FeĀ(CN)<sub>6</sub>]<sub>2</sub>Ā·3H<sub>2</sub>O, soft constituent). In
such bottom-up methodology, hard and soft counterparts form well-organized
microdimensional clusters that showed morphological fingerprints and
magnetic behavior clearly distinct from those of the initial building
units. In the engineered softāhard material, the magnetite
nanocrystals induced ferromagnetic ordering at room temperature of
closer contact layers of [NiĀ(en)<sub>2</sub>]<sub>3</sub>[FeĀ(CN)<sub>6</sub>]<sub>2</sub>Ā·3H<sub>2</sub>O, thus demonstrating the
ability to sensibly modify the [NiĀ(en)<sub>2</sub>]<sub>3</sub>[FeĀ(CN)<sub>6</sub>]<sub>2</sub>Ā·3H<sub>2</sub>O paramagnetic regime. The
magnetic ordering of [NiĀ(en)<sub>2</sub>]<sub>3</sub>[FeĀ(CN)<sub>6</sub>]<sub>2</sub>Ā·3H<sub>2</sub>O was triggered by the intrinsic
local field of the hard magnetic nanocrystals, which resembled, to
some extent, the effects promoted by large, external magnetic fields
Solvent Controlled Generation of Spin Active Polarons in Two-Dimensional Material under UV Light Irradiation
Polarons belong to
a class of extensively studied quasiparticles
that have found applications spanning diverse fields, including charge
transport, colossal magnetoresistance, thermoelectricity, (multi)ferroism,
optoelectronics, and photovoltaics. It is notable, though, that their
interaction with the local environment has been overlooked so far.
We report an unexpected phenomenon of the solvent-induced generation
of polaronic spin active states in a two-dimensional (2D) material
fluorographene under UV light. Furthermore, we present compelling
evidence of the solvent-specific nature of this phenomenon. The generation
of spin-active states is robust in acetone, moderate in benzene, and
absent in cyclohexane. Continuous wave X-band electron paramagnetic
resonance (EPR) spectroscopy experiments revealed a massive increase
in the EPR signal for fluorographene dispersed in acetone under UV-light
irradiation, while the system did not show any significant signal
under dark conditions and without the solvent. The patterns appeared
due to the generation of transient magnetic photoexcited states of
polaronic character, which encompassed the net 1/2 spin moment detectable
by EPR. Advanced ab initio calculations disclosed that polarons are
plausibly formed at radical sites in fluorographene which interact
strongly with acetone molecules in their vicinity. Additionally, we
present a comprehensive scenario for multiplication of polaronic spin
active species, highlighting the pivotal role of the photoinduced
charge transfer from the solvent to the electrophilic radical centers
in fluorographene. We believe that the solvent-tunable polaron formation
with the use of UV light and an easily accessible 2D nanomaterial
opens up a wide range of future applications, ranging from molecular
sensing to magneto-optical devices
Solvent Controlled Generation of Spin Active Polarons in Two-Dimensional Material under UV Light Irradiation
Polarons belong to
a class of extensively studied quasiparticles
that have found applications spanning diverse fields, including charge
transport, colossal magnetoresistance, thermoelectricity, (multi)ferroism,
optoelectronics, and photovoltaics. It is notable, though, that their
interaction with the local environment has been overlooked so far.
We report an unexpected phenomenon of the solvent-induced generation
of polaronic spin active states in a two-dimensional (2D) material
fluorographene under UV light. Furthermore, we present compelling
evidence of the solvent-specific nature of this phenomenon. The generation
of spin-active states is robust in acetone, moderate in benzene, and
absent in cyclohexane. Continuous wave X-band electron paramagnetic
resonance (EPR) spectroscopy experiments revealed a massive increase
in the EPR signal for fluorographene dispersed in acetone under UV-light
irradiation, while the system did not show any significant signal
under dark conditions and without the solvent. The patterns appeared
due to the generation of transient magnetic photoexcited states of
polaronic character, which encompassed the net 1/2 spin moment detectable
by EPR. Advanced ab initio calculations disclosed that polarons are
plausibly formed at radical sites in fluorographene which interact
strongly with acetone molecules in their vicinity. Additionally, we
present a comprehensive scenario for multiplication of polaronic spin
active species, highlighting the pivotal role of the photoinduced
charge transfer from the solvent to the electrophilic radical centers
in fluorographene. We believe that the solvent-tunable polaron formation
with the use of UV light and an easily accessible 2D nanomaterial
opens up a wide range of future applications, ranging from molecular
sensing to magneto-optical devices
Triggering Two-Step Spin Bistability and Large Hysteresis in Spin Crossover Nanoparticles via Molecular Nanoengineering
The local entrapment
of the spin crossover complex FeĀ(II)-trisĀ[2-(2ā²-pyridyl)Ābenzimidazole]
into the pluronic polymeric matrix (P123, PEG20āPPG70āPEG20,
MW ā¼ 5800) yielded the formation of magnetic nanoparticles
of ā¼26 nm (SCO-Np). Formation of SCO-Np was driven by the emergence
of noncovalent interactions between the aromatic āNH group
of the benzimidazole moieties present in FeĀ(II)-trisĀ[2-(2ā²-pyridyl)Ābenzimidazole]
with the aliphatic ether (āOā) groups of the pluronic
polymeric matrix. The nanoparticles show spin crossover behavior,
two-step spin bistability, and wide magnetic hysteresis, expressed
in the temperature range of 170ā280 K (Ī<i>T</i><sub>max</sub> = 38 K). The neat SCO molecules, FeĀ(II)-trisĀ[2-(2ā²-pyridyl)Ābenzimidazole],
on the contrary show only first-order spin transition and negligible
hysteresis. The developed matrix-confinement approach of SCO molecules
shown in this work yielded an unprecedented and significant improvement
of the magnetic cooperativity compared to the neat spin crossover
system, despite the decreased dimension of the magnetic domain in
the nanosized architecture
UV-Vis spectra of reconstituted R2F.
<p>(A) UV-Vis spectrum of 75 ĀµM R2F prior to reconstitution (dark-yellow line), R2F reconstituted with ferrous iron (blue line), and after incubation with 4 mM HU for 5 min (red line) at room temperature. (B) UV-Vis spectrum of 50 ĀµM Mn<sup>II</sup><sub>2</sub>-R2F reconstituted with 25 ĀµM of NrdI<sub>hq</sub> and O<sub>2</sub> (g) (blue line), 50 ĀµM Mn<sup>II</sup><sub>2</sub>-R2F with 25 ĀµM of NrdI<sub>ox</sub> (dark-yellow line), and manganese reconstituted R2F treated with 4 mM HU for 5 min at room temperature (red line).</p
Zero-Valent Iron Nanoparticles with Unique Spherical 3D Architectures Encode Superior Efficiency in Copper Entrapment
The
large-scale preparation of spherical condensed-type superstructures
of zero-valent iron (nZVI), obtained by controlled solid-state reaction
through a morphologically conserved transformation of a magnetite
precursor, is herein reported. The formed 3D nanoarchitectures (S-nZVI)
exhibit enhanced entrapment efficiency of heavy metal pollutants,
such as copper, compared to all previously tested materials reported
in the literature, thus unveiling the relevance in the materialās
design of the morphological variable. The superior removal efficiency
of these mesoporous S-nZVI superstructures is linked to their extraordinary
ability to couple effectively processes such as reduction and sorption
of the metal pollutant
Resonance Raman parameters for the Fe(III)-O-Fe(III) protein sites and phenoxyl Ī½<sub>7a</sub> bands of different RNR proteins.
<p>Resonance Raman parameters for the Fe(III)-O-Fe(III) protein sites and phenoxyl Ī½<sub>7a</sub> bands of different RNR proteins.</p
The Mn-substituted R2F-protein from <i>C. ammoniagenes</i> (PDB code 3MJO) [<b>26</b>] (A). and sketch of themolecular structure of the tyrosyl radical (B).
<p>In panel (A) the numbers in bold represent atomic distances (Ć
). The structure in (B) describes the dihedral angle Īø (C6-C1-CĪ²-CĪ±) used to illustrate the orientation of the Ī±-carbon: Īøā=ā0Ā° corresponds to the Ī±-carbon in the plane of the phenoxyl ring, while Īøā=ā90Ā° is perpendicular to the plane.</p
Spin-density distribution of an isolated tyrosyl radical obtained by density functional theory (DFT/UB3LYP/6-311++G(d,p) in gas phase, neutral form after geometry optimization (2>ā=ā0.7507, the dihedral angle Īø was constrained to 60Ā°).
<p>In this constrained conformation, the calculated atomic spin densities (from Mulliken population analyses) reveal much larger positive values located on H(Ī²1) with respect to the H(Ī²2) proton.</p