5 research outputs found
Probing Axial Water Bound to Copper in Tutton Salt Using Single Crystal <sup>17</sup>O‑ESEEM Spectroscopy
Electron spin–echo envelope
modulation (ESEEM) signals attributed
to axial water bound to Cu<sup>2+</sup> have been detected and analyzed
in CuÂ(II)-doped <sup>17</sup>O-water-enriched potassium zinc sulfate
hexahydrate (Tutton salt) crystals. The magnetic field orientation
dependences of low frequency modulations were measured to fit hyperfine
and quadrupole coupling tensors of a <sup>17</sup>O (<i>I</i> = <sup>5</sup>/<sub>2</sub>) nucleus. The hyperfine tensor (<i>A</i><sub><i>xx</i></sub>, <i>A</i><sub><i>yy</i></sub>, <i>A</i><sub><i>zz</i></sub>: 0.13, 0.23, −3.81 MHz) exhibits almost axial symmetry
with the largest value directed normal to the metal equatorial plane
in the host structure. Comparisons with quantum chemical calculations
position this nucleus about 2.3 Ã… from the copper. The isotropic
coupling (−1.15 MHz) is small and reflects the weak axial water
interaction with a d<sub>x2‑y2</sub> unshared orbital of copper.
The <sup>17</sup>O-water quadrupole interaction parameters (<i>e</i><sup>2</sup><i>qQ</i>/<i>h</i> = 6.4
MHz and η = 0.93) are close to the average of those found in
a variety of solid hydrates. In addition, the coupling tensor directions
correlate very closely with the O8 water geometry, with the maximum
quadrupole direction 3° from the water plane normal, and its
minimum coupling about 2° from the H–H direction. In almost
all previous magnetic resonance <sup>17</sup>O-water studies, the
quadrupole tensor orientation was based on theoretical considerations.
This work represents one of the few experimental confirmations of
its principal axis frame. When Cu<sup>2+</sup> dopes into the Tutton
salt, a Jahn–Teller distortion interchanges the relative long
and intermediate metal O7 and O8 bond lengths of the zinc host. Therefore,
only those unit cells containing the impurity conform to the pure
copper Tutton structure. This study provides further support for this
model. Moreover, coupling interactions from distant H<sub>2</sub><sup>17</sup>O such as in the present case have important implications
in studies of copper enzymes and proteins where substrates have been
proposed to displace weakly bound water in the active site
Models for Copper Dynamic Behavior in Doped Cadmium dl-Histidine Crystals: Electron Paramagnetic Resonance and Crystallographic Analysis
Electron
paramagnetic resonance and crystallographic studies of copper-doped cadmium dl-histidine, abbreviated as CdDLHis, were undertaken to gain further
understanding on the relationship between site structure and dynamic
behavior in biological model complexes. X-ray diffraction measurements
determined the crystal structure of CdDLHis at 100 and 298 K. CdDLHis
crystallizes in the monoclinic space group <i>P</i>2<sub>1</sub>/<i>c</i> with two cadmium complexes per asymmetric
unit. In each complex, the Cd is hexacoordinated to two histidine
molecules. Both histidines are l in one complex and d in the other. Additionally, each complex contains multiple waters
of varying disorder. Single crystal EPR spectroscopic splitting (<b>g</b>) and copper hyperfine (<b>A</b><sup><b>Cu</b></sup>) tensors at room temperature (principal values: <b>g</b> = 2.249, 2.089, 2.050; <b>A</b><sup><b>Cu</b></sup> =
−453, −30.5, −0.08 MHz) were determined from
rotational experiments. Alignments of the tensor directions with the
host structure were used to position the copper unpaired d<sub><i>x</i><sup>2</sup>‑<i>y</i><sup>2</sup></sub> orbital in an approximate plane made by four proposed ligand atoms:
the <i>N</i>-imidazole and <i>N</i>-amino of one
histidine, and the <i>N</i>-amino and <i>O</i>-carboxyl of the other. Each complex has two such planes related
by noncrystallographic symmetry, which make an angle of 65° and
have a 1.56 Ã… distance between their midpoints. These findings
are consistent with three interpretations that can adequately explain
previous temperature-dependent EPR powder spectra of this system:
(1) a local structural distortion (static strain) at the copper site
has a temperature dependence significant enough to affect the EPR
pattern, (2) the copper can hop between the two sites in each complex
at high temperature, and (3) there exists a dynamic Jahn–Teller
effect involving the copper ligands
Models for Copper Dynamic Behavior in Doped Cadmium dl-Histidine Crystals: Electron Paramagnetic Resonance and Crystallographic Analysis
Electron
paramagnetic resonance and crystallographic studies of copper-doped cadmium dl-histidine, abbreviated as CdDLHis, were undertaken to gain further
understanding on the relationship between site structure and dynamic
behavior in biological model complexes. X-ray diffraction measurements
determined the crystal structure of CdDLHis at 100 and 298 K. CdDLHis
crystallizes in the monoclinic space group <i>P</i>2<sub>1</sub>/<i>c</i> with two cadmium complexes per asymmetric
unit. In each complex, the Cd is hexacoordinated to two histidine
molecules. Both histidines are l in one complex and d in the other. Additionally, each complex contains multiple waters
of varying disorder. Single crystal EPR spectroscopic splitting (<b>g</b>) and copper hyperfine (<b>A</b><sup><b>Cu</b></sup>) tensors at room temperature (principal values: <b>g</b> = 2.249, 2.089, 2.050; <b>A</b><sup><b>Cu</b></sup> =
−453, −30.5, −0.08 MHz) were determined from
rotational experiments. Alignments of the tensor directions with the
host structure were used to position the copper unpaired d<sub><i>x</i><sup>2</sup>‑<i>y</i><sup>2</sup></sub> orbital in an approximate plane made by four proposed ligand atoms:
the <i>N</i>-imidazole and <i>N</i>-amino of one
histidine, and the <i>N</i>-amino and <i>O</i>-carboxyl of the other. Each complex has two such planes related
by noncrystallographic symmetry, which make an angle of 65° and
have a 1.56 Ã… distance between their midpoints. These findings
are consistent with three interpretations that can adequately explain
previous temperature-dependent EPR powder spectra of this system:
(1) a local structural distortion (static strain) at the copper site
has a temperature dependence significant enough to affect the EPR
pattern, (2) the copper can hop between the two sites in each complex
at high temperature, and (3) there exists a dynamic Jahn–Teller
effect involving the copper ligands
Electron Paramagnetic Resonance Spectroscopic Study of Copper Hopping in Doped Bis(l‑histidinato)cadmium Dihydrate
Electron
paramagnetic resonance (EPR) spectroscopy was used to
study CuÂ(II) dynamic behavior in a doped biological model crystal,
bisÂ(l-histidinato)cadmium dihydrate, in order to gain better
insight into copper site stability in metalloproteins. Temperature-dependent
changes in the low temperature X-band EPR spectra became visible around
100 K and continued up to room temperature. The measured 298 K g-tensor
(principal values: 2.17, 2.16, 2.07) and copper hyperfine coupling
tensor (principal values: −260, −190, −37 MHz)
were similar to the average of the 77 K tensor values pertaining to
two neighboring histidine binding sites. The observed temperature
dependence was interpreted using Anderson’s theory of motional
narrowing, where the magnetic parameters for the different states
are averaged as the copper rapidly hops between sites. The EPR pattern
was also found to undergo a sharp sigmoidal-shaped, temperature-dependent
conversion between two species with a critical temperature <i>T</i><sub>c</sub> ≈ 160 K. The species below <i>T</i><sub>c</sub> hops between the two low temperature site
patterns, and the one above <i>T</i><sub>c</sub> represents
an average of the molecular spin Hamiltonian coupling tensors of the
two 77 K sites. In addition, the low and high temperature species
hop between one another, contributing to the dynamic averaging. Spectral
simulations using this 4-state model determined a hop rate between
the two low temperature sites ν<sub><i>h</i>4</sub> = 4.5 × 10<sup>8</sup> s<sup>–1</sup> and between the
low and high temperature states ν<sub><i>h</i>2</sub> = 1.7 × 10<sup>8</sup> s<sup>–1</sup> at 160 K. An Arrhenius
relationship of hop rate and temperature gave energy barriers of Δ<i>E</i><sub>4</sub> = 389 cm<sup>–1</sup> and Δ<i>E</i><sub>2</sub> = 656 cm<sup>–1</sup> between the two
low temperature sites and between the low and high temperature states,
respectively
Electron Paramagnetic Resonance Spectroscopic Study of Copper Hopping in Doped Bis(l‑histidinato)cadmium Dihydrate
Electron
paramagnetic resonance (EPR) spectroscopy was used to
study CuÂ(II) dynamic behavior in a doped biological model crystal,
bisÂ(l-histidinato)cadmium dihydrate, in order to gain better
insight into copper site stability in metalloproteins. Temperature-dependent
changes in the low temperature X-band EPR spectra became visible around
100 K and continued up to room temperature. The measured 298 K g-tensor
(principal values: 2.17, 2.16, 2.07) and copper hyperfine coupling
tensor (principal values: −260, −190, −37 MHz)
were similar to the average of the 77 K tensor values pertaining to
two neighboring histidine binding sites. The observed temperature
dependence was interpreted using Anderson’s theory of motional
narrowing, where the magnetic parameters for the different states
are averaged as the copper rapidly hops between sites. The EPR pattern
was also found to undergo a sharp sigmoidal-shaped, temperature-dependent
conversion between two species with a critical temperature <i>T</i><sub>c</sub> ≈ 160 K. The species below <i>T</i><sub>c</sub> hops between the two low temperature site
patterns, and the one above <i>T</i><sub>c</sub> represents
an average of the molecular spin Hamiltonian coupling tensors of the
two 77 K sites. In addition, the low and high temperature species
hop between one another, contributing to the dynamic averaging. Spectral
simulations using this 4-state model determined a hop rate between
the two low temperature sites ν<sub><i>h</i>4</sub> = 4.5 × 10<sup>8</sup> s<sup>–1</sup> and between the
low and high temperature states ν<sub><i>h</i>2</sub> = 1.7 × 10<sup>8</sup> s<sup>–1</sup> at 160 K. An Arrhenius
relationship of hop rate and temperature gave energy barriers of Δ<i>E</i><sub>4</sub> = 389 cm<sup>–1</sup> and Δ<i>E</i><sub>2</sub> = 656 cm<sup>–1</sup> between the two
low temperature sites and between the low and high temperature states,
respectively