CuIIGHK and CuIIDAHK Complexes
FULL PAPER
A stock solution of coumarin-3-carboxylic acid (5 mm) was prepared in
phosphate (20 mm), NaCl (100 mm) buffer at pH 9 at room temperature.
The stock solution was stored at ꢀ208C.
chemical shifts are relative to tetramethylsilane. 1D NMR and 2D NMR
spectra were collected at 298 K in pure D2O.
Cyclic voltammetry (CV): CV measurements were recorded under argon
using a 620C electrochemical analyzer (CH Instruments, Inc). The work-
ing electrode was a glassy carbon disk and a Pt wire was used as counter-
electrode. The reference electrode was an AgCl/Ag electrode (0.223 V
versus NHE) isolated in a fritted bridge. Immediately before the mea-
surement of each voltammogram, the working electrode was carefully
polished with alumina suspensions (1, 0.3 and 0.05 mm, successively), so-
nicated in an ethanol bath and then washed carefully with ethanol. The
electrochemical cell medium used was milli-Q water with 0.1m sodium
phosphate (pH 7.4) added as supporting electrolyte.
Measurements of HO· production: These were performed in phosphate
(20 mm), NaCl (100 mm) buffer at pH 7.4. The reaction was started by
the addition of ascorbate (500 mm). In all these experiments, DFO (at a
final concentration of 1 or 2 mm depending on buffer concentration) was
15N-labelled glycine, 13C-(COOꢀ)-labelled glycine and 15N(Im)-labelled
histidine were purchased from Eurisotop (Saclay, France).
X-ray diffraction: Crystals suitable for X-ray diffraction were obtained
by slow ethanol diffusion and evaporation of a 0.2m solution in milli-Q
water of the corresponding complex. Data were collected using a Kappa
X8 APPEX II Bruker diffractometer with graphite-monochromated
MoKa radiation (l=0.71073 ꢄ). The temperature of the crystal was main-
tained at the selected value (100 K) by using a 700 series Cryostream
cooling device within an accuracy of ꢁ1 K. Intensity data were corrected
for Lorentz polarisation and absorption factors. The structures were
solved by direct methods using SHELXS-97[29] and refined against F2 by
full-matrix least-squares techniques using SHELXL-97[30] with anisotropic
displacement parameters for all non-hydrogen atoms.
C
added to avoid non-specific OH production by metallic ion impurities
Treatment of H: H atoms of the ligand were added from the difference
from the buffer.
Fourier map and refined by the riding model. For the [CuII
ACTHNUTRGNEU(GN DAHK)]
C [22b]
Coumarin-3-carboxylic acid (3-CCA) (Sigma) was used to detect HO .
complex only, the H atoms of the water molecules were subsequently in-
C
HO reacts with 3-CCA to form 7-hydroxycoumarin-3-carboxylic acid (7-
ꢀ
cluded in the refinement in geometrically idealized positions, with C H=
OH-CCA), which is fluorescent at 452 nm upon excitation at 395 nm.
The intensity of the fluorescence signal is proportional to the number of
ꢀ
0.96(3) ꢄ and H H=1.52(3) ꢄ, and refined using the riding model with
isotropic displacement parameters of Uiso(H)=1.4Ueq (parent atom). For
C
7-OH-CCA molecules formed, which in turn is proportional to the HO
[CuII
ACHTUNGTRENNUNG(GHK)], the lateral chain of lysine is disordered over two sites with
radicals generated. [CCA]=500 mm.
occupancies of 0.5:0.5. Occupancy parameters for the 16 water oxygen
atoms were refined. The net occupancy of the ordered water is 9.25. All
calculations were performed by using the Crystal Structure crystallo-
graphic software package WINGX.[31] The absolute configuration was de-
termined by refining the Flack parameter[32] using a large number of Frie-
del pairs.
Ascorbate consumption was monitored by UV/Vis spectroscopy. The in-
tensity of the Asc absorption band at l=265 nm (e=14500mꢀ1 cmꢀ1) was
monitored as a function of time, in 100 mm phosphate buffer (pH 7.4)
that contained 100 mm of Asc, 2 mm of DFO, 5 mm of CuII and after addi-
tion of 6 mm of GHK or DAHK peptide.
CCDC-809108 ([CuII(GHK)]) and 809109 ([CuII
ACHTUNGTRENNUNG ACHTUNGTERN(NUGN DAHK)]) contain the
supplementary crystallographic data for this paper. These data can be ob-
tained free of charge from The Cambridge Crystallographic Data Centre
Acknowledgements
ESI-MS measurements: ESI mass spectra were recorded using an API
This work was supported by a grant from the Agence Nationale de la Re-
cherche, Programme Blanc NT09-488591, “NEUROMETALS” (P.F.,
C.H. and P.D.) and 05-JCJC-0010-01, “NEUROARPE” (P.D.). We thank
the staff of the SAMBA beamline at SOLEIL and more particularly Dr.
Emiliano Fonda for help in performing the XAS experiments (SOLEIL
Project 20080324). Dr. Yannick Coppel and Valꢁrie Bourdon are ac-
knowledged for their help in NMR spectroscopic experiments and analy-
sis and in ESI-MS experiments, respectively. We thank Fanny Leroux for
365 MS mass spectrometer at a flow rate of 5 mLminꢀ1
.
XAS measurements: Cu K-edge XAS spectra were recorded using the
SAMBA bending magnet beamline at Synchrotron SOLEIL (Saint-
Aubin, France). The main optical elements consisted of a double crystal
SiACHTUNGTRENNUNG(111) dynamical focusing monochromator between two palladium-
coated mirrors, one collimating the beam in the vertical direction and
one focusing it on the sample. X-ray harmonic rejection was obtained by
setting the energy cutoff to change the incidence of the mirrors. The
measurements were performed on solution samples at room temperature
in the fluorescence mode using a single-element Silicon Drift Detector
(SDD). The energy was calibrated by the simultaneous measurement of a
Cu foil spectrum in transmission (first inflection point set at 8980.3 eV).
earlier results obtained on [CuII
ACTHNUTRGNEU(GN GHK)], Bertrand Badei for the ascor-
bate consumption experiments and Bruno Alies for his participation in
the NMR spectroscopic experiments.
Possible X-ray photo-reduction of the [CuII
ACTHNUTRGNE(NUG peptide)] samples was moni-
[1] a) H. Kozlowski, A. Janicka-Klos, J. Brasun, E. Gaggelli, D. Valen-
Conato, R. Gavioli, R. Guerrini, H. Kozlowski, P. Mlynarz, C. Pasti,
J. Biol. Inorg. Chem. 2007, 12, 913–918.
[3] L. Pickart, M. M. Thaler, Nature 1973, 243, 85–87.
[4] A. Simꢁon, F. Monier, H. Emonard, Y. Wegrowski, G. Bellon, J. C.
Monboisse, P. Gillery, W. Hornebeck, F.-X. Maquart, Curr. Top.
Pathol. 1999, 93, 95–101.
[5] L. Pickart, J. Biomater. Sci. Polym. Ed. 2008, 19, 969–988.
tored by checking, on consecutive scans, the appearance of the XANES
feature at 8984 eV, which is typical of CuI formation. After 5 scans, which
lasted around 10 min each, the feature was still small, thus indicating a
poor reduction effect. Two series of around 10 to 20 scans were recorded.
For the EXAFS analysis, the photo-reduction of scans that can be ne-
glected was averaged. For the XANES study, only the two first scans of
each series were added. Points were measured every 0.25 eV in the
XANES region and steps were gradually increased from 0.5 eV (at E=
9000 eV) to 5 eV (at E=9600 eV) in the EXAFS region.
EPR spectroscopy: EPR spectra (9.4 GHz) were recorded using
a
Bruker ELEXSYS 500 spectrometer equipped with a continuous-flow He
cryostat (Oxford). The field modulation frequency was 100 kHz. Pulsed
EPR experiments were recorded using a Bruker ELEXSYS 580 spec-
trometer at liquid helium temperatures. Pulsed EPR data were processed
by using routines locally written with Matlab (R2008b, The Mathworks,
Inc.).
NMR spectroscopy: 1D 1H and 13C experiments and 2D experiments
were recorded using a Bruker Avance 500 spectrometer equipped with a
5 mm triple-resonance inverse Z-gradient probe (TBI 1H, 31P, BB). All
[9] C. M. Perkins, N. J. Rose, B. Weinstein, R. E. Stenkamp, L. H.
Chem. Eur. J. 2011, 17, 10151 – 10160
ꢃ 2011 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
10159