Supplementary Figure 1. Ellipsoid plot of [Cu2(m-xpt)2(NO3)2](PF6)2 (1). Cu···Cu =
6.843(2) Å.
Supplementary Figure 2. Ellipsoid plot of [Cu2(m-xpt)2Cl2](PF6)2 (2). Cu1···Cu2 =
7.615(2) Å.
Supplementary Figure 3. Electrochemical Studies. Cyclic voltammograms of [Cu2(m-
xpt)2(NO3)2](PF6)2 (1, black); and [Cu2(m-xpt)2Cl2](PF6)2, (2, blue) in DMF containing 0.1
M Bu4NPF6 recorded on a static glassy carbon disc working electrode with a Pt wire
auxiliary electrode and Ag/AgCl reference electrode at 25 °C at a scan rate of 50 mV s–
1.
Supplementary Figure 4. Reduction of Cu(II) dimer to Cu(I), showing the
disappearance of Cu(II). A portion of the electronic spectrum of a 3.76 mM solution of
[Cu2(m-xpt)2(NO3)2(PF6)2, 1, in DMF (blue), with increasing amounts of added sodium
ascorbate: 0.25 eq (black) to 1.25 eq (red).
Supplementary Figure 5. Reduction of Cu(II) dimer to Cu(I), showing the
appearance of Cu(I). A portion of the electronic spectrum of a 0.20 mM solution of
[Cu2(m-xpt)2(NO3)2(PF6)2, 1, in DMF (blue), with increasing amounts of added sodium
ascorbate: 0.25 eq (black) to 1.25 eq (red). λmax = 384 nm.
Supplementary Figure 6. Reaction of Cu(I) dimer with CO2. A portion of the
electronic spectrum of a 0.12 mM solution of [Cu2(m-xpt)2](PF6)2, 3, in DMF showing the
disappearance of Cu(I) by its reaction with CO2. Compare Figure 3, which shows the
appearance of Cu(II) during the same reaction.
(a) (b) Supplementary Figure 7. IR spectra: (a) [Cu2(m-xpt)2(μ-C2O4)](PF6)2 (blue) and
[Cu2(m-xpt)2(μ-13C2O4)](PF6)2 (red), and (b) difference spectrum (13C labeled minus
unlabeled) showing ν13CO = 1651 cm−1.
Supplementary Figure 8. Crystals of compound 4. Crystals of the oxalate-bridged
compound [Cu2(m-xpt)2(μ-C2O4)](PF6)2, 4, synthesized starting from: (a) [Cu2(m-
xpt)2(NO3)2](PF6)2, 1 (crystal size ca. 0.3 mm); and (b) [Cu2(m-xpt)2Cl2](PF6)2, 2. (The
blue-green crystals in sample (b) were found to be of the starting complex, 2.)
Supplementary Table 1. Electrochemical parameters. The potential of the ferrocene
(Fc/Fc+) reference redox couple under these conditions was 0.56 V vs. Ag/AgCl. The
peak separation ΔEp for the Fc/Fc+ couple ranged from 60-65 mV (10, 25 mV s−1) to 75
mV (100 mV s−1) under the same conditions. Thus, the CuII/CuI waves for 1 and 2 (see
also Supplementary Fig. 3) are quasireversible, approaching reversible behavior at low
scan rates; and the redox process is more readily reversible for 2 than for 1.
Complex Scan Rate (mV s−1)
Epa Epc ΔEp E1/2 (vs. Ag/AgCl)
E1/2 (vs. Fc/Fc+)
1 10 0.33 0.24 0.09 0.29 −0.27
1 25 0.34 0.23 0.11 0.29 −0.27
1 50 0.38 0.20 0.18 0.29 −0.27
1 100 0.40 0.18 0.22 0.29 −0.27
2 10 0.32 0.24 0.08 0.28 −0.28
2 25 0.33 0.24 0.09 0.28 −0.28
2 50 0.33 0.23 0.10 0.28 −0.28
2 100 0.35 0.22 0.13 0.29 −0.27
Supplementary Table 2. Crystal Data and Structure Refinement Parameters.
Compound 1 2
deposition no. CCDC 1000457 CCDC 1000458
formula [Cu2(m-xpt)2(NO3)2](PF6)2 ·3.5CH3CN
[Cu2(m-xpt)2Cl2](PF6)2
·4.44C3H7NO
M 1329.93 1601.17
crystal system Monoclinic Orthorhombic
space group P21/c Pna21
a/Å 11.4090(16) 13.810(2)
b/Å 12.8455(18) 19.380(3)
c/Å 23.411(3) 24.711(3)
/deg 108.575(5) 90
V/Å3 3252.3(8) 6613.6(16)
Z 2 4
T/K 100.0(5) 90.0(5)
Dcalc/g cm−3 1.358 1.608
crystal dimensions/mm
0.35 x 0.17 x 0.10 0.04 x 0.14 x 0.31
Radiation CuK MoK
θ limits/deg 3.98 – 59.20 1.65 – 25.71
reflns, measd /unique/obsd
22792/4639/3982 52940/12074/7203
F(000) 1340 3278
μ/mm−1 2.066 0.871
Rint 0.0468 0.0525
R[I>2σ(I)] 0.1013 0.0830
Rw (all data) 0.3540 0.2604
GOF 1.624 1.053
Supplementary Table 2 (continued).
Compound 4 4a 5
deposition no. CCDC 984468 CCDC 984469 CCDC 984470
formula [C46H36Cu2N16O4](PF6)2 ·2C3H7NO
[C46H36Cu2N16O4](PF6)2
·4CH3CN [C44H40Cu2N16O2](NO3)4
·2C3H7NO·3.34H2O
M 1440.12 1458.14 1406.50
crystal system
Orthorhombic Orthorhombic Monoclinic
space group Cmca Cmca P21/n
a/Å 24.1471(17) 24.461(7) 11.4361(13)
b/Å 11.7107(7) 11.959(3) 22.691(3)
c/Å 20.5949(12) 20.008(5) 11.9848(13)
/deg 90 90 106.847(5)
V/Å3 5823.8(6) 5853(3) 2976.6(6)
Z 4 4 2
T/K 100.0(5) 100.0(5) 100.0(5)
Dcalc/g cm−3 1.642 1.655 1.569
crystal dimen-sions/mm
0.45x0.17x0.04 0.30x0.22x0.13 0.12x0.19x0.21
radiation MoK MoK CuK
θ limits/deg 1.69-30.05 2.04-30.23 4.32-69.67
reflns, measd /unique/obsd
44218/4357/3592 31270/4418/3607 52513/14803/12358
F(000) 2928 2960 1455
μ/mm−1 0.891 0.886 1.691
Rint 0.0310 0.0447 0.0741
R[I>2σ(I)] 0.0527 0.0346 0.0637
Rw (all data) 0.1531 0.0900 0.1928
GOF 1.033 1.031 1.024
Supplementary Methods
X-ray Crystallography. Intensity data were collected at low temperature on a Bruker
Kappa Apex-II DUO CCD diffractometer fitted with an Oxford Cryostream chiller. MoK
( = 0.71073 Å) radiation with a TRIUMPH curved graphite monochromator was used
for 2, 4, and 4a, and CuK ( = 1.54184 Å) radiation from an I S microfocus source
with QUAZAR multilayer optics was used for 1 and 5. Data reduction included
absorption corrections by the multiscan method, with SADABS,1 or TWINABS1 for 5.
The structures were determined by direct methods and difference Fourier techniques
and refined by full-matrix least squares, using SHELXL-97.2 All non-hydrogen atoms
were refined anisotropically except for the minor component in a disordered nitrate in 1
and 5, C atoms in 2, and the minor component of the disordered PF6− anion in 1 (vide
infra). For 2, low data quality did not allow anisotropic refinement of the C atoms.
Disordered solvents were removed using the SQUEEZE3 procedure for 2, resulting in
non-integral solvent stoichiometry (see the CIF file for details). Normal refinement
procedures for 2 led to several unreasonable distances within the m-xpt ligands.
Therefore, for the final refinement, the two sets of ligand atoms were restrained to yield
similar bond distances and angles. For 4 and 4a, the PF6− anion is disordered into two
orientations, and a single solvent molecule (DMF for the crystals prepared by reaction of
Cu(I) (3) with CO2; CH3CN for those prepared by reaction of Cu(II) (1 or 2) with oxalate)
is disordered across a mirror plane. The crystal of 5 was a nonmerohedral twin by 180º
rotation about real axis [−1 0 1]. Refinement was vs. HKLF5 data, and twin components
were present approximately 52/48%. This structure has a disorder involving a nitrate ion
in two positions and a partially occupied water molecule associated with one of them.
All H atoms were placed in idealized positions, except for water hydrogen atoms. Water
H atoms were refined with restrained O-H distances, but the H atoms of the water
molecule in the nitrate/water disorder of 5 could not be located. Crystal data and
structure refinement parameters are presented in Supplementary Table 2.
Supplementary References:
1 SADABS (University of Göttingen, Germany). 2 Sheldrick, G. M. A short history of SHELX. Acta Crystallogr A 64, 112-122
(2008). 3 Spek, A. L. Structure validation in chemical crystallography. Acta Crystallogr.,
Sect. D 65, 148-155 (2009).