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nitrosyl oxygen atoms to adopt the proper orientation to coordi-
nate to the copper centers. As a result, the dihedral angle for P1–
C7–C8–N1 is reported to be 74.45(3)° and 154.78(2)° for P1–
C13–C14–N2. Additionally, the angle between the planes of the
pyridyl groups is 66.55(7)°. The Jahn–Teller effect is evidenced in
the N3–Cu–O3#1 axis as both the N–Cu and O–Cu bond lengths
are about 0.3 Å longer than the lengths of the corresponding N4–
Cu–O1 axis.
3.2.5. Structure of compound 6
Given the labile nature of the CH3OH molecule coordinated to
the copper center in compound 5, the crystal structure 6 was ob-
tained by addition of one equiv. of 4,40-bipyridine to a reaction
mixture containing Cu(BF4)2, L3, and 2,20-bipyridine. A thermal
ellipsoid plot of the discrete molecule of 6 is presented in Fig. 7,
and selected bond lengths and angles are given in Table 4. The
reaction product, formed by controlled and stepwise addition of
the reactants, consists of a discrete molecule composed of two cop-
per centers in an octahedral environment interconnected by a 4,40-
bipyridine molecule. The Cu–N and Cu–O bond distances fall in the
range of reported values, although they cover an important range
of values. For example, the Cu1–N3 interaction at 1.8600(2) Å is
considerably shorter than Cu1–N4 at 2.0020(3) Å, which confirms
the sterics that exists around the metal center. This geometric con-
straint is induced by the pyridyl arm that binds to Cu1 through O3,
and helps explain the deviation from planarity of the rings of the
2,20-bipyridine with an angle of 14.44(1)°, being this more pro-
nounced than the one observed in compound 5. The Jahn–Teller
distortion is found by looking at the Cu1–N5 bond at 2.2560(3) Å
and the Cu1–O3 at 2.8569(4) Å, both of these are considerably
longer than any of the other Cu–N or Cu–O bonds. Another conse-
quence of the steric constrains present in the molecule is the devi-
ation from linearity of the O3–Cu1–N5 angle with a value of
161.75(10)° to describe a rather distorted octahedral geometry.
The center of 4,40-bipyridine lies on a crystallographic inversion
center.
3.2.3. Structure of compound 4
The reaction of a second equivalent of L3 with a 1:1 ligand to
metal ratio mixture forces the core structure observed in 3 to rup-
ture into a molecular structure formed by two independent and
unique copper centers, but still interconnected by the phosphine
oxide ligands. In the crystal structure of 4, shown in Fig. 5 each
copper is bound to an L3 molecule, two oxygen atoms (P@O and
N–O) from a second phosphine oxide ligand, and a nitrosyl group
belonging to a bridging third equiv. of L3. Hence, both copper cen-
ters display a distorted octahedral geometry, where the axial Cu–O
bonds exhibit rather long distances compared to the equatorial
interactions, which can be attributed to the commonly known
Jahn–Teller distortions. This distortion is more pronounced in
Cu1, where the Cu1–O4 distance is 2.2767(17) Å, and the Cu1–O3
bond is considerably longer at 2.5067(2) Å. The rest of Cu1–O dis-
tances fall into the range of reported values with an average of
1.97 Å. For Cu2, the axial bond distances are 2.2647(18) and
2.3281(18) Å for Cu2–O11 and Cu2–O8, respectively. The equato-
rial Cu2–O interactions range between 1.9517(16) and
2.0328(18) Å. All angles around Cu1 and Cu2 are only slightly devi-
ated from the ideal values of an octahedral geometry.
3.2.6. Structure of compound 7
The crystal structure of compound 7 consists of a polymeric ar-
ray obtained by addition of 1 equiv. of L3 into a reaction mixture
containing Cu(BF4)2ꢁxH2O and 4,40-bipyridine in a 1:1 ratio. Chang-
ing the order of reaction of the reactants by adding the bipyridine
to a solution containing the copper salt and the phosphine oxide
ligand, only results in the formation of compound 3, which is indic-
ative that the bridging effect of 4,40-bipyridine is not as favored as
the chelating effect of 2,20-bipyridine to disrupt the dimeric copper
structure described for 3. The crystal structure of 7 contains two
crystallographically independent molecules (Fig. 8b) differentiated
only by the interaction of a BF4 anion and a water molecule with
Cu1 and Cu2, respectively. The extended polymeric structure of
the monomer containing Cu2 is shown in Fig. 8a and reveals an
infinite chain in a zigzag conformation as indicated by the N4–
Cu1–N3 angle of 90.88(12)°. The octahedral environment observed
in 7 is formed by one molecule of L3 capping a face of the molecule,
two 4,40-bipyridines in a cis position, and a H2O molecule trans to
the P@O–Cu interaction. The rings of the bipyridine ligand are
highly twisted with an angle of 34.38(2)°. The Jahn–Teller distor-
tion for this molecule involves the BF4ꢀ ion and phosphoryl oxygen
for Cu1 and the solvent H2O and phosphoryl oxygen for Cu2. For
Cu1 the anion to Cu distance is 2.727 and to O1 is 2.218 Å. For
Cu2 these interactions are Cu2–O8 2.5639(4) and Cu2–O4
2.287(3) Å. The angle for O4–Cu2–O8 is rather deviated from the
ideal 180° with a value of 167.92(1)°, while the equatorial plane
display a range of angles between 83.84(11)° and 95.84(11)°.
3.2.4. Structure of compound 5
Formation of compound 4 as a result of the reaction of an
additional equivalent of L3 with a 1:1 ligand to metal ratio mix-
ture provides evidence that more complex coordinative structures
could result from the addition of different electron donating li-
gands. As a first example of this series of mixed-ligand complexes
Fig. 6, shows the crystal structure of 5 obtained by reaction of the
bidentate 2,20-bipyridine with a solution containing Cu(BF4)2 and
L3 in a 1:1:1 ratio of the reactants. As expected, the bipyridine
binds the copper cation in a chelating fashion to form a discrete
molecule. The disruption of the dimeric copper motif observed
in 3 is likely due to steric effects rather than electronic factors,
as it might be expected that the 2,20-bipyridine would substitute
the CH3CN molecules in 3 but conserve the structural conforma-
tion. The copper center in 5 is in a distorted octahedral environ-
ment, where a MeOH molecule is occupying an axial position
along with the interaction between Cu1 and O3 to display an an-
gle of 169.67(6)° (Table 4). The Jahn–Teller effect is displayed
along this axis by the very long Cu–O3 distance of 2.5550(14) Å
and the Cu–O4 distance of 2.3308(16) Å. It is interesting to note
that the methanol oxygen is considerably closer to the copper
center than the nitrosyl oxygen, this may be due to some steric
crowding around the Cu center. The equatorial angles range be-
tween 81.38(7)° and 96.60(6)°, the smallest value corresponding
to the acute binding of the 2,20-bipyridine. The biggest deviation
among the reported angles for 5 with respect to the ideal values
for an octahedral geometry is exemplified by O1–Cu1–O3 with a
value of 79.44(5)°, which is evidence of the constraining effect of
the ligand coordinated to the metal center. The angles around P1
suggests a slightly distorted tetrahedral geometry, being close to
the ideal 109.5°, ranging between 104.25(10)° and 115.83(9)°. The
aromatic rings of 2,20-bipyridine are slightly twisted from planar-
ity at an angle of 9.09(1)°, a well-known characteristic of bipyri-
dine ligands.
3.3. Electrochemical properties
The electrochemical properties of compounds 1–7 were investi-
gated by cyclic voltammetry. All of the experiments were per-
formed at room temperature in CH3CN solutions. Before each
measurement, the solutions were degassed and the working elec-
trode polished with alumina powder (1.0, 0.3, and 0.05 lm). The
voltammograms were recorded under nitrogen atmosphere
containing approximately 0.1 M [Bu4N][PF6] as the supporting
electrolyte, all relative to the formal potential of the