248
W.-C. Lin et al. / Polyhedron 42 (2012) 243–248
The coordination bond lengths Cu–O(1) 1.900(2) Å, Cu–N(1)
3.5. 1H NMR spectroscopic data for 8 in CDCl3
2.004(3) Å, Cu–N(2) 1.909(3) Å and Cu–N(3) 1.994(3) in 7 are with-
in the limit found for Cu(II) porphyrins.
The C(17) in 7 is no longer bonded to copper as indicated by its
longer internuclear distance, 2.530(3) Å for Cuꢃ ꢃ ꢃC(17). This
Cuꢃ ꢃ ꢃC(17) bond distance is largely compared to that observed in
copper(II) square planar complexes [2.007(4) Å] [10].
In solution, the 1H NMR spectrum exhibits six pyrrole reso-
nances [Hb(12), Hb(13), Hb(2), Hb(3), Hb(7), Hb(8)] for 8 (Fig. 4).
The doublet at 8.05 ppm is assigned as Hb(12) with 3J(H–
H) = 4.8 Hz and the other doublet at 7.92 ppm is due to Hb(13) with
3J(H–H) = 5.4 Hz (Fig. 4b). The doublet at 8.28 ppm is assigned as
Hb(3) with 3J(H–H) = 5.4 Hz and the other doublet at 7.99 ppm is
due to Hb(2) with 3J(H–H) = 4.8 Hz. The doublet at 8.19 ppm is as-
signed as Hb(7) with 3J(H–H) = 4.8 Hz and the other doublet at
8.18 ppm is due to Hb(8) with 3J(H–H) = 5.4 Hz. The external benzyl
ligand (Bz) unit in 8 gave rise to series of 1H resonances at 6.74 [t,
1H, p-H(49), 3J(H–H) = 7.2 Hz], 6.60 [t, 2H, m-H(48, 50), 3J(H–
H) = 7.8 Hz], 5.69 [d, 2H, o-H(47, 51), 3J(H–H) = 7.8 Hz], 5.33 [d,
1H, H(45A), 3J(H–H) = 16.2 Hz] and 5.13 [d, 1H, H(45B), 3J(H–
H) = 16.2 Hz] (Fig. 4a). The diamagnetic property of 8 was inferred
from its diamagnetic 1H NMR spectra in CDCl3 (Fig. 4).
The Rhꢃ ꢃ ꢃC(17) distance of 2.170(3) Å in 8 is slightly longer than
that observed in [Rh]–CHCl [2.050(7)–2.161(2)] complexes con-
taining the Rh–CH2Cl moiety [11]. The short distance 2.170(3) Å
for Rh–C(17) clearly signifies as
g
2 interaction between the Rh cen-
ter and the inner carbonyl group. Such a coordination mode was
previously reported by Dolphin and co-workers for Ni(CTTPPO)
(pyridine) (3) [6], by Hung for Co(CTPPO)(NO) (4) [7] and by Rach-
lewicz for Fe(CTPPO)Br (6). This Rh–C(17) contact may be de-
scribed as a weak covalent bond [8]. The geometry around Rh3+
in 8 is described as a distorted octahedron. The bond distance (Å)
for 8 are Rh–Cl = 2.3743(9) and Rh–C(17) = 2.170(3) and the mean
Rh–N(p) = 2.047(3) (Table 2).
4. Conclusion
We adopt the plane of the three strongly bound pyrrole nitro-
gen atoms [i.e., N(1), N(2) and N(3)] as a reference plane 3N for
7–8. The oxygen atom O(1) (or O) in 7 (or 8) is located considerably
far from the 3N plane. In 7, Cu and O(1) are located on the same
sides at 0.21 and 1.27 Å from its 3N plane. In 8, Rh3+ and O are lo-
cated on the different sides at 0.14 and ꢀ1.59 Å from its 3N plane.
The C(17) pyrrole rings bearing the CH2CH2CH2OC6H5 group (or
CH2C6H5) in 7 (or 8) deviate mostly from the 3N plane, thus orient-
ing separately in a dihedral angle of 35.7° (or 25.4°) for 7 (or 8),
whereas a small angle of 9.4°, 3.3° and 3.9° occur with N(1), N(2)
and N(3) pyrrole for 7 and the corresponding angles are 11.7°,
8.9° and 11.5° with N(1), N(2) and N(3) pyrrole for 8. Overall, the
carbon atom [C(17)] which is bonded to oxygen is not bonded to
the copper ion in 7 whereas the rhodium ion, in complex 8, is
bonded to both the oxygen atom and C(17). Complex 8 is diamag-
netic and structurally similar to an C-oxide with paramagnetism in
Ni(CTPPO)(py) (3) [6], Co(CTPPO)(NO) (4) [7], and Fe(HCTPPO)Br
(6) [8].
We have investigated two new inverted N-confused porphyrin
inner C-oxide metal complexes, namely paramagnetic 7 and dia-
magnetic complex 8, and their X-ray structures were established.
Complex 8 has been prepared and characterized by 1H NMR and
O
UV–Vis spectroscopy to have a structure incorporating an
Rh
C
unit. A copper(II) complex 7 has been isolated and characterized
by electron spin resonance spectroscopy.
Acknowledgements
The financial support from the National Science Council of the
ROC under Grants NSC 100-2113-M-005-002 is gratefully
acknowledged. We thank Dr. S. Elango for helpful discussions.
Appendix A. Supplementary data
CCDC 870784, 870785 and 870786 contain the supplementary
crystallographic data for 1, 7 and 8. These data can be obtained free
from the Cambridge Crystallographic Data Centre, 12 Union Road,
Cambridge CB2 1EZ, UK; fax: (+44) 1223-336-033; or e-mail:
3.3. ESR studies
Complex 7 is paramagnetic because of the d9 configuration of
Cu(II). The unpaired electron resides in the dx2 ꢀ y2 orbital, which
leads to characteristic ESR spectra of 7 in CH2Cl2 at 293 K: four peaks
due to the nuclear spin (I = 3/2) of the Cu and a seven-line pattern
due to the hyperfine interactions with the three nitrogens (I = 1)
of the porphyrin. The ESR spectra are typical for the planar cop-
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14N) = 13.0 G for 7 in CH2Cl2 at 293 K (Fig. 2a) and with
so
g = 2.125 and A (63Cu) = 173 for 7 in CH2Cl2 at 77 K (Fig. 2b). These
k
k
hyperfine couplings are similar in magnitude to those of giso = 2.060,
Aiso
(
63Cu) = 79.7 G and Aiso 14N) = 13.0 G obtained from Cu(tpp–N–
(
O) (monomer) in CHCl3 (or CH2Cl2) solution at 293 K [12].
3.4. UV–Vis absorption spectra for compound 8
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The visible spectrum of 8 is shown in Fig. 3 that has a ligand field
of close to Oh symmetry. The spectrum shows an intense near-UV
Soret band, consisting of 320 nm (
e
= 81.0 ꢁ 103 Mꢀ1 cmꢀ1) and a
shoulder at 348 nm (
e
= 69.2 ꢁ 103 Mꢀ1 cmꢀ1), together with two
weaker visible bands at 484 nm (
e
= 39.9 ꢁ 103 Mꢀ1 cmꢀ1) and
584 nm
(e
= 22.0 ꢁ 103 Mꢀ1 cmꢀ1
) assignable to Q bands. As
expected from the Tanabe-Sugano diagram of d6, the electronic
spectrum consists of two bands owing to the transitions
1A1g ? 1T1g (584 nm) and 1Ag ? 1T2g (484 nm) (Fig. 3) [13,14].