2c could allow them to be resolved, providing potentially new
sets of ligands for asymmetric homogeneous catalysis.14
We thank the National Science Foundation (Grant CHE-
0909613) for financial support.
Notes and references
z Crystal data for 2a: C46H40N2, M = 620.80, monoclinic, space
˚
group C2/c, colorless, a = 17.936(1), b = 10.398(1), c = 20.003(1) A,
3
b = 116.370(1)1, V = 3342.4(4) A , Z = 4, Dc = 1.234 g cmꢁ3
,
=
˚
m(Mo-Ka) = 0.71 cmꢁ1, T = 293 K, 3820 unique data with Rint
0.0439. Final R1 = 0.0554, wR2 = 0.1495 for 3052 reflections with
I 4 2s(I), GOF = 1.046. CCDC 750096. Crystal data for 2c:
C66H52N6ꢂ2CH2Cl2, M = 1098.99, monoclinic, space group C2/c,
˚
yellow,
a
=
27.005(2),
b
=
14.736(1),
c
=
17.778(2) A,
b = 128.084(2)1, V = 5568.6(8) A , Z = 4, Dc = 1.311 g cmꢁ3
,
=
3
˚
Fig.
3
UV–vis absorption spectra of 13 (—), 14 (ꢂ ꢂ ꢂ) and
m(Mo-Ka) = 2.62 cmꢁ1, T = 293 K, 6323 unique data with Rint
[Ru(40-EtOtpy)2](PF6)2 (---) in CH3CN at room temperature.
0.0494. Disordered CH2Cl2 molecules treated with SQUEEZE routine
in PLATON. Final R1 = 0.0665, wR2 = 0.1843 for 3872 reflections
with I 4 2s(I), GOF = 0.959. CCDC 750095.
(J = 21.0 Hz) and 4.83 (J = 21.0 Hz). For 13 without the
presence of paramagnetic ruthenium ions, the AB quartet
signals appear at d 4.46 (J = 21.6 Hz) and 4.30 (J = 21.6 Hz).
The 1H NMR signals of the ethoxyl groups and the hydrogens
on the diindeno-fused phenanthryl system are sharp with well-
defined splitting patterns. Similarly, for 14 the AB quartet
signals appear at d 4.46 (J = 21.6 Hz) and 4.30 (J = 21.6 Hz).
Again, due to slow rate of rotation around the carbon–carbon
single bonds attaching the terpyridyl units to the phenanthryl
system, the signals of the aromatic hydrogens on the terpyridyl
groups of 13 and 14 are broad.
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The UV–vis spectra of 13 and 14 show ligand-centered
bands of the aromatic terpyridyl structures in the near-UV
region (Fig. 3).11,13 The less intense bands in the visible region
can be attributed to the spin-allowed metal-to-ligand charge-
transfer (MLCT) transitions involving promotion of an elec-
tron from the metal t2g orbital to a p* antibonding orbital of
the ligand with absorption maxima at ca. 495 to 505 nm.
Compared to the parent [Ru(tpy)2](PF6)2 complex, which
exhibits an absorption maximum at 474 nm,11 these MLCT
bands undergo a red shift. Such a red shift is reminiscent of
what was observed in the cases of [Ru(40-EtOtpy)2](PF6)2
complex (l = 485 nm) bearing electron donating ethoxyl
groups, [Ru(40-Cltpy)2](PF6)2 complex (l = 480 nm) bearing
chloro substituents, and [Ru(40-Phtpy)2](PF6)2 complex
(l = 487 nm) bearing phenyl groups.11 Luminescence was
not observed for 13 and 14 at room temperature.
In conclusion, three 4,5-diheteroarylphenanthrenes 2a, 2b
and 2c possessing severe helical twists were synthesized from
the corresponding benzannulated enyne–allenes. The struc-
tures of 2a and 2c were established by X-ray crystal structure
analyses, permitting direct measurements of the extent of the
structural distortion. The presence of two terpyridyl units in 2c
allowed it to be used as a ligand for the synthesis of helical
dinuclear Ru(II) bis(terpyridine) complexes. The two Ru(II)
units are in close proximity to each other, making it possible
for electronic interactions between the two heteroaromatic p
systems for energy- and electron-transfer processes.3 The high
configurational stability of the helical structures of 2a, 2b and
13 A. Winter, J. Hummel and N. Risch, J. Org. Chem., 2006, 71,
4862–4871.
14 G. Chelucci and R. P. Thummel, Chem. Rev., 2002, 102,
3129–3170.
ꢀc
This journal is The Royal Society of Chemistry 2010
1940 | Chem. Commun., 2010, 46, 1938–1940