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J. P. Harney et al. / Tetrahedron Letters 53 (2012) 4700–4703
CO2Me
H
CO2Me
O
H
Fe
10 R =
11 R =
NH
NH
HN
HN
(i - ii)
Fe
Fe
N
N
R
Zn
R
or
N
N
7 - 8 %
CO2Me
2
2 or 6
O
MeO2C
CO2Me
5
Scheme 2. Reagents and conditions: (i) CH3CN, BF3ÁOEt2, NH4Cl, 0 °C, p-chloranil (ii) Zn(OAc)2, CH2Cl2, MeOH (iii) THF, aq. NaOH.
(a)
(b)
ZnTCPP
blank TiO2
TiO2 / ZnTCPP
TiO2 / trans-Fc-ZnP-CO2H
TiO2 / trans-Fc2-ZnP-(CO2H)2
1.0
0.8
0.6
0.4
0.2
0.0
trans-Fc-ZnP-CO2H
trans-Fc2-ZnP-CO2H
1.0
0.8
0.6
0.4
0.2
0.0
1.0
0.8
0.6
0.4
0.2
0.0
500
600
700
800
400
500
600
700
800
400
500
600
700
800
Wavelength (nm)
Wavelength (nm)
Figure 2. UV–Vis spectra (a) in methanol (b) on TiO2. Analogous spectra were observed for Fc-ZnP-CO2H and Fc-ZnP-(CO2H)3, for clarity only the former is included.
vent in the presence of ammonium chloride as the water scaven-
ger. A relatively low yield (7%) is observed under these conditions
consistent with literature reports.8 However this is a small trade-
off for the benefit of isolating the single targeted porphyrin product
10. Zinc insertion was carried out in a similar manner to trans-Fc-
ZnP-CO2Me. Porphyrin Fc-ZnP-(CO2Me)3 was prepared under
analogous minimal scrambling conditions yielding free base fol-
lowed by zinc insertion yielding the methyl ester 11 in good yield.
Hydrolysis gave the target compound in relatively good yield
phyrin systems relative to ZnTCPP. The photoelectrochemical
properties of these systems are currently under investigation.
Acknowledgments
J. Rochford thanks the University of Massachusetts Boston for
financial support.
References and notes
11
(Scheme 2).
1. Liska, P.; Vlachopoulos, N.; Nazeeruddin, M. K.; Comte, P.; Gratzel, M. J. Am.
Chem. Soc. 1988, 110, 3686–3687.
2. Vlachopoulos, N.; Liska, P.; Augustynski, J.; Gratzel, M. J. Am. Chem. Soc. 1988,
110, 1216–1220.
The UV–Vis absorption spectra of trans-Fc-ZnP-CO2Me, Fc-ZnP-
(CO2Me)3, and trans-Fc2-ZnP-(CO2Me)2 in methanol are shown in
Figure 2(a) overlayed with the reference compound ZnTCPP. Sub-
stantial electronic coupling of the redox active ferrocene and the
porphyrin is evident. For example, the Soret absorption is signifi-
cantly broadened due to vibronic coupling of the porphyrin S2 state
and the ferrocene substituent resulting in large increases of the
peak full width half maxima (FWHM) from 11 nm for ZnTCPP up
to 32 nm for trans-Fc2-ZnP-(CO2Me)2. In addition, intensity bor-
rowing of both the ferrocenyl MLCT and the porphyrin Q band
transitions is evident. The three complexes trans-Fc-ZnP-CO2Me,
Fc-ZnP-(CO2Me)3, and trans-Fc2-ZnP-(CO2Me)2 were easily hydro-
lyzed under basic conditions and covalently attached to mesopor-
ous TiO2 nanoparticle films.12 UV–Vis absorption spectra of cover
glass/TiO2/porphyrin films are shown in Figure 2(b). Results indi-
cate an increased absorption cross section of the ferrocenyl por-
3. O’Regan, B.; Gratzel, M. Nature 1991, 353, 737–740.
4. Yella, A.; Lee, H.-W.; Tsao, H. N.; Yi, C.; Chandiran, A. K.; Nazeeruddin, M. K.;
Diau, E. W.-G.; Yeh, C.-Y.; Zakeeruddin, S. M.; Grätzel, M. Science 2011, 334,
629–634.
5. Boyle, N. M.; Rochford, J.; Pryce, M. T. Coord. Chem. Rev. 2010, 254, 77–102.
6. Rochford, J.; Rooney, A. D.; Pryce, M. T. Inorg. Chem. 2007, 46, 7247–7249.
7. Lee, C. H.; Lindsey, J. S. Tetrahedron 1994, 50, 11427–11440.
8. Littler, B. J.; Miller, M. A.; Hung, C. H.; Wagner, R. W.; O’Shea, D. F.; Boyle, P. D.;
Lindsey, J. S. J. Org. Chem. 1999, 64, 1391–1396.
9. Zaidi, S. H. H.; Loewe, R. S.; Clark, B. A.; Jacob, M. J.; Lindsey, J. S. Org. Proc. Res.
Dev. 2006, 10, 304–314.
10. Venkatraman, S.; Kumar, R.; Sankar, J.; Chandrashekar, T. K.; Sendhil, K.;
Vijayan, C.; Kelling, A.; Senge, M. O. Chem.-Eur. J. 2004, 10, 1423–1432.
11. 1H NMR spectroscopic data for selected compounds: (4) (CDCl3) d: 2.43 (6H, s,
Me), 4.11–4.26 (9H, m, Cp), 5.32 (1H, s, methine), 6.07 (2H, s, b), 6.73 (2H, s, b),
7.29 (4H, d, J = 8.10 Hz, ph), 7.78 (4H, d, J = 8.10 Hz, ph), 10.26 (2H, s, NH) ppm.
trans-Fc-ZnP-CO2Me (8) (CDCl3) d: 2.72 (6H, s, Me), 4.07 (3H, s, CO2Me), 4.24