Chemistry Letters Vol.33, No.11 (2004)
1419
.
BF3 OEt2 and TFA catalysis for 3 h under dark and nitrogen at-
one. We believe that the porphyrin free face, not hydroquinone
face, should attach to the graphite surface. The entropic contri-
bution to the adsorption free energy is calculated to be ca.
1.7 kJ molꢄ1 (¼ RT ln 2, T ¼ 293 K) from the difference in sym-
metry number.13 In the case of pyridine-coordinated rhodium
chloride with the same alkyl chain length (C18), we had no mo-
lecular image.9 Therefore, the covalently linked approach using
the strapped porphyrin 10 is more attractive than the axial-coor-
dination approach from the viewpoint of the formation of stable
alkyl-chain-assisted SAMs.
This protocol will lead to the functionalization of alkyl-
chain-assisted SAMs by introducing the functional molecule in
the strapped moiety. The molecular design of the strapped moie-
ty is considered to be free since the structure of the opposite side
(porphyrin free face) is always the same. 2-D array of the func-
tional porphyrin conjugates is expected to exhibit the novel at-
tractive characteristics. The detailed STM characterization of
the strapped porphyrin 10, characterization of SAMs as a func-
tional device, and further functionalization of the strapped por-
phyrin are now in progress.
mosphere. After the addition of DDQ, the solution was refluxed
for 1 h under dark. After cooling to room temperature, the solu-
tion was directly adsorbed to dry silica gel and eluted the crude
product by CHCl3. The recovered product was purified by silica
gel chromatography twice [First: CHCl3/hexane = 7/3 (v/v),
Second: hexane/AcOEt = 10/1 (v/v)]. The product 10 was
confirmed by H, 13C NMR, MS, and elemental analysis.10
1
SAMs of the strapped porphyrin 10 were confirmed by
STM. STM observations were conducted in a droplet of the sam-
ple solution (solvent: dichlorobenzene) on a fleshly cleaved
graphite surface. Figure 2a is a representative STM image of
SAMs of the strapped porphyrin 10. We were able to confirm
the characteristic two-fold symmetry structure.5 The bright spots
aligned in lines and the dark stripes correspond to the strapped
porphyrin moiety and the closely packed alkyl chains on the
graphite surface, respectively. The lattice parameters of the unit
cell a ꢂ b and ꢀ (Figure 2c) were 3:94 ꢃ 0:1 ꢂ 2:01 ꢃ 0:1 nm
and 101 ꢃ 5ꢁ. As for the proposed structure of SAMs shown
in Figure 2c, the lattice parameters were 3:96 ꢂ 2:02 nm and
104.8ꢁ (a ꢂ b and ꢀ). These values are well consistent with
the observed ones.
This study was supported by the Industrial Technology
Research Grant Program of the New Energy and Industrial
Technology Development Organization (NEDO) of Japan.
References and Notes
1
2
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a) H. Imahori and Y. Sakata, Eur. J. Org. Chem., 1999, 2445. b) D.
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Figure 2. (a) STM image of self-assembled monolayers con-
sisting of strapped porphyrin 10 on a graphite surface (10 ꢂ
10 nm2). Solvent: dichlorobenzene. Tunneling conditions: I ¼
200 pA, V ¼ ꢄ1000 mV. (b) Partial molecular structure of the
strapped porphyrin 10 (MM2 calculation). (c) Proposed structure
of SAMs consisting of the strapped porphyrin 10. Each molecu-
lar structure was optimized using MM2 calculation.
8
9
10 1H NMR (400 MHz, CDCl3): ꢁ ꢄ2:63 (s, NH), 0.88 (t, CH3), 1.20–1.55
(m, CH2), 1.62 (m, CH2), 1.97 (m, CH2), 2.77 (br, CbH2), 3.62 (s,
CaH), 3.81 (br, CcH2), 4.24 (m, OCH2), 6.79 (s, CdH), 7.03 (d,
J ¼ 8:4 Hz, CeH), 7.20, 7.25 (br, CgH), 7.87, 8.22 (br, ChH), 8.37
(d, J ¼ 8:4 Hz, CfH), 8.83 (m, CiH); 13C NMR (100 MHz, CDCl3): ꢁ
14.6, 23.2, 26.7, 29.9, 30.0, 30.1, 30.2, 32.4, 68.8, 69.0, 69.1, 69.6,
101.6, 105.6, 113.1, 115.4, 115.8, 119.6, 125.3, 131 (br), 134.9,
135.8, 136.2, 151.0 (br), 152.8, 159.3, 160.8, 161.2; MS (MALDI):
m=z: 1881.8 ½Mꢅþ; C126H184N4O8 (1882.8): calcd C 80.38, H 9.85,
N 2.98; found C 80.74, H 9.80, N 2.71%.
11 This value is consistent with that for the crystal structure of the capped
porphyrin. See: M. R. Johnson, W. K. Seok, and J. A. Ibers, J. Am.
Chem. Soc., 113, 3398 (1991).
12 ‘‘Scanning Probe Microscopy and Spectroscopy: Method and
Application,’’ ed. by R. Wiesendanger, Camblidge University Press,
New York (1994).
From the section analysis of STM image, the average appa-
rent height of the strapped porphyrin 10 was 0:57 ꢃ 0:05 nm,
which is clearly more than that of C18OPP (0:20 ꢃ 0:03 nm).
In the molecular structure calculated by MM2 (Figure 2b), the
average distance between the porphyrin (pyrrole and meso car-
bons) and strapped benzene planes was 0.38 nm.11 However,
we must consider the fluttering of the strapped moiety and the
interaction between the strapped benzene and porphyrin. In prin-
ciple, the apparent STM height is not comparable to the real
height of the molecule.12
In compared to C18OPP, the molecular adsorption of the
strapped porphyrin 10 is entropically unfavorable owing to less
molecular symmetry. Namely, C18OPP has two equivalent faces
to adsorb to the surface while the strapped porphyrin 10 has only
13 W. F. Bailey and A. S. Monahan, J. Chem. Educ., 55, 489 (1978).
Published on the web (Advance View) October 2, 2004; DOI 10.1246/cl.2004.1418