An Electron-Deficient Porphyrin Tape
meso–meso-Linked Diporphyrin (8)
1.652 gcmÀ3; T=93(2) K; R1 =0.0753 [I>2s(I)]; Rw =0.2214 (all data);
GOF=1.012; crystals were grown from PhCl/MeOH.
To a solution of tetrapyrroethane (5, 500 mg, 1.72 mmol) and dicarbinol
6[14b] (2.65 g, 3.79 mmol, 2.2 equiv) in dry CH2Cl2 (100 mL) was added p-
toluenesulfonic acid monohydrate (372 mg, 1.89 mmol, 1.1 equiv), and
the resulting solution was stirred under a N2 atmosphere at ambient tem-
perature for 1 h. After the addition of DDQ (2.35 g, 10.3 mmol,
6.0 equiv), the solution was stirred for a further 1 h and then passed
through a short alumina column to remove any tar. The reaction mixture
was purified by GPC and column chromatography on silica gel to afford
porphyrin 7 (225 mg, 278 mmol, 8.1% yield) and diporphyrin 8 (104 mg,
64 mmol, 3.7% yield). The spectroscopic data of compound 7 were the
same as those reported previously.[18]
Crystallographyic Data
CCDC 871954 (3) and CCDC 871954 (8) contain the supplementary crys-
tallographic data for this paper. These data can be obtained free of
charge from The Cambridge Crystallographic Data Centre via
Two-photon-Absorption Experiments
The TPA spectrum was measured in the NIR region by using the open-
aperture Z-scan method with 130 fs pulses from an optical parametric
amplifier (Light Conversion, TOPAS) operating at a repetition rate of
3 kHz that was generated from a Ti:sapphire regenerative amplifier
system (Spectra-Physics, Hurricane). After passing through a 10 cm focal
length lens, the laser beam was focused and passed through a 1 mm
quartz cell. Because the position of the sample cell could be controlled
along the laser beam direction (z axis) by using the motorcontrolled
delay stage, the local power density within the sample cell could be
simply controlled under constant laser intensity. The transmitted laser
beam from the sample cell was then detected by using the same photo-
diode as that used for reference monitoring. The on-axis peak intensity
of the incident pulses at the focal point (I0) was in the range of 40–
60 GWcmÀ2. For a Gaussian beam profile, the nonlinear absorption coef-
ficient can be obtained by curve fitting of the observed open-aperture
traces T(z) to Equation (1), where a0 is the linear absorption coefficient,
l is the sample length, and z0 is the diffraction length of the incident
beam.
1
8: H NMR (600 MHz, CDCl3, 298 K): d=9.00 (m, 8H; b-H), 8.61 (d, J=
4.6 Hz, 4H; b-H), 8.15 (d, J=4.6 Hz, 4H; b-H), À2.31 ppm (brs, 4H;
inner NH); 19F NMR (565 MHz, CDCl3, 298 K): d=À126.44 (m, 12F; o-
F), À151.15 (t, J=22.0 Hz, 2F; p-F), À151.27 (t, J=22.0 Hz, 4F; p-F),
À161.19 (dt, 1J=6.1 Hz, 2J=23.0 Hz, 4F; m-F), À161.39 ppm (dt, 1J=
6.1 Hz, 2J=23.0 Hz, 8F; m-F); UV/Vis (CHCl3): lmax (e)=410 (209000),
447 (215000), 518 (61000), 591 (18000), 647 (3500), 664 nm
(4000 molÀ1 dm3 cmÀ1); HRMS (ESI-TOF, positive-ion mode): m/z calcd
for C76H21N8F30: 1615.1405; found: 1615.1384 [M+H]+.
Crystal data: C76H20F30N8·2.5C2H4Cl2; Mw =1862.38; triclinic; space
group: P-1 (No. 2); a=18.5492(3), b=21.5458(4), c=22.1560(4) ꢁ; a=
68.6717(9), b=89.6696(9), g=64.5465(8)8; V=7327.5(2) ꢁ3; Z=4;
1calcd =1.688 gcmÀ3; T=93(2) K; R1 =0.1051 [I>2s(I)]; Rw =0.3173 (all
data); GOF=1.069. Crystals were grown from 1,2-dichloroethane/
MeOH.
meso–meso-Linked ZnII–Diporphyrin (9)
To a solution of compound 8 (83.5 mg, 51.7 mmol) in MeOH (100 mL)
was added ZnACHTUNGTRENNUNG(OAc)2·2H2O (190 mg, 1.1 mmol, 20 equiv) and the result-
ing solution was stirred under a N2 atmosphere at ambient temperature.
After 12 h, the reaction mixture was washed with water, dried over
Na2SO4, and the solvent was removed under reduced pressure to afford
the product as a red solid (86.2 mg, 49.5 mmol, 96% yield). 1H NMR
(600 MHz, CDCl3, 298 K): d=9.08 (m, 8H; b-H), 8.67 (d, J=4.6 Hz, 4H;
b-H), 8.18 ppm (d, J=4.6 Hz, 4H; b-H); 19F NMR (565 MHz, CDCl3,
298 K): d=À136.70 (m, 12F; o-F), À151.86 (t, J=22.0 Hz, 2F; p-F),
À151.98 (t, J=22.0 Hz, 4F; p-F), À161.74 (dt, 1J=5.9 Hz, 2J=23.5 Hz,
4F; m-F), and À161.78 ppm (dt, 1J=5.9 Hz, 2J=23.5 Hz, 8F; m-F); UV/
Vis (CHCl3): lmax (e)=320 (37000), 418 (203000), 456 (210000), 563
After the nonlinear absorption coefficient has been obtained, the TPA
cross-section s(2) of one solute molecule (in GM, where 1 GM=
10À50 cm4 sphotonÀ1 moleculeÀ1) can be determined by using Equation (2),
where NA is the Avogadro constant, d is the concentration of the com-
pound in solution, h is the Planck constant, and n is the frequency of the
incident laser beam.
(51000), 602 nm (14000 molÀ1 dm3 cmÀ1); fluorescence (CHCl3, lex
=
418 nm): lmax =597, 652 nm; HRMS (ESI-TOF, negative-ion mode): m/z
calcd for C76H16N8F30Zn2Cl: 1776.9244; found: 1776.9220 [M+Cl]À.
Transient Absorption Experiments
meso–meso,b-b,b-b Triply Linked ZnII–Diporphyrin (3)
The femtosecond time-resolved transient absorption (TA) spectrometer
used for this study consisted of a femtosecond optical parametric amplifi-
er (Quantronix, Palitra-FS) pumped by a Ti:sapphire regenerative ampli-
fier system (Quantronix, Integra-C) operating at 1 kHz repetition rate
and an accompanying optical-detection system. The generated OPA
pulses had a pulse width of about 100 fs and an average power of 1 mW
in the range of 450–800 nm, which were used as pump pulses. White light
continuum (WLC) probe pulses were generated with a sapphire window
(2 mm thick) by focusing a small portion of the fundamental 800 nm
pulses, which were picked off by a quartz plate before entering into the
OPA. The time delay between the pump and probe beam was carefully
controlled by making the pump beam travel along a variable optical
delay (Newport, ILS250). The intensities of the spectroscopically dis-
persed WLC probe pulses were monitored by a miniature spectrograph
(OceanOptics, USB2000+). To obtain the time-resolved transient absorp-
tion difference signal (DA) at a specific time, the pump pulses were chop-
ped at 25 Hz and absorption-spectra intensities were saved alternately
with or without pump pulses. Typically, 6000 pulses were used to excite
the samples and to obtain the TA spectra at a particular delay time. The
polarization angle between the pump and the probe beam was set at the
magic angle (54.78) by using a Glan-laser polarizer with a half-wave re-
tarder to prevent polarization-dependent signals. The cross-correlation
To a solution of compound 9 (55.0 mg, 31.6 mmol) in dry toluene (80 mL)
was added ScACHTUNGTRENNUNG(OTf)3 (77.9 mg, 158 mmol, 5.0 equiv) and DDQ (35.9 mg,
158 mmol, 5.0 equiv) and the resulting solution was stirred under a N2 at-
mosphere at 1108C for 6 h. After cooling to RT, THF was added to the
reaction mixture and the resulting solution was passed through an alumi-
na column with THF as an eluent. The solution was evaporated and re-
crystallization from CH2Cl2/MeOH gave the product as violet crystals
(36.4 mg, 20.9 mmol, 66% yield). 1H NMR (600 MHz, CDCl3, 298 K): d=
7.71 (d, J=4.6 Hz, 4H; b-H), 7.67 (d, J=4.6 Hz, 4H; b-H), 7.09 ppm (s,
1
4H; bay-area); 19F NMR (565 MHz, CDCl3, 298 K): d=À137.17 (dd, J=
7.3 Hz, 2J=25.7 Hz, 8F; o-F), À137.43 (dd, 1J=7.3 Hz, 2J=25.7 Hz, 4F;
o-F), À151.88 (m, 6F; p-F), À161.14 ppm (m, 12F; m-F); UV/Vis
(CH2Cl2): lmax(e)=414 (137000), 523 (54600), 559 (128000), 601 (91400),
661 (35000), 945 (13300), 1077 nm (13600 molÀ1 dm3 cmÀ1); fluorescence
(CHCl3, lex =414 nm): lmax =1101, 1272 nm; HRMS (ESI-TOF, negative-
ion mode): m/z calcd for C76H12N8F30Zn2Cl: 1772.8931; found: 1772.8920
[M+Cl]À.
Crystal data: C76H18F30N8Zn2·5MeOH·2PhCl; Mw =2088.93; monoclinic;
space group: P21/c (No. 14); a=21.6317(7), b=6.9196(2), c=
28.9465(6) ꢁ; b=104.2737(14)8; V=4199.0(2) ꢁ3; Z=2; 1calcd
=
Chem. Asian J. 2012, 00, 0 – 0
ꢀ 2012 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
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