Synthesis and Photophysical Properties of Neutral Luminescent
Rhenium-Based Molecular Rectangles
T. Rajendran,† Bala. Manimaran,† Rong-Tang Liao,†Ren-Jay Lin,‡P. Thanasekaran,† Gene-Hsiang Lee,§ Shie-Ming Peng,§Yen-Hsiang Liu,† I-Jy Chang,*,‡S. Rajagopal,*,†,|and Kuang-Lieh Lu*,†
Institute of Chemistry, Academia Sinica, Taipei 115, Taiwan, Department of Chemistry, National Taiwan Normal UniVersity, Taipei 117, Taiwan, Department of Chemistry, National Taiwan UniVersity, Taipei 107, Taiwan, and School of Chemistry, Madurai Kamaraj UniVersity, Madurai, 625 021, India
Received January 29, 2003
A series of neutral luminescent molecular rectangles [{Re(CO)3(µ-bpy)Br}{Re(CO)3(µ-L)Br}]2 (1−4) having fac-Re(CO)3Br as corners and 4,4′-bipyridine (bpy) as the bridging ligand on one side and other bipyridyl ligands of varying length (L) on the other side have been synthesized and characterized. The crystal structure of 1 shows a rectangular cavity with the dimensions of 11.44×7.21 Å. When the cavity size is tuned from 1 to 4, a dimension of 11.4×20.8 Å could be achieved, as revealed by the molecular modeling. These rectangles exhibit luminescence in solution at room temperature. In particular, compound 4 containing 1,4-bis(4′-pyridylethynyl)benzene (bpeb) as bridging ligand shows the excited-state lifetime of 495 ns. Fine-tuning of the cavity size of the rectangles improves their excited-state properties. These properties facilitate the study of excited-state electron-transfer reactions with electron acceptors and donors and host−guest binding. Crystallographic information: 1‚6CH3COCH3is monoclinic, P21/c, with a ) 12.0890(2), b ) 24.2982(2), and c ) 12.8721(2) Å, β ) 107.923(1)°, and Z ) 2.
Introduction
The ground- and excited-state properties of the organo-metallic complex fac-[ClRe(CO)3LL], where LL is a diimine, and its derivatives have been extensively studied in the past 2 decades due to their potential for use in solar energy conversion and as sensors.1-12These complexes are ideally
suited for such applications since they display intense luminescence in the visible region and are stable to photo-decomposition. In this decade much attention has been paid to transition-metal-directed self-assembly to construct many
* To whom correspondence should be addressed. E-mail: lu@ chem.sinica.edu.tw (K.-L.L.). Fax: int. code + (2)27831237.
†Academia Sinica.
‡National Taiwan Normal University. §National Taiwan University. |Madurai Kamaraj University.
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different supramolecular architectures such as molecular squares, boxes, helices, and many interesting three-dimen-sional structures.7-20 The rigid macrocycles based on cis-bridging ligation of transition metals have tremendous promise in host-guest, inclusion, and molecular recognition chemistry.9-15Recent interest is the synthesis and charac-terization of luminescent molecular squares containing a variety of bipyridyl groups between Re(I) centers.9-12,16-18 Though the synthesis of several dozens of squares has been successfully demonstrated from many groups of workers, the reports on the Re(I)-containing rectangles are relatively scarce.19,20 A rectangular cavity is reasonably expected to offer enhanced binding and selectivity particularly for planar aromatic guests.19c
We have initiated a systematic study on the synthesis of light-emitting neutral molecular rectangles, and the prelimi-nary results have been reported.20a To improve the cavity size and luminescent properties of molecular rectangles, we have introduced acetylene, butadiyne, and 1,4-bis(ethynyl)-benzene groups between two pyridine moieties in the ligand on one side while keeping 4,4′-bipyridine on the other side for the synthesis of Re(I)-containing rectangles. In this report the details on the synthesis, characterization, photophysical properties, and host-guest interactions of the rectangles containing pyrazine (pz), 4,4′-dipyridylacetylene (dpa), 4,4′ -dipyridylbutadiyne (dpb), and 1,4-bis(4′ -pyridylethynyl)-benzene (bpeb) bridges are presented.
Results and Discussion
Synthesis and Characterization. The molecular
rect-angles [{Re(CO)3(µ-bpy)Br}{Re(CO)3(µ-L)Br}]2(1, L ) pz;
2, L ) dpa; 3, L ) dpb; 4, L ) bpeb) were synthesized as
shown in Scheme 1. Treatment of Re(CO)5Br with 1 equiv of Me3NO in the presence of CH3CN at 0°C gave Re(CO)4 -(NCMe)Br, which on reaction with 4,4′-bipyridine (bpy) afforded {Re(CO)4Br}2(µ-bpy). Further treatment of the bimetallic edge{Re(CO)4Br}2(µ-bpy) with 2 equiv of Me3 -NO at 5°C followed by addition of pyrazine or acetylene-containing bipyridyl ligands afforded the molecular rect-angles 1-4.
The molecular rectangles 1-4 were characterized by a variety of analytical techniques such as IR, NMR, FAB-mass, and elemental analysis. The1H NMR spectrum of 1 showed two sets of signals in a 3:1 ratio for both the pyrazine and the pyridyl groups of the bpy ligand, indicating that 1 exists as two isomeric forms in solution at ambient temperature. Compared to the free ligands these signals were shifted toward low field due to the formation of new coordination bonds between the nitrogen-containing ligands and the Re metal centers.21The FAB mass spectrum of 1 showed the molecular ion peak at m/z 1880 whose experimental isotope pattern matches very closely with that calculated.
By use of the single-crystal X-ray diffraction method, we obtained solid evidence to support the structure of complex
1. An ORTEP diagram of 1 is shown in Figure 1, and its
pertinent crystallographic data are given in Tables 1 and 2. The core geometry can be viewed as a molecular rectangle in which two Br(CO)4Re-bpy-Re(CO)4Br edges are bridged by two pyrazine moieties with the cavity dimension of 11.44
× 7.21 Å. Br(1) and Br(2) are disordered with CO group in
73/27 occupancy, which is corroborated by the isomeric1H NMR spectral pattern of 1. An infinite number of open-end channels are observed from the packing diagram because of the effectiveπ stacking of the aromatic rings of the molecules (Figure 2).
The result of the molecular modeling study of 1-4 reveals that a cavity dimension of 11.4× 20.8 Å could be achieved by the proper selection of the acetylene-containing bipyridyl ligands (Table 3). The large cavity dimension promises (13) (a) Caulder, D. L.; Raymond, K. N. Acc. Chem. Res. 1999, 32, 975.
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(20) (a) Rajendran, T.; Manimaran, B.; Lee, F. Y.; Lee, G. H.; Peng, S. M.; Wang, C. M.; Lu, K. L. Inorg. Chem. 2000, 39, 2016. (b) Manimaran, B.; Rajendran, T.; Lu, Y. L.: Lee, G. H.; Peng, S. M.; Lu, K. L. J. Chem. Soc., Dalton Trans. 2001, 515.
(21) Kuehl, C. J.; Huang, S. D.; Stang, P. J. J. Am. Chem. Soc. 2001, 123, 9634.
Scheme 1
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interesting host-guest interactions. Since 1-4 contain large cavities, the solvent molecules such as acetone are present inside them and could not be removed completely under vacuum at room temperature for several hours.
Ground-State Properties. Table 4 summarizes the
ab-sorption spectral data of rectangles 1-4 in comparison with squares [Re(CO)3(µ-pz)Cl]4 (5), [Re(CO)3(µ-bpy)Cl]4 (6),
and [Re(CO)3(µ-dpb)Cl]4(7), corners Re(CO)3(bpy)2Cl (8) and Re(CO)3(dpb)2Cl (9), and the ligands (Chart 1). Figure 3 compares the absorption spectra of rectangle 4 and the free ligands bpy and bpeb. The electronic absorption spectra of rectangles 1-4 exhibit two main features: the high-energy band in the near-UV region (∼260 nm) is assigned to the ligand centeredπ-π* transition, and the low-energy band, to the metal-to-ligand charge transfer (MLCT) transition.1,4,22 In the rectangle 3, the lowest energy band is solely of MLCT character similar to square 7. It is noted that the MLCT bands (22) Meyer, T. J. Pure Appl. Chem. 1986, 58, 1193.
Figure 1. ORTEP diagram of 1.
Table 1. Crystal and Structure Refinement Data for
[{Re(CO)3(µ-bpy)Br}{Re(CO)3(µ-pz)Br}]2‚6CH3COCH3, 1‚6CH3COCH3
formula C58H60Br4N8O18Re4
fw 2221.58
cryst syst monoclinic
space group P21/c a, Å 12.0890 (2) b, Å 24.2982 (2) c, Å 12.8721 (2) β, deg 107.923 (1) V, Å3 3597.57 (9) Z 2 cryst dimens, mm 0.35× 0.18 × 0.12 Fcalcd, Mg/m3 2.051 µ(Mo KR), mm-1 8.998
range of transm factors 0.2767-0.4921 data/restraints/params 7285/0/451
R1 (I > 2σ(I)) 0.0356
wR2 (all data) 0.0724
Table 2. Selected Bond Distances (Å) and Bond Angles (deg) for 1 (a) Bond Distances (Å)
Re(1)-Br(1) 2.5694(14) Re(1)-C(1) 1.929(7) Re(1)-C(2) 1.922(6) Re(1)-C(3) 1.92(2) Re(1)-N(1) 2.212(5) Re(1)-N(3) 2.221(5) Re(2)-Br(2) 2.5873(13) Re(2)-C(4) 1.919(6) Re(2)-C(5) 1.924(7) Re(2)-C(6) 1.917(14) Re(2)-N(2) 2.212(4) Re(2)-N(4) 2.218(5) C(1)-O(1) 1.146(7) C(2)-O(2) 1.153(7) C(3)-O(3) 1.16(3) C(4)-O(4) 1.153(7) C(5)-O(5) 1.149(7) C(6)-O(6) 1.17(2)
(b) Bond Angles (deg)
N(1)-Re(1)-N(3) 84.5(2) C(1)-Re(1)-N(1) 178.0(2) C(3)-Re(1)-N(1) 90.5(10) C(2)-Re(1)-N(1) 94.1(2) C(3)-Re(1)-N(3) 92.6(10) C(2)-Re(1)-N(3) 178.6(2) C(1)-Re(1)-N(3) 93.6(2) C(1)-Re(1)-Br(1) 93.2(2) C(3)-Re(1)-Br(1) 177.3(10) C(2)-Re(1)-Br(1) 90.9(2) N(1)-Re(1)-Br(1) 87.21(12) N(3)-Re(1)-Βr(1) 88.67(12) C(6)-Re(2)-N(2) 90.5(5) C(5)-Re(2)-N(2) 175.3(2) C(6)-Re(2)-N(4) 91.5(5) C(4)-Re(2)-N(4) 177.6(2) C(5)-Re(2)-N(4) 93.5(2) C(6)-Re(2)-Br(2) 178.4(5) C(4)-Re(2)-Br(2) 91.8(2) C(5)-Re(2)-Br(2) 89.8(2) N(2)-Re(2)-Br(2) 87.91(11) N(4)-Re(2)-Br(2) 88.65(12)
Figure 2. Packing diagram of 1.
Table 3. Molecular Modeling Data for Interatomic Distances (Re‚‚‚Re) in 1-4
rectangle Re-bpy-Re (Å) Re-L-Re (Å) Lb
1 11.4 (11.440)a 7.19 (7.214)a pz
2 11.4 14.0 dpa
3 11.4 16.6 dpb
4 11.4 20.8 bpeb
aFrom X-ray structure analysis.bbpy ) 4,4′-bipyridine; pz ) pyrazine; dpa ) 4,4′-dipyridylacetylene; dpb ) 4,4′-dipyridylbutadiyne; bpeb ) 1,4-bis(4′-pyridylethynyl)benzene.
Table 4. Absorption and Emission Spectral and Excited-State Lifetime Data for Re(I) Compounds and Ligands in CH2Cl2at 298 K
compd absλmax, nm emissionλmax, nm lifetimeτ, ns
1 252, 336 606 86 2 259, 352 611 86 3 259, 323, 357 616 72 4 260, 351 616 495 5c 274, 396 682 54 6c 248, 348 632 134 7d 322, 360a 635a 39a 8c 248, 314 585 1670 9e 251, 262, 288, 302, 322, 345 612 100 bpy 240, 265 b dpa 263, 276, 293 b dpb 245, 256, 285, 304, 325 b bpeb 319, 339 b pz 261, 270, 313 b
aMeasurements taken in THF.bNo detectable emission.cReference 9c. dReference 16d.eReference 23.
Rajendran et al.
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of rhenium complexes are insensitive to the variation of the halide.24The absorption data for 1-4 show that the substitu-tion of pz by dpa, dpb, and bpeb leads to a red shift, but the introduction of bpeb in place of dpb does not lead to substantial change in the absorption spectrum of the rect-angle. On the other hand, if we compare the rectangle 3 with square 7, both of them have a peak near 320 nm but an additional peak is obtained at 357 nm for 3 and at 360 nm for 7. If we compare 3 and 6, two MLCT peaks are observed for 3 at 323 and 357 nm but one peak for 6 at 348 nm, whereas the corners 8 and 9 have absorption maxima at 316 and 342 nm, respectively. Thus, we can assign the peak at 323 nm to Re(I) f bpy and 357 nm to Re(I) f dpb. In a comparison of 3 and 4, theλmaxvalue of 4 at 351 nm may be assigned to the MLCT transition Re(I) f bpeb.
Excited-State Properties. Maxima of emission spectra
(λmaxem) and excited-state lifetime (τ) of rectangles, squares, and corners are collected in Table 4. The broad luminescence spectra of rectangles 2-4 (Figure 4) indicate that the luminescence originates from the lowest3MLCT state. The assignment of the lowest emitting level as MLCT in character is based on the position and shape of the emission band and the emission lifetime which are consistent with those
previously reported for similar complexes assigned as MLCT emitters.5-10,16,19,20Similar to the observation in the absorption spectra, the emission maxima of rectangles 1-4 are slightly shifted to lower energy while the conjugation of the ligand is extended. The emission spectra of rectangles 2-4 have also been recorded at 77 K, and the emission maxima (λmaxem ) 542, 526, and 536 nm for 2-4, respectively) are shifted
to blue compared to the values at 298 K as observed with other metal complexes.25 These λmaxem values at 77 K correspond to the energy of the 0-0 transition and of3MLCT state and have been used in the estimation of excited-state redox potentials in combination with ground-state redox potentials (vide infra).
Though the emission lifetime of rectangles 1-3 is similar, it is very high for 4. As far as Ru(II) and Re(I) complexes are concerned, the lifetime of 3MLCT is controlled by its energy.26If the3MLCT state is close to the3MC state, the deactivation may take place via3MC which is nonemissive (Figure 5). If the3MLCT state is close to the ground state, according to the energy gap law, nonradiative decay is facile. Emission spectra recorded at 77 K show that the 3MLCT level of rectangle 4 falls between 2 and 3. Thus, the probable explanation for the long lifetime of 4 compared to 2 and 3 with the available emission spectral data is that the3MLCT state of 4 is suitably positioned in such a way that it is away from 3MC as well as from the ground state. A possible
(23) Sun, S. S.; Anspach, J. A.; Lees, A. J.; Zavalij, P. Y. Organometallics
2002, 21, 685.
(24) Giordano, P. J.; Wrighton, M. S. J. Am. Chem. Soc. 1979, 101, 2888.
(25) (a) Nieuwenhuis, H. A.; Stufkens, D. J.; Vlcek, A., Jr. Inorg. Chem.
1995, 34, 3879. (b) Grosshenny, V.; Harriman, A.; Romero, F. M.;
Ziessel, R. J. Phys. Chem. 1996, 100, 17472.
(26) Anderson, P. A.; Keene, F. R.; Meyer, T. J.; Moss, J. A.; Strouse, G. F.; Treadway, J. A. J. Chem. Soc., Dalton Trans. 2002, 3820. Figure 3. Absorption spectra of (a) 4,4′-bipyridine (bpy), (b) 1,4-bis(4′
-pyridylethynyl)benzene (bpeb), and (c) [{Re(CO)3(µ-bpy)Br}{Re(CO)3
(µ-bpeb)Br}]2(4) in CH2Cl2.
Chart 1
Figure 4. Luminescence spectra of molecular rectangles 2-4 in CH2Cl2
at 298 K.
Figure 5. Energy level diagram of Re(I) rectangles.
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alternative explanation for the long lifetime of 4 compared to 1-3 is the involvement of the extendedπ system of the bpeb ligand.
To gain insight into the excited-state lifetime of rectangles
1-4 an energy-gap plot has been constructed. The rates of
decay of emissive excited states of Re(I) complexes, i.e., lifetime (τ), are typically controlled by nonradiative decay process. Figure 6 shows a plot of ln(1/τ) vs Eem for the rectangles 1-4, squares 5 and 6, and corners 8 and 9 in CH2 -Cl2. An analysis of the nonradiative decay rates for all complexes showed that the nonradiative decay rate constant is increased when the excited-state energy decreased. A linear relationship of ln(1/τ) vs Eemwith a correlation of 0.940 has been observed for rectangle 4 along with squares and corners. This effect can be understood in terms of the energy-gap law.27,28Deviation from a linear relation between ln(1/τ) vs Eem occurs for complexes 1-3 in which the vibrational modes of deactivation is sensitive to nonradiative decay. Whereas 4 minimizes the rate of nonradiative decay and hence it has a long excited-state lifetime. Thus by modulation of the nature of the ligand, design of a neutral molecular rectangle with sufficiently long triplet lifetime and large cavity can be achieved.
Electrochemical Properties. The measured cyclic
volta-mmetric data for the rectangles 1-4, squares 5-7, and corners 8 and 9 are collected in Table 5. The rectangles 2-4 in CH2Cl2 show two reduction waves and three oxidation waves. The first reduction wave at around -1.0 V can be assigned to the reduction of the non-bpy ligand, and the second reduction, to the bpy ligand. The ligand-centered reduction potential of the rectangles is much lower than those observed for free ligands.29The complexation of the ligand to the metal usually stabilizes theπ* level in the ligand and lowers the energy of theπ* orbital.
The first oxidation of the rectangles 2-4 around 0.4 V may be assigned to the oxidation of bromide ion.30 The
quasireversible oxidation waves observed in the range 1.35-1.70 V may be attributed to the oxidation of the metal centers present in the rectangle. This redox behavior of these rectangles can be exploited in their utilization as electron donors in the efficient electron-transfer reactions with electron acceptors, quinones, and nitroaromatics and as electron acceptors with aromatic amines.31
Luminescence Quenching Studies. Recently it has been
established that luminescent compounds with internal cavities find potential applications in host-guest chemistry, in molecular recognition, and as sensors.9-21,32-34 Since the rectangles 1-4 contain a large cavity and are luminescent, they can be tested for host-guest interactions. To check the ability of 1-4 to act as hosts, we have studied the reactions of these rectangles with several nitroaromatics and quinones, good electron acceptors, and aromatic amines, electron donors. Interestingly, these substrates quench the lumines-cence of the rectangles efficiently and have quenching rate constants (kq) in the range 3.0 × 107-6.2 × 1011M-1 s-1 (kqvalues have been calculated from Stern-Volmer plots using the luminescence intensity and lifetime data). The decrease in the emission intensity of the rectangle 3 with the increase in the concentration of the quencher (1,2-chloranil) is shown in Figure 7. The kq values for the quenching of 2-4 with several quinones, nitroaromatics, and amines and the sample Stern-Volmer plots are given in the Supporting Information (Table T6 and Figure F4). It is important to point out that though the Stern-Volmer plots
(27) Strouse, G. F.; Schoonover, J. R.; Duesing, R.; Boyde, S.; Jones, W. E., Jr.; Meyer, T. J. Inorg. Chem. 1995, 34, 473.
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Y.; Reibenspies, J. H. Inorg. Chem. 1996, 35, 4989.
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(33) (a) Hunter, C. A. In ComprehensiVe Supramolecular Chemistry; Atwood, J. L., Davies, J. E. D., MacNicol, D. D., Vogtle, F., Lehn, J. M., Eds.; Pergamon: Oxford, U.K., 1996. (b) Hunter, C. A. J. Chem. Soc., Chem. Commun. 1991, 749. (c) Brooksby, P. A.; Hunter, C. A.; McQuillan, A. J.; Purvis, D. H.; Rowan, A. E.; Shannon, R. J.; Walsh, R. Angew. Chem., Int. Ed. Engl. 1994, 33, 2489.
(34) Sanders, J. K. M. Pure Appl. Chem. 2000, 72, 2265. Figure 6. Energy-gap plot for molecular rectangles 1-4, squares 5 and
6, and corners 8 and 9. Excited-state lifetime data were obtained in
deoxygenated CH2Cl2at 298 K.
Table 5. Ground-State Electrochemical Potentials of 1-9
compd solvent Eox, V (∆Ep, mV) Ered, V (∆Ep, mV)
1 acetonitrile +1.05 -1.446
-1.606
2 dichloromethane +0.45 -0.94 (i)
+1.35 (160) -1.176 (i) +1.70
3 dichloromethane +0.35 (i) -1.07 (i)
+1.35 (191) -1.54 (i) +1.64 (53)
4 dichloromethane +0.36 (i) -1.06 (i)
+1.35 (133) -1.40 (122) +1.67 (129) 5 acetonitrile +1.58 -0.92 -1.23 6 acetonitrile +1.35 -1.15 -1.26 7 tetrahydrofuran -1.70 (i) 8 acetonitrile +1.36 -1.57 -1.67
9 dichloromethane +1.09 (i) -1.69 (i)
-1.97 (i)
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drawn from the luminescence intensity and lifetime data are linear, the intensity quenching is more efficient than lifetime quenching implying contribution of static quenching.35,36This means that ground-state complex formation between the rectangle and the quencher is possible leading to both static and dynamic quenching. Thus, it is essential to resolve the two contributions to get the rate constants for the dynamic and static quenching processes. To realize the extent of binding between the rectangle and the quencher, the binding constants have been calculated from the modified Stern-Volmer eq 1 or by the Benesi-Hildebrand method:37,38
Here Ioand I are the emission intensities of rectangles 2-4 in the absence and presence of quenchers, respectively, τo is the excited-state emission lifetime of rectangles, kqis the quenching rate constant, [Q] is the concentration of quencher, and K is the binding constant. The rate constants obtained from the linear part of the Io/I vs [Q] plots at low [Q] are high compared to the values obtained fromτo/τ vs [Q] plots. Further, the binding constants have been calculated from eq 1 and the values for 1,4-naphthaquinone with 2-4 are 280, 295, and 1202 M-1, respectively, and for 9,10-anthraquinone with 2 and 4 are 124 and 178 M-1, respectively. These results point out that the major contribution for the quenching process comes from static quenching. i.e., quenching after the formation of associated complex between the rectangle and the quencher.
In summary, we have accomplished the synthesis of light-emitting neutral rhenium-based molecular rectangles that possess large cavity sizes having no counterions. By a judicial choice of bridging ligands, we were able to tune the
excited-state lifetime of the rectangles from 72 to 495 ns. Fine-tuning of the cavity size and excited-state properties of these molecular rectangles extend their applications to study the excited-state electron-transfer reactions and molecular rec-ognition capabilities.
Experimental Section
Chemicals. Reagents were used as received. All manipulations were performed under a nitrogen atmosphere using standard Schlenk techniques, and chromatographic separations were carried out in air. Acetone, acetonitrile, dichloromethane, and hexane were dried over CaH2and were freshly distilled before use. Compounds 4,4′
-dipyridylacetylene (dpa), 4,4′-dipyridylbutadiyne (dpb), and 1,4-bis(4′-pyridylethynyl)benzene (bpeb), were synthesized by published methods.39,40Tetrabutylammonium perchlorate (TBAP) was dried
at 100°C for 24 h prior to use.
Instrumentation. IR spectra were recorded on a Perkin-Elmer 882 FT-IR spectrophotometer. UV-visible spectra were obtained on a Hewlett-Packard-8453 spectrophotometer at room temperature in 1-cm quartz cell. The fluorescence spectra were collected by using a Hitachi F-4500 fluorescence spectrophotometer under a nitrogen atmosphere. NMR spectra were recorded on Bruker AC 300 and AMX-400 FT-NMR spectrometers. Elemental analyses were performed using a Perkin-Elmer 2400 CHN elemental analyzer. Electrochemical measurements were recorded on a BAS 100B/W EC Workstation. The electrochemical cell consisted of a three-electrode configuration (glassy-carbon electrode, platinum counter electrode, Ag/AgNO3reference electrode). The ferrocene/
ferrocenium couple served as internal reference. The scan rate was 100 mV/s, unless otherwise noted. Cyclic voltammograms were obtained in deoxygenated anhydrous CH3CN and CH2Cl2with the
complexes under investigations (1.0× 10-3M) and 0.1 M TBAP as supporting electrolyte.
Synthesis of [{Re(CO)3(µ-bpy)Br}{Re(CO)3(µ-pz)Br}]2(1).
The details of the synthesis of bimetallic edge{Re(CO)4Br}2(
µ-bpy) and rectangle [{Re(CO)3(µ-bpy)Br}{Re(CO)3(µ-pz)Br}]2(1)
were given in the previous report.20a
Synthesis of [{Re(CO)3(µ-bpy)Br}{Re(CO)3(µ-dpa)Br}]2(2).
A CH2Cl2solution of Me3NO (38 mg, 0.51 mmol) was added to a
solution of{Re(CO)4Br}2(µ-bpy) (228 mg, 0.25 mmol) in CH2Cl2
(200 mL) and CH3CN (1 mL). The reaction mixture was stirred at
5°C for 3 h and filtered through Celite. The solvent was removed under vacuum to obtain{Re(CO)4(NCMe)Br}2(µ-bpy). The flask
containing{Re(CO)4(NCMe)Br}2(µ-bpy) was charged with CH2
-Cl2(200 mL), and a solution of 4,4′-dipyridylacetylene (dpa) (45
mg, 0.25 mmol) in CH2Cl2was added dropwise and stirred at 5 °C. Completion of the reaction was monitored by IR spectroscopy, and the solvent was removed under vacuum. The product was subjected to chromatographic separation on a silica gel column using a mixture of acetone and CH2Cl2 (1:99) as eluent to afford the
rectangle 2 (88 mg, 0.042 mmol, 34%) as a bright yellow solid. IR (CH2Cl2): νCO 2030 (vs), 1932 (s), 1896 (s) cm-1. 1H NMR
(acetone-d6): δ 9.04 (d,3J ) 5.9 Hz, H3, 8 H, bpy), 8.91 (d,3J )
6.0 Hz, H3, 8 H, dpa), 8.02 (d, H2, 8 H, bpy), 7.70 (d, H2, 8 H,
dpa).13C NMR (acetone-d
6): δ 196.6, 192.3 (s, 2:1, CO), 156.3
(C3, bpy), 155.7 (C3, dpa), 147.1, 147.0 (C1, bpy), 133.0, 132.9
(C1, dpa), 128.8, 128.7 (C2, bpy), 124.8 (C2, dpa), 93.3, 93.1 (35) Canepa, M.; Fox, M. A.; Whitesell, J. K. J. Org. Chem. 2001, 66,
3886.
(36) (a) Prasad, E.; Gopidas, K. R. J. Am. Chem. Soc. 2000, 122, 3191. (b) Smitha, M. A.; Prasad, E.; Gopidas, K. R. J. Am. Chem. Soc. 2001, 123, 1159.
(37) (a) Lakowicz, J. R. Principles of Fluorescence Spectroscopy, 2nd ed.; Kluwer Academic/Plenum Publishers: New York, 1999. (b) White, H. S.; Becker, W. G.; Bard, A. J. J. Phys. Chem. 1984, 88, 1840. (38) Benesi, M. L.; Hildebrand, J. H. J. Am. Chem. Soc. 1949, 71, 2703.
(39) (a) Lin, J. T.; Sun, S. S.; Wu, J. J.; Lee, L.; Lin, K. J.; Huang, Y. F. Inorg. Chem. 1995, 34, 2323. (b) Ciana, L. D.; Haim, A. J. Heterocycl. Chem. 1984, 21, 607.
(40) Champness, N. R.; Khlobystov, A. N.; Majuga, A. G.; Schroder, M.; Zyk, N. V. Tetrahedron Lett. 1999, 40, 5413.
Figure 7. Emission intensity of rectangle 3 (8× 10-5M) decreasing with the quencher (1,2-chloranil) concentration in the range of (a) 0 M, (b) 2× 10-4M, (c) 3× 10-4M, (d) 4× 10-4M, (e) 5× 10-4M, and (f) 6× 10-4M in CH2Cl2.
Io/I ) (1 + kqτo[Q])(1 + K[Q]) (1)
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(ethynyl, dpa). Anal. Calcd for C56H32N8O12Br4Re4‚4CH3COCH3:
C, 35.42; H, 2.45; N, 4.86. Found: C, 35.88; H, 2.42; N, 4.74. Synthesis of [{Re(CO)3(µ-bpy)Br}{Re(CO)3(µ-dpb)Br}]2(3).
The rectangle 3 was synthesized by following the previously described procedure for 2, using 4,4′-dipyridylbutadiyne (dpb) (46 mg, 0.23 mmol) instead of 4,4′-dipyridylacetylene. Rectangle 3 was obtained as a bright yellow solid. Yield: 125 mg (47%). IR (CH2
-Cl2): νCO2029 (vs), 1931 (s), 1895 (s) cm-1.1H NMR (acetone-d6): δ 9.04 (d,3J ) 6.1 Hz, H3, 8 H, bpy), 8.93 (d,3J ) 5.9 Hz, H3, 8 H, dpb), 8.02 (d, H2, 8 H, bpy), 7.71 (d, H2, 8 H, dpb).13C NMR (acetone-d6): δ 196.6, 196.5, 192.2 (s, 1:1:1, CO), 156.3 (C3, bpy), 155.6 (C3, dpb), 147.0 (C1, bpy), 132.2 (C1, dpb), 129.3 (C2, bpy), 124.8 (C2, dpb), 81.5, 81.2 (C2, ethynyl, dpb), 80.0, 79.9
(C1, ethynyl, dpb). Anal. Calcd for C
60H32N8O12Br4Re4‚6CH3
-COCH3: C, 37.93; H, 2.78; N, 4.54. Found: C, 37.56; H, 2.55; N,
4.48.
Synthesis of [{Re(CO)3(µ-bpy)Br}{Re(CO)3(µ-bpeb)Br}]2(4).
The rectangle 4 was synthesized by following the previously described procedure for 2, using 1,4′-bis(4-pyridylethynyl)benzene (bpeb) (70 mg, 0.25 mmol) instead of 4,4′-dipyridylacetylene. Rectangle 4 was isolated as a bright yellow solid. Yield: 122 mg (43%). IR (CH2Cl2): νCO2028 (vs), 1929 (s), 1894 (s) cm-1.1H
NMR (acetone-d6): δ 9.04 (d,3J ) 5.9 Hz, H3, 8 H, bpy), 8.88 (d, 3J ) 6.6 Hz, H3, 8 H, bpeb), 8.03 (d, H2, 8 H, bpy), 7.71 (m, 8 H,
phenyl, bpeb), 7.65 (d, H2, 8 H, bpeb).13C NMR (acetone-d 6): δ
196.7, 192.3 (s, 2:1, CO), 156.3 (C3, bpy), 155.4 (C3, bpeb), 147.0
(C1, bpy), 134.4 (C1, bpeb), 133.3 (C2, phenyl, bpeb), 128.5 (C2,
bpy), 124.7 (C2, bpeb), 123.6 (C1, phenyl, bpeb), 97.3, 97.2 (C2,
ethynyl, bpeb), 88.8, 88.7 (C1, ethynyl, bpeb). Anal. Calcd for
C72H40N8O12Br4Re4‚6CH3COCH3: C, 41.22; H, 2.92; N, 4.28.
Found: C, 41.22; H, 2.70; N, 4.13.
Excited-State Lifetime Measurements. Excited-state lifetimes of rectangles 1-4 were measured by a home-constructed time-resolved laser spectrometer. The instrument was equipped with a Quanta Ray GCR-170, pulsed Nd:YAG laser. The third harmonic of the laser (355 nm, fwhm ) 10 ns) was used as excitation source. Emission signals were focused into an ARC SpectraPro-500 double monochromator. The monochromator output was sent into a PMT (Hamamatsu, R928). The signal was digitized by a LeCory 9350A digitizer. Single exponential decays were observed in each case, and the lifetimes obtained were found to be reproducible within
(5%. Decay traces were transferred to a personal computer loaded
with the commercial software Origin 4.0. (The luminescence decay profile is shown in the Supporting Information, Figure F3.)
Luminescence Quenching Measurements. The photochemical oxidation/reduction of the molecular rectangles with nitroaromatics, quinones, and aromatic amines was studied by the luminescence quenching technique. The sample solutions were purged with dry nitrogen for 30 min carefully to ensure that there was no change in
the volume of the solution. The quenching rate constant, kq, values
were determined from the Stern-Volmer equation.41-44
Crystallographic Determination. A suitable single crystal with dimensions of 0.35 × 0.18 × 0.12 mm for 1 was selected for indexing and intensity data collection. A total of 1420 frames constituting a hemisphere of X-ray intensity data were collected with a frame width of 0.3°inω and a counting time of 10 s/frame,
using a Bruker SMART CCD diffractometer. The first 50 frames were recollected at the end of data collection to monitor crystal decay. No significant decay was observed. The raw data frames were integrated into SHELX-format reflection files and corrected for Lorentz and polarization effects using the SAINT program and
absorption using the SADABS program (Tmin/max ) 0.2767/
0.4921).45 The space group was determined to be P2
1/c. Direct
methods were used to solve the structure using the SHELX-TL program packages.46All non-hydrogen atoms were refined
aniso-tropically by full-matrix least squares based on F2values on the
basis of 7285 independent reflections out of 18 370 reflections collected. The maximum and the minimum peaks in final difference maps were 1.195 and -0.838 e Å-3. The largest residual density peak is close to the Re atom. Basic information pertaining to crystal parameters and structure refinement is summarized in Table 1, and selected bond distances and angles are provided in Table 2.
Acknowledgment. We thank Academia Sinica and the
National Science Council of the Republic of China for financial support. We are also grateful to Professor Chong Mou Wang for valuable discussions.
Supporting Information Available: Crystallographic data, isotopic distribution patterns of the M+peaks for{Re(CO)4Br}2
-(µ-bpy) and rectangle 1, luminescence quenching rate constants of
rectangles 2-4 with quenchers, and a molecular modeling diagram of 2-4. This material is available free of charge via the Internet at http://pubs.acs.org.
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(45) SMART/SAINT/ASTRO, release 4.03; Siemens Energy & Automation, Inc.: Madison, WI, 1995.
(46) Sheldrick, G. M. SHELX-TL; University of Gottingen: Gottingen, Germany.
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