10.1002/chem.202001919
Chemistry - A European Journal
COMMUNICATION
dimeric cation radical with syn-syn-syn conformer has the most
stable structure, furthermore, the TD-DFT calculation indicated
electron density is mainly delocalized within the pyrene groups in
Fig. 4. a) Deconvolution absorption spectra from titration. B) ESI-MS spectrum
+●
of dimer cation radical (T-tmp)2
.
(T-tmp)
+•. The investigation of novel molecular tweezers with
2
more pyrene units are under progress in our lab.
In order to further study the structure and electronic
properties of the dimerization products, we performed (TD-)DFT
calculations using CAM-B3LYP-D3BJ/6-31G*+PCM(CH2Cl2)
level of theory (for computational details see the SI). The results
show that the syn-syn-syn structure has the lowest energy (Fig.
5a), which is about 1.5 kcal/mol more stable than the next lowest
structure. The possible structures and corresponding relative
energies are summarized in the SI.
Conflicts of interest
There are no conflicts to declare.
Acknowledgements
The dimerization energy for the formation of (T-tmp)2+• is
about 40 kcal/mol. It should be noted that this value for the
The authors would like to thank Prof. Scott A. Reid (Marquette
University) for helpful discussion and the National Science
Foundation (CHE-1508677) for financial support. The
computational calculations were performed on the high-
performance computing cluster Pere at Marquette University.
+•
formation of (TMP)2 is around 12 kcal/mol. The distance
between pyrene layers are 3.4, 3.3 and 3.5 Å in (T-tmp)2+•, which
is slightly shorter than model compound TMP with 3.5 Å (Fig. 5b).
The TD-DFT calculation results indicated the electron density is
mainly delocalized within the pyrene groups and the spectrum
simulation of (TMP)2+• show the intense NIR absorption (>1500
nm, max = 2430 nm) corresponding to HOMO to LOMO transition,
which is in good agreement with our experiment results. In case
of (TMP)2+•, the predicted NIR absorption (>1300 nm,max = 2000
nm) is also well matched with experiment results (>1400 nm, max
= 1965 nm). Also, the calculated near-IR transition shows lower
Keywords: tweezers • cation radical • dimer • charge transfer •
trimethylpyrene
[1] a) J. K. Kochi, R. Rathore and P. Le Magueres, J. Org. Chem. 2000, 65,
6826-6836; b) J. A. E. H. van Haare, L. Groenendaal, E. E. Havinga, R. A.
J. Janssen and E. W. Meijer, Angew. Chem., Int. Ed. Engl. 1996, 35, 638-
640; c) T. S. Navale, K. Thakur, V. S. Vyas, S. H. Wadumethrige, R. Shukla,
S. V. Lindeman and R. Rathore, Langmuir 2012, 28, 71-83; d) M. Banerjee,
R. Shukla and R. Rathore, J. Am. Chem. Soc. 2009, 131, 1780-1786; e) S.
Wiedbrauk, T. Bartelmann, S. Thumser, P. Mayer and H. Dube, Nat.
Commun. 2018, 9, 1-9.
+•
oscillator strength for (TMP)2+• compared to (T-tmp)2 (0.11 vs
0.13, respectively; Fig. 5c and Fig. 5d) which agrees with the
experimental data (Fig. 3).
[2] a) I. C. Lewis and L. S. Singer, The Journal of Chemical Physics 1965, 43,
2712-2727; b) C. Kröhnke, V. Enkelmann and G. Wegner, Angewandte
Chemie International Edition in English 1980, 19, 912-919; c) J. A. Ayllón, I.
C. Santos, R. T. Henriques, M. Almeida, E. B. Lopes, J. Morgado, L. Alcácer,
L. F. Veiros and M. T. Duarte, Journal of the Chemical Society, Dalton
Transactions 1995, 3543-3549; d) V. Gama, R. T. Henriques, G. Bonfait, L.
C. Pereira, J. C. Waerenborgh, I. C. Santos, M. T. Duarte, J. M. P. Cabral
and M. Almeida, Inorganic Chemistry 1992, 31, 2598-2604; e) M. A. J.
Rodgers, Journal of the Chemical Society, Faraday Transactions 1: Physical
Chemistry in Condensed Phases 1972, 68, 1278-1286.
[3] R. Rathore, A. S. Kumar, S. V. Lindeman and J. K. Kochi, The Journal of
Organic Chemistry 1998, 63, 5847-5856.
[4] a) S. C. Zimmerman, Z. Zeng, W. Wu and D. E. Reichert, Journal of the
American Chemical Society 1991, 113, 183-196; b) S. C. Zimmerman, C. M.
VanZyl and G. S. Hamilton, Journal of the American Chemical Society 1989,
111, 1373-1381; c) S. C. Zimmerman and C. M. VanZyl, Journal of the
American Chemical Society 1987, 109, 7894-7896.
[5] K. Thakur, D. Wang, S. V. Lindeman and R. Rathore, Chemistry – A
European Journal 2018, 24, 13106-13109.
+•
Fig. 5. DFT optimized structures of a) (T-tmp)2 and b) (TMP)2+•; TD-DFT
[6] M. Banerjee, V. S. Vyas, S. V. Lindeman and R. Rathore, Chem. Commun.
(Cambridge, U. K.) 2008, 1889-1891.
calculation of spectrum simulation of c) (T-tmp)2 and d) (TMP)2+•, the
corresponding HOMO and LUMO isovalue plots (±0.02 au) are inserted.
+•
[7] a) M. V. Ivanov, K. Thakur, A. Boddeda, D. Wang and R. Rathore, J. Phys.
Chem. C 2017, 121, 9202-9208; b) W. Y. Heng, J. Hu and J. H. K. Yip,
Organometallics 2007, 26, 6760-6768.
[8] H. Maeda, T. Maeda, K. Mizuno, K. Fujimoto, H. Shimizu and M. Inouye,
Chem. - Eur. J. 2006, 12, 824-831.
In summary, we report the design and synthesis of a new
molecular tweezer (T-tmp) with electron-rich pincers. The
electrochemical properties indicated the two pyrenyl groups have
a weak interaction after one electron oxidation. Furthermore,
monocationic radicals and self-assembled dimer radicals were
successfully prepared by chemical-oxidative titration. The
dimerization binding constant was determined to be 5.0 (±1.5) ×
105 M-1. With the aid of DFT calculations, we found that the
[9] T. Cooper, A. Novak, L. D. Humphreys, M. D. Walker and S. Woodward,
Advanced Synthesis & Catalysis 2006, 348, 686-690.
[10] D. Qiu, F. Mo, Z. Zheng, Y. Zhang and J. Wang, Organic Letters 2010, 12,
5474-5477.
[11] D. Wang, M. R. Talipov, M. V. Ivanov and R. Rathore, J. Am. Chem. Soc.
2016, 138, 16337-16344.
4
This article is protected by copyright. All rights reserved.