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Radical mono- and trianion species of 1 were generated by chemical reduction in solution in a sealed tube and were detected by ESR spectroscopy measurements. However, their isolation was not performed. See
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Radical mono- and trianion species of 1 were generated by chemical reduction in solution in a sealed tube and were detected by ESR spectroscopy measurements. However, their isolation was not performed. See J. Janata, J. Gendell, C.-Y. Ling,W. Barth, L. Backes, H. B. Mark, Jr., R. G. Lawton, J. Am. Chem. Soc. 1967, 89, 3056-3058
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39
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0031966878
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Scott, Rabinovitz, and co-workers reported the reduction of several corannulene derivatives having annelated six- or five-membered rings. The closed-shell anions were characterized by NMR spectroscopy, however the open-shell ones were not detected.
-
Scott, Rabinovitz, and co-workers reported the reduction of several corannulene derivatives having annelated six- or five-membered rings. The closed-shell anions were characterized by NMR spectroscopy, however the open-shell ones were not detected. See A.Weitz, E. Shabtai, M. Rabinovitz, M. S. Bratcher, C. C. McComas, M. D. Best, L. T. Scott, Chem. Eur. J. 1998, 4, 234-239
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43
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77956043306
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Ph.D. Thesis, Boston College
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P.-C. Cheng, Ph.D. Thesis, Boston College, 1996
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Cheng, P.-C.1
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33747448920
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Petrukhina, M.A.5
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46
-
-
77956055450
-
-
The quinone derivative 7 forms convex-convex type dimeric pairs in the crystal. To our knowledge, this is the first convex- convex type crystal structure in bowl-shaped π-conjugated molecules. For details, see the Supporting Information
-
The quinone derivative 7 forms convex-convex type dimeric pairs in the crystal. To our knowledge, this is the first convex- convex type crystal structure in bowl-shaped π-conjugated molecules. For details, see the Supporting Information.
-
-
-
-
47
-
-
77956028125
-
-
The stability of the samples was judged from the signal intensity of their solution ESR spectra
-
The stability of the samples was judged from the signal intensity of their solution ESR spectra.
-
-
-
-
48
-
-
77956054988
-
-
23Na ENDOR/TRIPLE spectra are shown in the Supporting Information
-
23Na ENDOR/TRIPLE spectra are shown in the Supporting Information.
-
-
-
-
49
-
-
77956047061
-
-
All DFT calculations were performed with the Gaussian03 program (revision E.01) Gaussian, Inc., Wallingford CT, 2004; the full reference is given in the Supporting Information
-
All DFT calculations were performed with the Gaussian03 program (revision E.01) Gaussian, Inc., Wallingford CT, 2004; the full reference is given in the Supporting Information.
-
-
-
-
50
-
-
77956029110
-
-
- and the dianion species. The voltammogram is given in the Supporting Information
-
- and the dianion species. The voltammogram is given in the Supporting Information.
-
-
-
-
51
-
-
77956050095
-
-
-, and 6.3° and 0.67 Å for the dianion, respectively. The detailed data are described in the Supporting Information
-
-, and 6.3° and 0.67 Å for the dianion, respectively. The detailed data are described in the Supporting Information.
-
-
-
-
52
-
-
84962409127
-
-
On the basis of theory it is suggested that their curvature shallows in a stepwise manner with increasing negative charge. For 1, see
-
On the basis of theory it is suggested that their curvature shallows in a stepwise manner with increasing negative charge. For 1, see: C. Bruno, R. Benassi, A. Passalacqua, F. Paolucci, C. Fontanesi, M. Marcaccio, E. A. Jackson, L. T. Scott, J. Phys. Chem. B 2009, 113, 1954-1962.
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J. Phys. Chem. B
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, pp. 1954-1962
-
-
Bruno, C.1
Benassi, R.2
Passalacqua, A.3
Paolucci, F.4
Fontanesi, C.5
Marcaccio, M.6
Jackson, E.A.7
Scott, L.T.8
-
53
-
-
57349148274
-
-
For the phenalenyl-fused corannulene, see
-
For the phenalenyl-fused corannulene, see: S. Nishida, Y. Morita, A. Ueda, T. Kobayashi, K. Fukui, K. Ogasawara, K. Sato, T. Takui, K. Nakasuji, J. Am. Chem. Soc. 2008, 130, 14954-14955.
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J. Am. Chem. Soc.
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, pp. 14954-14955
-
-
Nishida, S.1
Morita, Y.2
Ueda, A.3
Kobayashi, T.4
Fukui, K.5
Ogasawara, K.6
Sato, K.7
Takui, T.8
Nakasuji, K.9
-
54
-
-
77956017039
-
-
The details of bond-length analyses and resonance structures of these redox species are shown in the Supporting Information
-
The details of bond-length analyses and resonance structures of these redox species are shown in the Supporting Information.
-
-
-
-
55
-
-
77956021246
-
-
The temperature dependence of the ESR intensity is given in the Supporting Information. The absolute concentration of the radical was accurately measured by exploiting a dual-sampleport cavity
-
The temperature dependence of the ESR intensity is given in the Supporting Information. The absolute concentration of the radical was accurately measured by exploiting a dual-sampleport cavity.
-
-
-
-
56
-
-
77956047969
-
-
The simulated ESR spectra and hfccs are shown in the Supporting Information
-
The simulated ESR spectra and hfccs are shown in the Supporting Information.
-
-
-
-
57
-
-
0003013464
-
-
- is similar to that of several alkali-metal salts of an o-benzosemiquinone radical (see reference [4d]). In contrast, the magnitude of hfcc of an alkali-metal counterion of fluorenone ketyl or pbenzosemiquinone radical salts decreases with decreasing temperature. See
-
- is similar to that of several alkali-metal salts of an o-benzosemiquinone radical (see reference [4d]). In contrast, the magnitude of hfcc of an alkali-metal counterion of fluorenone ketyl or pbenzosemiquinone radical salts decreases with decreasing temperature. See N. Hirota, J. Am. Chem. Soc. 1967, 89, 32-41
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(1967)
J. Am. Chem. Soc.
, vol.89
, pp. 32-41
-
-
Hirota, N.1
-
58
-
-
0001183630
-
-
See also references [4,5]
-
M. P. Khakhar, B. S. Prabhananda, M. R. Das, J. Am. Chem. Soc. 1967, 89, 3100-3106. See also references [4,5].
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, pp. 3100-3106
-
-
Khakhar, M.P.1
Prabhananda, B.S.2
Das, M.R.3
-
59
-
-
77956054515
-
-
The y axis is the line passing through the two oxygen atoms (shown in red), and the xy plane is coplanar with the semiquinone moiety. The z axis is perpendicular to the xy plane and passes through the origin O. The parameter θ represents the angle between the x axis and the line connecting the sodium cation with the origin O. Positive and negative q values mean that the sodium cation is in the concave and convex sides, respectively
-
The y axis is the line passing through the two oxygen atoms (shown in red), and the xy plane is coplanar with the semiquinone moiety. The z axis is perpendicular to the xy plane and passes through the origin O. The parameter θ represents the angle between the x axis and the line connecting the sodium cation with the origin O. Positive and negative q values mean that the sodium cation is in the concave and convex sides, respectively.
-
-
-
-
60
-
-
77956043756
-
-
The calculated hfccs of protons are unchanged without angular dependence
-
The calculated hfccs of protons are unchanged without angular dependence.
-
-
-
-
61
-
-
77956020822
-
-
Na| change when the sodium cation moves on the x axis was examined by DFT calculations. For details, see the Supporting Information
-
Na| change when the sodium cation moves on the x axis was examined by DFT calculations. For details, see the Supporting Information.
-
-
-
-
62
-
-
77956027695
-
-
This situation is in contrast to a planar o-benzosemiquinone radical salt without such sign dependence of θ
-
This situation is in contrast to a planar o-benzosemiquinone radical salt without such sign dependence of θ.
-
-
-
-
63
-
-
77956044465
-
-
- (0.064 and 0.061 mT; bowl depth=0.62 Å). For details, see the Supporting Information
-
- (0.064 and 0.061 mT; bowl depth=0.62 Å). For details, see the Supporting Information.
-
-
-
-
64
-
-
34247538143
-
-
For our recent studies on planar neutral p radicals based on phenalenyl and oxophenalenoxyl systems, see
-
For our recent studies on planar neutral p radicals based on phenalenyl and oxophenalenoxyl systems, see: S. Nishida, Y. Morita, K. Fukui, K. Sato, D. Shiomi, T. Takui, K. Nakasuji, Angew. Chem. 2005, 117, 7443-7446
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37649006955
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Y. Morita, S. Suzuki, K. Fukui, S. Nakazawa, H. Kitagawa, H. Okamoto, A. Naito, A. Sekine, Y. Ohashi, M. Shiro, K. Sasaki, D. Shiomi, K. Sato, T. Takui, K. Nakasuji, Nat. Mater. 2008, 7, 48-51
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Phenalenyls, cyclopentadienyls, and other carbon-centered radicals
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For a review of recent phenalenyl chemistry, see, (Ed.: R. Hicks), Wiley-Blackwell, in press
-
For a review of recent phenalenyl chemistry, see: "Phenalenyls, Cyclopentadienyls, and Other Carbon-Centered Radicals": Y. Morita, S. Nishida in Stable Radicals: Fundamentals and Applied Aspects of Odd-electron Compounds (Ed.: R. Hicks), Wiley- Blackwell, in press.
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Stable Radicals: Fundamentals and Applied Aspects of Odd-Electron Compounds
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25144432424
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Metal complexes of bowl-shaped π-conjugated molecules have been extensively studied for corannulene and sumanene derivatives. Most of them are closed-shell systems, and electronic-spin structure and magnetic properties are not revealed. See
-
Metal complexes of bowl-shaped π-conjugated molecules have been extensively studied for corannulene and sumanene derivatives. Most of them are closed-shell systems, and electronic-spin structure and magnetic properties are not revealed. See M. A. Petrukhina, L. T. Scott, Dalton Trans. 2005, 2969-2975
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(2005)
Dalton Trans.
, pp. 2969-2975
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Petrukhina, M.A.1
Scott, L.T.2
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74
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77956031534
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T. Amaya, W.-Z. Wang, H. Sakane, T. Moriuchi, T. Hirao, Angew. Chem. 2010, 122, 413-416
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(2010)
Angew. Chem.
, vol.122
, pp. 413-416
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Amaya, T.1
Wang, W.-Z.2
Sakane, H.3
Moriuchi, T.4
Hirao, T.5
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75
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73349089963
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and references cited therein
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Angew. Chem. Int. Ed. 2010, 49, 403-406, and references cited therein.
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(2010)
Angew. Chem. Int. Ed.
, vol.49
, pp. 403-406
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76
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77956051168
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- is expected
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- is expected.
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77
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0035977623
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We have calculated the bowl-inversion energy barrier of the corannulene-based semiquinone radicals with different curvature using the Siegel equation, see the Supporting Information). For further investigation of the inversion from the experimental side, variable-temperature NMRspectroscopy measurements and pulsed ESR spectroscopy for the direct observation of the dynamic molecular and electronic-spin structures are underway
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We have calculated the bowl-inversion energy barrier of the corannulene-based semiquinone radicals with different curvature using the Siegel equation (T. J. Seiders, K. K. Baldridge, G. H. Grube, J. S. Siegel, J. Am. Chem. Soc. 2001, 123, 517-525; see the Supporting Information). For further investigation of the inversion from the experimental side, variable-temperature NMRspectroscopy measurements and pulsed ESR spectroscopy for the direct observation of the dynamic molecular and electronic-spin structures are underway.
-
(2001)
J. Am. Chem. Soc.
, vol.123
, pp. 517-525
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-
Seiders, T.J.1
Baldridge, K.K.2
Grube, G.H.3
Siegel, J.S.4
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