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3 (R. G. Aickin, N. S. Bayliss, A. L. G. Rees, Proc. Roy. Soc. London 1938, A169, 234-245; e) in solution the complex exhibits a large solvatochromic shift: N. S. Bayliss, J. Chem. Phys. 1950, 18, 292-296; f) Nature 1949, 163, 764-765.
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0642285511
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3 (R. G. Aickin, N. S. Bayliss, A. L. G. Rees, Proc. Roy. Soc. London 1938, A169, 234-245; e) in solution the complex exhibits a large solvatochromic shift: N. S. Bayliss, J. Chem. Phys. 1950, 18, 292-296; f) Nature 1949, 163, 764-765.
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Kokovin, G.A.1
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0642346814
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3 (R. G. Aickin, N. S. Bayliss, A. L. G. Rees, Proc. Roy. Soc. London 1938, A169, 234-245; e) in solution the complex exhibits a large solvatochromic shift: N. S. Bayliss, J. Chem. Phys. 1950, 18, 292-296; f) Nature 1949, 163, 764-765.
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0000010875
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3 (R. G. Aickin, N. S. Bayliss, A. L. G. Rees, Proc. Roy. Soc. London 1938, A169, 234-245; e) in solution the complex exhibits a large solvatochromic shift: N. S. Bayliss, J. Chem. Phys. 1950, 18, 292-296; f) Nature 1949, 163, 764-765.
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0642346809
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3 (R. G. Aickin, N. S. Bayliss, A. L. G. Rees, Proc. Roy. Soc. London 1938, A169, 234-245; e) in solution the complex exhibits a large solvatochromic shift: N. S. Bayliss, J. Chem. Phys. 1950, 18, 292-296; f) Nature 1949, 163, 764-765.
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Aickin, R.G.1
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19
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0346488520
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3 (R. G. Aickin, N. S. Bayliss, A. L. G. Rees, Proc. Roy. Soc. London 1938, A169, 234-245; e) in solution the complex exhibits a large solvatochromic shift: N. S. Bayliss, J. Chem. Phys. 1950, 18, 292-296; f) Nature 1949, 163, 764-765.
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0348084266
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3 (R. G. Aickin, N. S. Bayliss, A. L. G. Rees, Proc. Roy. Soc. London 1938, A169, 234-245; e) in solution the complex exhibits a large solvatochromic shift: N. S. Bayliss, J. Chem. Phys. 1950, 18, 292-296; f) Nature 1949, 163, 764-765.
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0642285508
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0642346813
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Institut für Physikalische Chemie, Universität Erlangen-Nürnberg, unpublished results
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Brehm, B.1
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For a review see R. Herges, Angew. Chem. 1995, 107, 57-59; Angew. Chem. Int. Ed. Engl. 1995, 34, 51-53.
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30
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33947293427
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∞h symmetry for bromine dimers. The structures were optimized within their point group and characterized by harmonic frequency calculations at the DFT level. Stationary points of higher order were further investigated by following the imaginary frequency modes with intrinsic reaction coordinate calculations (IRC): a) D. G. Truhlar, A. Kuppermann, J. Am. Chem. Soc. 1971, 93, 1840-1851; b) K. Fukui, Acc. Chem. Res. 1981, 14, 363-368; c) Pure Appl. Chem. 1982, 54, 1825-1836. Structure 3 was found with this procedure. All other structures were converted into known stationary points of lower order.
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33751044609
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∞h symmetry for bromine dimers. The structures were optimized within their point group and characterized by harmonic frequency calculations at the DFT level. Stationary points of higher order were further investigated by following the imaginary frequency modes with intrinsic reaction coordinate calculations (IRC): a) D. G. Truhlar, A. Kuppermann, J. Am. Chem. Soc. 1971, 93, 1840-1851; b) K. Fukui, Acc. Chem. Res. 1981, 14, 363-368; c) Pure Appl. Chem. 1982, 54, 1825-1836. Structure 3 was found with this procedure. All other structures were converted into known stationary points of lower order.
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Fukui, K.1
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0000866922
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∞h symmetry for bromine dimers. The structures were optimized within their point group and characterized by harmonic frequency calculations at the DFT level. Stationary points of higher order were further investigated by following the imaginary frequency modes with intrinsic reaction coordinate calculations (IRC): a) D. G. Truhlar, A. Kuppermann, J. Am. Chem. Soc. 1971, 93, 1840-1851; b) K. Fukui, Acc. Chem. Res. 1981, 14, 363-368; c) Pure Appl. Chem. 1982, 54, 1825-1836. Structure 3 was found with this procedure. All other structures were converted into known stationary points of lower order.
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