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1842328286
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note
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In this region, the standard methods for computing steepest descent lines would fail to locate the correct relaxation path (e.g., these methods usually retain the symmetry of the initial structure). Accordingly, for this region, we have computed the MEP using a computational strategy based upon a series of IRD optimizations performed at increasing values of the distance (radius of the hypersphere) from the starting point.
-
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-
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46
-
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1842294868
-
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note
-
32d) yield the same charge distribution. Thus, in Figure 5 we report Mulliken charges only.
-
-
-
-
47
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33744614883
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(b) Computed with the program: NBO Version 3.1, Glendening, E. D.; Reed, A. E. Carpenter, J. E.; Weinhold, F. See also: Reed, A. E.; Weinhold, F. J. Am. Chem. Soc. 1980, 102, 7211).
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48
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33744614883
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(b) Computed with the program: NBO Version 3.1, Glendening, E. D.; Reed, A. E. Carpenter, J. E.; Weinhold, F. See also: Reed, A. E.; Weinhold, F. J. Am. Chem. Soc. 1980, 102, 7211).
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1842412785
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note
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These surfaces have been computed using ab initio MC-SCF theory with a 6-31G* basis set. We are grateful to Dr. Barbara Frabboni for providing these data.
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54
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0001612847
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56
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1842375376
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note
-
2·dm(s)/ds = -dE(s)/ds where s is the photoisomerization coordinate and m(s) and E(S) are the corresponding effective reduced mass and potential energy along the composite MEP series of FC →IC → trans-product.
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-
-
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57
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1842370565
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note
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+ configurations there is a flat region centered on stretched structures. The detailed topology of this region will be presented in a more technical paper.
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