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3943078972
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note
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2 and R = Me in 100 mL of toluene at 0°C for 15 min.
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18
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3943059215
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note
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5 g/mol provides an estimate for the ratio of termination events to insertion events of 1:28900. Applying Boltzmann statistics to this ratio gives a ΔΔG‡ of 5.6 kcal/mol and an estimate for the termination barrier of 15.5-16.5 kcal/mol. In calculating ΔΔG‡ we have assumed that every hydrogen transfer event leads to the loss of the chain and, consequently, chain termination.
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20
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0029011701
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K. M. M.
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Cornell, W. D.; Cieplak, P.; Bayly, C. I.; Gould, I. R., Jr.; K. M. M.; Ferguson, D. M.; Spellmeyer, D. C.; Fox, T.; Caldwell, J. W.; Kollman, P. A. J. Am. Chem. Soc. 1995, 117, 5179.
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Spellmeyer, D.C.6
Fox, T.7
Caldwell, J.W.8
Kollman, P.A.9
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21
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0042041206
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Rappé, A. K.; Casewit, C. J.; Colwell, K. S.; Goddard, W. A., III; Skiff, W. M. J. Am. Chem. Soc. 1992, 114, 10024.
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22
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3943063306
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note
-
CM-N2-CA, Ni-N2-CA, and N2-CM-CT angle parameters were replaced by CM-N*-CT, H-N2-CA, and CM-CM-CT angle parameters of the AMBER95 force field, respectively. The X-N2-CM-X torsional parameters was replaced by the X-N2-CA-X parameter of the AMBER95 force field. The X-Ni-N2-X torsional parameter was assigned a barrier of zero.
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23
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0001251327
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Woo, T. K.; Margl, P. M.; Blöchl, P. E.; Ziegler, T. Organometallics 1997, 16, 3454.
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Ziegler, T.4
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24
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0030465140
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Woo, T. K.; Margl, P. M.; Lohrenz, J. C. W.; Blöchl, P. E.; Ziegler, T. J. Am. Chem. Soc. 1996, 118, 13021.
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Ziegler, T.5
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25
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15844413581
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Margl, P.; Lohrenz, J. C. W.; Blöchl, P.; Ziegler, T. J. Am. Chem. Soc. 1996, 118, 4434.
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Ziegler, T.4
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31
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36549097329
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De Raedt, B.; Sprik, M.; Klein, M. L. J. Chem. Phys. 1984, 80, 5719.
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De Raedt, B.1
Sprik, M.2
Klein, M.L.3
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32
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3943076911
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Unpublished work
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Blöchl, P. E. Unpublished work.
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Blöchl, P.E.1
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33
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3943075519
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Animations of the simulations presented here are available at our research group's web site at 〈http://www.chem.ucalgary.ca/groups/ziegler〉.
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34
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0031020614
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Deng, L.; Margl, P. M.; Ziegler, T. J. Am. Chem. Soc. 1997, 119, 1094.
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35
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3943099672
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note
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23 In the present case, one might expect a larger hysteresis due to the low-frequency modes of the ligands in the QM/MM simulation. In this case, however, the good agreement in the free energy barriers with static QM/ MM calculations indicates that the effect is small as well.
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