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2
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0004576555
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(personal communication): incidentally, a similar approximation gives the correct long-time survival probability of the random walk in first passage time problems
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S. Redner (personal communication): incidentally, a similar approximation gives the correct long-time survival probability of the random walk in first passage time problems.
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Redner, S.1
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4
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85034300741
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note
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Scheraga has argued that, for a Gaussian smoothing transformation, the catchment region with the greatest area will be the last surviving minimum of the transformed function. This is true in one dimension when the local minima of the objective function are well separated. In that case, the magnitude of the integral over each well is most negative for the well of greatest volume. For the Gaussian kernel the separation between minima that is required for this argument to hold will be greater than for the case of the "top-hat" smoothing function. It follows that the argument that the last surviving minimum in the smoothing transformation will be the minimum of greatest volume is stronger for the case of the method of bad derivatives.
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6
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0000594925
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L. Piela, J. Kostrowicki, and H. A. Scheraga, J. Phys. Chem., 93, 3339 (1989); J. Kostrowicki, L. Piela, B. J. Cherayil, and H. Scheraga, J. Phys. Chem., 95, 4113 (1991).
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L. Piela, J. Kostrowicki, and H. A. Scheraga, J. Phys. Chem., 93, 3339 (1989); J. Kostrowicki, L. Piela, B. J. Cherayil, and H. Scheraga, J. Phys. Chem., 95, 4113 (1991).
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9
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85034278075
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note
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9 the phase-space trajectory of a noise-contaminated evolution is smoothed by replacing the geometric center of a suitably chosen neighborhood by its mass center.
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14
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84986512474
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B. R. Brooks, R. Bruccoleri, B. Olafson, D. States, S. Swaninathan, and M. Karplus, J. Comput. Chem., 4, 187 (1983).
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85034274429
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note
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Similarly, when a "tent" smoothing kernel is employed: equation presented the expression for the second derivative of the smoothed function takes on the simple form: equation presented As for the first derivative, this exact second derivative of the smoothed function takes the form of a three-point finite-difference approximation to the second derivative of U(x).
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28
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0002251853
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C. A. Floudas and P. M. Pardalos, Eds., Princeton University Press, Princeton, NJ
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Shalloway, D.1
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