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10 Nov 2012: ISSN: 1525-2027. Copyright 2006 by the American Geophysical Union 1 of 24. ... GeochemistryGeophysicsGeosystems G3G3 poore et al.: neogene overflow of ncw 10.1029/2005GC001085. 4 of 24.

15 Aug 2012: Rotator pin-ball. Ruijgrok and Cohen [24] have proposed a general studyof mirror and rotator' models. ... Quas, A., Some properties of Lorentz lattice gas models (1996) (to appear).24.

20 Apr 2012: E [vol (Wg(t))] c E [vol (W0(t))]. (7). The expected volume of the Wiener sausage with g 0 is known to satisfy [24, 2]. ... P [Kct ] t exp(c1L). (24). We will now derive an upper bound for P[H̃t].

3 Sep 2012: 6)) and since gn (t, B),. ‖ VJn ( f gn)‖22 infg ‖ f g‖22 c(B)22 Jn t 4τn (24). ... the inequality holding for L 0 large enough and some c > 0, as in (24).

21 Sep 2012: Γ(. 2 2d)2d/(d4). 24/(d4). R. J. Samworth Nonparametric classification. Further regret comparisons.

15 Aug 2012: the links between the Potts partition functionand the Tutte polynomial surveyed earlier by Welsh and Merino, [24]. ... 24] D. J. A. Welsh and C. Merino. The Potts model and the Tutte polyno-mial.

14 Mar 2012: P (Tisol > t) = exp. (c̃d. t. Ψd(t)(1 o(1)). )? (24). Peres et al. [14] and Peres and Sousi [15] studied the detection time for the case when u also ... ClearlyTnonperc Tisol. We conclude with the question below. Question. Do the tail probabilities of

1 Jun 2012: 24]. On Sd the differential operator L coincideswith the usual Laplace–Beltrami operator, and we have. ... As mentioned in (24) abovethis is tantamount to assuming a classical t -Hölder condition on f.

13 Sep 2012: K}. We aim to minimise the misclassification error rate orrisk :. Risk(C) = P(. C(X) 6= Y). September 13, 2012- 24. R.

15 Aug 2012: mains unproved. Using Theorem 4.2 and an argument of Zhang (see [24, p. ... Related Fields 92, 511–527. 24. Grimmett, G. R. (1989), Percolation, Springer–Verlag, Berlin.