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14 Feb 2012: Which works best? Blade angle 45 degrees. Blade angle 20 degrees.

15 Oct 2012: 4096. 0. 5. 10. 15. 20. 25. 30. 35. 40. 45. ... 5. 10. 15. 20. 25. 30. 35. 40. 45. T(s. ). Dense Matrix Trace 76.148163264. Figure 4: Timings for sparseand dense matrix products in fccsilicon with 4 NGWFs per

15 Oct 2012: No Cropping Cropping00.20.40.60.8. 11.21.41.61.8. 2W. all t. ime. per. mat. rix.

15 Oct 2012: 15. 20. 25. 30. 3. 3.5. 4. 4.5. 5. 5.5. 6. ... 5.3. -5.1. -4.9. x. yV. 0 5 10 15 20 25 30 0.

15 Oct 2012: 10.0. -5.0. 0.0. 5.0. 10.0. 15.0. 20.0. 0 1 2 3 4 5 6 7. ... 2eV within the bandgap. 1e-30. 1e-25. 1e-20. 1e-15. 1e-10. 1e-05. Def.

24 Jun 2012: 256809-4. ground-state incompressibility [37], noise correlations[20,38], and possibly a direct measurement of quasiholestatistics [11]. ... Rev. Lett. 96, 180407. (2006).[20] R. N. Palmer, A. Klein, and D.

26 Jan 2012: 1. Thisallows for an alternative potential implementation, usingan optical dice lattice for single species atoms [18].Negative hopping can be achieved in principle by shakinglattice sites [20]; the application in this ... Gerbier (private communications).

26 Jan 2012: 20 JANUARY 2012. 0031-9007=12=108(3)=036806(4) 036806-1 2012 American Physical Society. ... Bonderson and J. K. Slingerland, Phys. Rev. B 78,. 125323 (2008).[20] A.

10 Oct 2012: 20 CHAPTER 2. SECOND QUANTISATION. where n is the total number of particles in state (for fermions, Pauli exclusion en-forces the constraint n = 0, 1, i.e. ... 20 (2.6). where =", # is the spin quantum number, denotes the set of additional quantumnumbers

10 Oct 2012: 1.20). Yet a closer inspection reveals that these identities are in fact in conflict with the Coulomb gauge!

8 Mar 2012: and want to market a 1kW heat source, you can simply install 20 of your 50 watt devices, and then, by simple arithmetic, you end up with a 1kW heat source.

29 Jun 2012: Cm); they form stochastic submatrices. 10. Page 23, Line 20 and below, and the whole of Page 24 should read asfollows:. ... 25. Page 107, Lines 19-20 down:black and white. black or white.

29 Mar 2012: 4. 20) Page 95, Line 6 from above: Problem 1.71. ... 2/2. 6) Page 155, Line 8 from above, after the answer to Problem 2.20.

6 Nov 2012: He needs (s=8) kg to survive the winter. Nuts can be hidden in (n=20) places, of which a random (m=10) will be vandalized (or forgotten).

26 Apr 2012: Choosing tours at random is. p> =1. 63(1, 5, 5, 5, 20, 5, 5, 20, 5, 5, 20, 20, 20, 20, 60). ... 63(1, 5, 5, 5, 20, 5, 5, 20, 5, 5, 20, 20, 20, 20, 60).

7 Feb 2012: Seminar at Microsoft, Cambridge, June 20, 2011. The Multi-armed Bandit Problem.

19 Jan 2012: 2964. 1384x,1. }. c(x). x0.10.20.30.40.5. 10 20 30 40. {k(n, 2)}40. ... Naval Res Logist Q 20(4):661–672. Samuel E (1970) On some problems in operations research.

21 Mar 2012: Stochastic Optimization and Control. Editor Karreman, Publ. 20, Math Research Center, U.S.

5 Jan 2012: G(x,u,t,η) = η[0.001(50 x)x u] u,. anddη/dt = 0.002(x 10)η. Suppose that x(0) = 20 and that under an optimal policy

21 Mar 2012: Lemma 5.5 gives F(x) = F(x). 20. 6 Bandit Processes and the Gittins Index.

16 Mar 2012: 20). Having completed these lectures you can now attempt all of Examples Sheet 1. ... It would be better to allow 15, 15, 20. Lecture 1 Dynamic Programming.

4 Sep 2012: Number of visits to this page since 20/10/11:. Richard Weber ( rrw1@cam.ac.uk ). Last modified: November 2011.

4 Sep 2012: This map shows the sources of visitors to this Markov Chains course web site over the past 4 days (20-23 October). ... Course Blog. Number of visits to this page since 20/10/11:. Richard Weber ( rrw1@cam.ac.uk ). Last modified: November 2011.

13 Sep 2012: It offers potential improvements for small sample sizes. September 13, 2012- 20.

21 Sep 2012: There are too many subsets to evaluate ŜSSn,τ whenn 20. • ... Statist., 20, 1611–1624. • Meinshausen, N. and Bühlmann, P. (2010) Stability selecti on, J.

21 Sep 2012: 0.00. 0.10. 0.20. 0.30. s. Mar. gina. l Den. sitie. s.

21 Sep 2012: 0 20 40 60 80 100. 0.00. 00. 002. 0.00. 40. ... 1.15. 1.20. d. Reg. retr. atio. R. J. Samworth Nonparametric classification.

21 Sep 2012: One car. 0.5% of the U.S. Library of Congress. 2% of the data collected by the Hubble spacetelescope in the last 20 years. ... One car. 0.5% of the U.S. Library of Congress. 2% of the data collected by the Hubble spacetelescope in the last 20 years. •

10 Nov 2012: 296 Savin et al. [1981] Ellis [1975] 6.099–11.454 1617.864–20.834 30. 574A Pisias et al. ... 20] We have applied the Simulation Extrapolation(SIMEX) algorithm of Cook and Stefanski [1994]and Carroll et al.

20 Dec 2012: 58 104 1:68 103 3:29 103 5:52 1030.50 1:31 104 6:18 104 1:58 103 3:10 103 5:20 1030.51 1:23 104 ... 20 104 1:15 1030.69 3:88 105 1:58 104 3:64 104 6:60 104 1:05 1030.70 3:56 105 1:45 104 3:35 104

26 Nov 2012: 10 x. 20 o(‖x‖2)) and. xjx01. = sj(1 x10 x20 o(‖x‖2)), wewrite. ... 20. ‖x‖2 1. ‖x‖2 o(‖x‖2)). (. 1 αψ(s) αd1j=1. ( sjx0.

20 Apr 2012: ments [20]. See the Remark following the proof of Corollary 1.7 in Section 5. ... where. mj =mj1 4j1. 4. (34). 20. We will set the j in a moment.

21 Nov 2012: This resolves an open question of Aldous [1, Chapter 4, OpenProblem 20] and of Imbuzeiro Oliveira [6]. ... 13. Proof of Theorem 1.7 (for continuous time walk). Consider the graph G7,20.

14 Mar 2012: k such that Xi ξi() B(0, r̃,n), and henceusing (20) we get. ... arXiv:1008.6322v2. [20] D. Stoyan, W.S. Kendall, and J. Mecke. Stochastic Geometry and its Applications.

20 Apr 2012: going to use the Nash-Williams criterion ofrecurrence, which can be found for instance in [20, Chapter 21, Proposition 21.6]. ... c′|In,l|,. since β < 1 and < 2β(n1). Hence using (5.20) we get that.

3 Sep 2012: 20]. 123. A. D. Bull, R. Nickl. While the case of two fixed smoothness classes in Theorem 1 is appealing in itsconceptual simplicity, it does not describe the typical adaptation problem, ... 20). which completes the bound for the type-one errors in view

1 Jun 2012: lim supn. 2 jn d jn. nsupyM. | fn( j, y) E fn(y, d)| D almost sur el y (20). ... We shall use the subsample S2 to select ĵn following this idea, which is due toLepskiı̆ [20], formalised as follows:.

6 Mar 2012: Kj f ‖ ‖Kj ‖r ‖f ‖s C(K, r)2j (11/r) U,(20)a bound that remains true when r = since |2j K(2j (x y))| ‖K‖2j. ... 2nσ 2x 73 U x. } 2ex. Combining the moment estimate Lemma 1 with (20) and (21), we obtain, for2j j (r) < n with j () = j and j

10 Jan 2012: As shown in [12] (see also [20])such estimators can be used in the construction of (near-)adaptive confidence bandsunder certain analytic conditions on the elements of (s). ... Let us briefly describethe results in [12, 20]. Let n be a sequence of

1 Oct 2012: and. 0 rqbi,k rbi1,k for all k 1 i t 20 rbt2,k. ... Personal communication. (2009)[20] M. Schweizer and J. Wissel. Term structures of implied volatilities: Absence of arbitrage and existence results.

15 Aug 2012: 13 (1998), 467–483. 10. Jiang, T., Li, M., Vitányi, P., The average-case area of Heilbronn-type triangles, RandomStructures and Algorithms 20 (2002), 206–219.

15 Aug 2012: We illustrate this approach in the nextsection, by sketching the details in a particular case.Important references include [20, 156, 157, 268]. ... The following theorem is taken from [20] and may be proved in amanner similar to the proof given in the

15 Aug 2012: First,(3.20) k = i 6=? for 1 < i k A(A)where A = f1 = k1 =? g. Now,(3.21) (A) = Yr:srjk1 1sr Yr:sr-k1 2sr Yr 1 2sr ... The last quantity is strictly positive since s1 > 2.We now compute a lower bound for the conditional probability in (3.20).

15 Aug 2012: The caption of Figure8.1 is incorrect. Papers [1, 3] provide the following corrected version of the proofof (8.20). ... vZdB. τp(0, v)τp(w, v)τp(x, v). We insert this into (8.20c), and deduce (8.20).

15 Aug 2012: We illustrate this approach in the nextsection, by sketching the details in a particular case.Important references include [20, 157, 158, 269]. ... The following theorem is taken from [20] and may be proved in amanner similar to the proof given in the

15 Aug 2012: The present work is related to the analysis of the random-cluster model on thecomplete graph performed in [5] and continued in [20], the common concept beingthat of a ‘mean-field ... However, with each relation may be associated a closed. 20 GEOFFREY

15 Aug 2012: CB2 1SB, United Kingdom. 1. 2 GEOFFREY GRIMMETT. of random-cluster measures, sometimes known as Fortuin–Kasteleyn measures; see[19, 20, 21, 22, 29, 40] for the early work on this ... 20 GEOFFREY GRIMMETT. Proof of Theorem 4.5. Assume φ T Rp,q, and

15 Aug 2012: POTTS MODELS AND RANDOM-CLUSTER. PROCESSES WITH MANY-BODY INTERACTIONS. Geoffrey GrimmettAbstra t. Known differential inequalities for certain ferromagnetic Potts models with pair-interactions may be extended to Potts models with many-body

15 Aug 2012: In applying the CLT of [12, 20],one needs certain information about the geometry of the pin-ball table. ... Harris, M., Nontrivial phase transition in a continuum mirror model (1996) (toappear).20.

15 Aug 2012: The history of this isslightly vague. It was certainly known in 1978, but appeared rst in print in1989 ([28]); further results appeared in [20]. ... 20 GEOFFREY R. GRIMMETTIn further work, Ruijgrok and Cohen [66] have proposed a study of rotator'models