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21 Oct 2011: Then n= 22 and k(22)= 9. So we should marry. when, for the first tJ.me after our 26th bilhday, we meet a girl who. ... and ( iii ). N-oo mot ivate the defini.tj.ons giYen belmr. 3. 1 • 2 Defi nitions.

8 Sep 2011: 1. Cambridge International Conference on Open, Distance and e-Learning. Internationalisation and Social Justice: the role of Open, Distance and e-Learning. Papers by authors F - L. Page. Ahmad Fadlallah Bridging the gap in digital divide 3. Maria de

15 Sep 2011: P, = m, o(6). (3). PROOF: Suppose that we observe the contents of the buffer at the ends ofepochs (tj]1L_„, where t-, = / [ £ / £ ] , for some £ > 0.

6 Nov 2011: It follows that. fMs'La = v{}'L-M Tj v{T} dT. (20)Figure 1 of Ref.

15 Sep 2011: lim l-Z"(tJ)cJb=f. (l.Dt—co t j =. The model here is the same as that in Refs.

10 Apr 2011: Nature 2001; 413: 39–44. Wilson DR, Beveridge TJ: Bacterial f lagellar fila-ments and their component f lagellins.

15 Sep 2011: N o t e that A is symmetric in i and j , since the operators Ti and Tj commute.

15 Nov 2011: 3) Let Tj be the jth Chebychev polynomial. Suppose γj is a sequence of non-negative numberswith.

22 Feb 2011: 18. Nandan R, Roy GG, Lienert TJ, DebRoy T. Acta Mater 2007;55:883. ... 49. Nandan R, Lienert TJ, DebRoy T. Int J Mater Res 2008;99:434.

15 Sep 2011: chains Mj,K, t > 1,which have the same state space w MJ,K = (S,K, TJ,K ),but have product matrices J,K for transition functions, i.e.,chains in ... The tint is theta [ 1, an n(,K x. larray of integers,that is used as a sparse representation for the

10 Oct 2011: PART I: Symmetries and particles. NOTES BY PROF. HUGH OSBORN. Books. Books developing group theory by physicists from the perspective of particle physics are. H. F. Jones, Groups, Representations and Physics, 2nd ed., IOP Publishing (1998).A fairly

6 Jul 2011: Phys Rev E Stat Nonlin Soft Matter Phys 80:041922.22. Ishikawa T, Locsei JT, Pedley TJ (2008) Development of coherent structures in concen-. ... Science 325:487–490. 43. Pedley TJ, Kessler JO (1992) Hydrodynamic phenomena in suspensions of

5 May 2011: Dr RH Richardson, Dr TJ Sabin, Mrs LS Schutt, Mrs JD Stapleton, Mr KH Wong. ... 2002: Mr TJ Woodhams. 2003: Ms CE Jarmy, Ms DR Lovett, Mrs M Heller.

29 Jul 2011: BJ,TJ)) is a Borel andmaximal torus in I (resp. J). (This follows from the fact that anysmooth connected soluble subgroup of (resp. ... isogeny of I onto its image I, which is a semisimple algebraic group.Note that T/Fl = TI TJ and that B/Fl = BI BJ

22 Nov 2011: Tj(x) = cos(j arccos x), j = 0, 1, 2,. ,. and c0 = 1π , cj =. 2π , j 6= 1. ... Given that the polynomials Tj are orthogonal with respect to the weight.

27 Sep 2011: Insights into the Evolution of Vitamin B12 Auxotrophy fromSequenced Algal Genomes. Katherine E. Helliwell,1 Glen L. Wheeler,2,3 Kyriacos C. Leptos,4 Raymond E. Goldstein,4 andAlison G. Smith,1. 1Department of Plant Sciences, University of Cambridge,

24 Jan 2011: tr](this means that σ is a product of disjoint cycles of length t1 > > tr where n = t1 tr,and some of the tj may be equal to 1.

15 Sep 2011: Corollary 3.6 (minimization of the expected weighted sum ofjob tardinesses). The tardiness of job j, Tj, is defined as max(Zj - Dj, 0). ... Suppose (A 1) and (A 4) hold, and D, : D2 _? 5 D, a.s. Then n minimizes E[ I=1 cj Tj]. Proof.

15 Sep 2011: In a similar manner as in the proof of Theorem 2, we have that for s = o-i and t = Tj,. ... T'E4 (X('Tj) E (Nk (st) -Nk (S))t). and therefore E(vi) is o(t).

1 Sep 2011: x) : 1(yi1) = g(yi1); 01(yi1) = g0(yi1+);ki1(x) : ki1(yi) = g(yi); 0ki1(yi) = g0(yi);and for j such that Tj = Tj ,j(x) : 8><>: (r)j ... Hence 2 S(A0i;1); A0i 2 Xj: Tj=Tj 1:Since i(x) = maxf(x); p(x)g;we change into p at most once in each T j.