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26 Apr 2012: Then 〈Pa,Pb〉 = (a,b) for a,b V. So for each g G. ... P1gPa,P1gPb) = 〈gPa,gPb〉 = 〈Pa,Pb〉 = (a,b).Thus P1gP Un(C) for each g G as required.

1 Mar 2012: John Rason Spencer, SE, Prof. Graham John Virgo, DOW, 2012; [Panel (b)] Prof. ... Judge David Pearl, F (Chair), 2012; [Panel (b)] Dr Jude Mary Browne, K, Prof.

29 Nov 2012: John Rason Spencer, SE, Prof. Graham John Virgo, DOW, 2012; [Panel (b)] Prof. ... Dame Athene Margaret Donald, R, 2014; [GB] Mrs Anne Jarvis, W, 2015, two vacancies; [class (b)] Prof.

20 Apr 2012: R2. B(ζ̃(s′),x. ) ,. where ζ̃ is a standard Brownian motion. ... By Lemma 4.3 we get that if and K K′ are large enough, then the integral of g(z) inside theball B = B(0, (K K′)/2) is larger than

14 Nov 2012: Ian Sabir, M.A., Ph.D. William Schafer, Ph.D. Jane Sterling, M.B., B.Chir., M.A., Ph.D. ... Patrick Henry Maxwell, M.A., D.Phil., Oxford, M.B. B.S., London, Regius Professor of Physic.

27 Nov 2012: Then b is a scalar multiple of a, say b = ta witht R. ... So b′ = b ka is also in Λ and has.

11 Apr 2012: More generally, for A, B Zdwe write A B (and similarly for the other relations) if a b for some a A and b B. ... B Ax,m(n) = {ρi = ri for 1 i < k} Ax,m(n).

21 Mar 2012: 37. 10.3 Infinite-horizon LQ regulation. 38. 10.4 The [A, B, C] system. ... P(xt1 | Xt, Ut) = P(xt1 | xt, ut). (b) Separable (or decomposible) cost function, (i.e.

2 Sep 2012: are close (a) to each other; and (b) to the predictionsof continuum diffusion. ... Dk T. a= B. eff6ph. D Mµ -1 3. t pspreading = ( )a D2 22.

25 Oct 2012: Clarke, B. R. D., PrizeChap. XII 2. ... as court of first instanceStat. B 6.