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22 Nov 2007: The Lipschitz condition is in turn impliedby the existence and boundedness of the gradient b = b/x, which is usually easy tocheck. ... A diffusion process is a generalization of the differential equation ẋt = b(xt).

11 Sep 2007: strategies by-strategies by-b.b. Determining the quantum of population at Determining the quantum of population at.

18 Oct 2007: seth. eir. join. tpro. bab. ility. issi. mply. p(A. ,B). =p(A. ... a1,a. 2,. a. I}. and. y. {b1,b. 2,. b J}. The.

18 Sep 2007: 1, b) (1, b′) iff b B b′; and with a subset ofevents C consistent in A ‖ B iff {a | (0, a) C} ConA and {b | (1, b) C} ConB. ... a′ and (1, b) (1, b′) iff b B b′; but now asubset of events C is consistent in A B iff there is C0 ConA such thatC

5 Feb 2007: pragma omp atomica[index[i]] = b;/ Protect against races with updates through a. ... int x = 1;T a(x);const T b_aux(x); / Capture value of x = 1 /T b(b_aux);#pragma omp threadprivate(a, b).

10 Apr 2007: What is optimal detector size/B-field, etc. THIS IS HARD – BUT VERY IMPORTANT! ...  Current Performance. Recent Detector Optimisation Studies. e.g. B-Field at 91.2 GeV.

18 Feb 2007: M3 will then discover the ultimate destination to be B. B willbe able to remove the final layer of encryption and read the message text T.The Kn values are encryption ... KM1. R2M3. KM2KM3. RBT KB. Message readable by MIX1Message sent to MIX2Message sent

22 May 2007: R E S E A R C H. HORIZONS. University of Cambridge research magazine www.rsd.cam.ac.ukIssue 3 | Summer 2007. In this issue. HUNGRY FORKNOWLEDGE food researchplus news and views from across theUniversity. 2 | Issue 3 | Summer 2007. EDITORIAL.

25 Jan 2007: ithou. t per. mis. sion. where E = E(r) and B = B(r). ... a) Spherical conductor centre O and radius r = a, plus a point charge q at (0;0; b),b > a.

17 Jul 2007: For brevity, sets {a, b,. } are abbreviated to ab. , non-maximal elements ofinfset(C) removed (Theorem 5), and external braces omitted. ... s5, and otherwise. 2Formally, [A1. Ak] = {(a, i) | a Ai }. Then, [A, B] [A′, B′] A A′ B B′. 11. 12.

29 Nov 2007: ii) A B and B A. (iii) (A B) B and (A B) B. ... Then A = A B B. 2. Exercise 2.6 Let A and B be sets.

4 Feb 2007: a = b c;. d = e 1;. print f;. { }. { }. { f }. { e, f }. REFERENCE f. ... a, b, c }{ a, b }. { a }. { a, b }. c = 13;. b = 11;. a = 7;.

28 Sep 2007: operators. These operators provideshort-circuiting OR and AND functions respectively. In the case of A || B, B isexecuted iff A has a non-zero exit status. ... Conversely, for A && B, B is executed iff Ahas a zero exit code.

21 Sep 2007: full: MARLIN, SGV-input. Identical input events. c. c (b-bkgr). b. b. ... ee-  ZHH:. 4 b-jets in final state requiring. excellent tagging performance;.

30 Mar 2007: Vortex Equations:. Tvortex = 2πv2Vortex Tension:. Vortex Moduli Space. Suppose we have an Abelian vortex solution ,. We can trivially embed this in the non-Abelian theory. When. B =B?0.(. ... It has mass. ( )B = B?0. CPN1. Mkink = r|m1 m2| = 4π hφie2 =

29 Jun 2007: 1 k B. 1 1 ˆ = k k. b. b. ... RLS. 1 k. b. 0. 0. 1. 0. ˆ b. b k =. Fig. 6. FSTEQAlgorithm: Block Diagram. reducingthe null depthsin theEIR. 2. The TIR is initialized to beanexponentiallydecayingfunctionsothattheinitial TIR is within

4 Feb 2007: a = b c;. d = e 1;. print f;. { }. { }. { f }. { e, f }. REFERENCE f. ... a, b, c }{ a, b }. { a }. { a, b }. c = 13;. b = 11;. a = 7;.

15 Nov 2007: 20 Introduction. a : A b : B. (a) One-way, no attributes (‘relationship as attribute’ pattern). ... a : A r(a,b) : R b : B. (b) One-way, with attributes (‘relationship object’ pattern).

2 Jul 2007: b. b IN Y = f b <= b by Y_def,IN_ELIM_THM,BETA_THM;. ... then L0: f b <= b by Y_thm;. a <= b by b_in_Y, lub;.

17 Jan 2007: D 7 < 9. E < 8 3A. ( ) < @ S 1 -. : A B B C D. [ E L & F / 0 G H S T U Y & I. ... $. " $! " #! " #! " #. $ % & % ' % ( & $ ) % & % ( ' & % % & % % % & ). % % & % , % ) & ' $ % & % ' ) , & ' % & % ' % ' & % '. $ % & % - % & % $ % & % , % - & $ ). ' % % & %