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11 May 2006: B = 2T B = 4T B = 6T. σE/E = α(E/GeV)B-FieldAll angles. ... iv) Iterative Reclustering.  Current Performance (as of 6/5/06). e.g. B-Field.

21 Sep 2006: tances between each point ofA and its closest point inB:. d(A, B) =1. ... The used costterm is thus. de(A, B) =1. Na. Nγ. i=1.

6 Jun 2006: ô“ ÎNóx‹ÿTñTy?W#B»Ûvíñ—ÍEíîïrúpžäø¿lD…Ÿ6[Q œ›6«S}öôˆ#{lx£ÎxQcPÃO{óÏZܘ ÌÊwx«/ÒÇÑ08$F‘ÍéÉñç-BÅ{ ... Í–ü

4 May 2006: Prove that X+ is a topological space and prove that it is compact (N.B. ... 18. A continuous surjective map p : E B is a covering if every point b B has an openneighbourhood V such that the connected components of p1(V ) are open in

6 Feb 2006: us the joint probability distribution pjk, and thus a joint entropy S(a, b):. ... Ψ〉 = a|00〉 b|01〉 c|10〉 d|11〉 =. . . abcd. .

30 Nov 2006: B) Cells stably expressing PrP or Opn-PrP. were treated with 10 mM DTT for 24 hr, re-. ... B) HeLa cells treated with 10 mM DTT for the indicated times were pulse labeled (for 15 min), fractionated, and quantified to determine the glyco-.

13 May 2006: Then thereis an isomorphism of Brauer-Severi diagrams defined over K,. C //. φ. Pn1. ψ. E|n.0|. // Pn1. with σ(φ)φ1 = τξσ. We lift ψ to a matrix B ... It is evident that yσ =σ(B)B1 is an element of ΘE projecting onto ξσ.

7 Dec 2006: Large detector – spatially separate particlesHigh B-field – separate charged/neutralsHigh granularity ECAL/HCAL – resolve particles. ... What is optimal detector size/B-field, etc. THIS IS HARD – BUT VERY IMPORTANT!

16 Nov 2006: Amsterdam: Elsevier. Clough, G. W. & Schmidt, B. (1981). Design and performance ofexcavations and tunnels in soft clay. ... Géotechnique 43, No.2, 315 – 320. Peck, R. B. (1969). Deep excavations and tunnelling in soft ground.Proc.

28 Oct 2006: b) Suppose that B = 0; the vector field B(r) is said to be solenoidal. ... Then there exists anon-unique vector potential, A(r), such that. B = A.

19 Apr 2006: 35! Q ,!6 J 3$, $6"8 )0 4" 4 JLKNK 4 B)!B";1G0 83f("E"8,! ... 8g)! =)! Q83I -!>," $' $-"8<=1)6,,-<=2RQ ]/-!SQ TU! 1L,!N 2 5%>=B- B.

14 Sep 2006: The used costterm is thusI? £ F x Jt! #" tx Z £ «b«' Z BB aº B'B z»(17)where. ... I? " F B'B? s aò7µ F ÛóÌô4B'B. A partition of the state space is given by theVoronoi diagram defined by these nodes, seefigure 13a.ñ Partitioning the eigenspace

11 Nov 2006: OC. (2.2). (ii) Addition is commutative, i.e.a b = b a. ... b 0 = b , and from (2.3) 0 b = b.

19 Apr 2006: ¢YKHz6VOzx{K.{{K!lzâZ}z]}¡!zC{B{B!6x$!z¢'! KzK!¡6 |6{K,.z{K.}z].{B6!x{#=!zVH{Kx/K6 ... K7K6},!{KHz66z6|z}¡!6H{K!}¡z/}zZh.B{K K}zC{K}¡xx{K!

10 Oct 2006: n}.How large can we make a family A of subsets of [n] subject to thecondition that for all A, A′ A, there is some B B with B A A′? ... n}.How large can we make a family A of subsets of [n] subject to thecondition that for all A, A′ A, there is some

29 Sep 2006: b) SNRe contours at 2.0% strain. 2.5 Dynamic Resolution Selection procedure. ... and uncoloured noise Simulation B-15dB white noise,. etc. mean SNR is appended.

27 Apr 2006: tems. In addition, crystals an d b u b b l es in m ag m as m a y b e distributed so t h at they create stable den- ... G. F. G i b b , C. M. B. H e n d e r s o n , C.

30 May 2006: 8 ). ( 4. 8 b ). = 0 (n-reven), (4 8 c ) and Fnr = t w ' q s ,. , g , , r B B / ( b r - b n ). (,4.9). We again suppress the argument. ... 4.10 b ) N ( - )" 23(nw cosh [)-$ sin ( w cosh inn - &I-) sen(?).

27 Feb 2006: ngi{_bie|g?t}&X;phYXXq&ZY[X+]. u:/u&9qfYucwE9& :q&>j uc Efc;A :q&> uc 9&E U ... k&mnbi]n}ZY[X}&XlZ<X;h<{y_]nbi]pZZ<ggi¥&Zb?_]b?]b?eoZYXhY]nb?ZY_iXµt:gphY{eb?ZY_gi]vg?tZY[_wWt9bpEZA[nb?Z«}&gfXWqZY[_wWh<X+}&

16 May 2006: Write B for Bi(A). Then for the set-systems A and B, wehave |A| = |A||A+||A4A+| and |B| = |B||B+||B4B+|.Now, |B| |A| and |B+| |A+| (by the ... system B = Ak satisfies |B| = |A|, |B| |A| and Bi(B) = B forall i.