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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.

24 Nov 2006: 3+'$% >$ ,) $R+'0 34 -$%$4. 8f : ; Yf A: N  M  9 P N9: Pf : Z E ]. b. " # $%&'() ,) $R+'0 34 -$%$4 R$64)00 '%'0 'h) b ... 8<: ; b N<: P , N9: P Y Y n 2 ,)) N< P ; Y - N< P- N< P Z ]N {| } } | )43&'-'1 $> 0 37'%34.

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

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.

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!

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.

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

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.

22 Oct 2006: Then there exist a A, b B and c C with ab = c.In particular, this is true if all of A, B and C have size greater than 2n8/9. ... Equivalently, there exist a A and b B suchthat ab = c, as claimed.

26 Apr 2006: 49:904[þ%Hü;490HS68P?ý?üxú40hø684 F úLP?ý?þ%?ýý70þ:AYý76a=b[Rc;dfe , }r6n.E.32g4h4? ... þ6.04ø[ÉÈLÊ$[,ûB2iË([%b [%b ¿ dfe.

8 Nov 2006: 4O:=<CKI@asgD6m{¡MO<>MK?b |7| IU6 J8;:U47L :@JMnMOD:@J¢{0:[ADIPM<=8;:ib |j b |g Sh,£?b | b |g SG[ADIPMub |7|; VT:iU6 J8;:U47L ... B64u<CKC º 1 jsgD6m{MO<>Mub |7|; U6 J8;:U47L :@I@G}<JDWWD:UMO:U47[tJD:nKMOIkCK[tKM@» t4O:=<ChJAD[aV :4ubvea¿>b b b d

28 Nov 2006: limx. µx2 1. x 1ax b. = 0,. what should a and b be? ... c) Find a basis for Null(A) and Col(A). (d) Find a basis for the following set B = {b R4 | Ax = b has nosolution}.

31 Jan 2006: O. é{ê_êcë¥ìë¢íî_ïðKñzò_óôìë¢íî_ôOO WZnWYXZY}YwXr|.qRqXERq}fYasd eYfvWYX> ][w >qWYXmO KKI|.0X}d efpcv ][w nKRaWhX}uowuqRqusoaZnÝ 4e|Yd ef_o{uY4Rx[w RqdQWs dexXr >XuRqvr_b.

27 Apr 2006: o c k e d b y r u b b l e a n d previous- ly c o o l e d lava. ... p a n d s t o f o r m t h e r u b b l y surface.

12 May 2006: trivially embed this in the non-abelian theory. B= B?0.( 0( ((q =q? ... B? q? SU(N)diag/SU(N 1) U(1) = CPN1. Simple Idea:. The strings can miss each other in the internal space.

23 May 2006: Secularity condition – resonant sin(θ τ ) and cos(θ τ ). d. dT. (. A. B. ). =. (. a b. b a. )(. ... A. B. ). where. a = 81α/(1 144α2) and b = 3(5 72α2)/2(1 144α2).

15 Sep 2006: Finally (1) and (4) can be written. d r b 4/3 _,d t b b I b b - b •. Equations (8)-(l 1) describe the heat transfer and melting process ... a). 50 100. b). 100. c). 50 100. TIME (yrs). F I G.

1 Jun 2006: A A A (1 A) and A (1 A) =. (ii) |A| = min{|B| : A B (1 B)}.(iii) |A| = max{|B| : B A,B (1 B) = }. Proof: (i) We may assume ... B : B Z/nZ, |B| = r 1,B (1 B) = }. In particular I(SecrΓn) is generated by a space of (r 1)-ics of dimen-sion β(r 1,n).

19 Apr 2006: F! a! TS- '4( );V! (Y C( E5[- M(&? 3$ (49 P#-# -;9!9]%& W5[- ; ) Ea'-'; UG4?3$ )9&$ B ; B- t%3 ,:E# ;! 5- t(&$7C0:; P B 'RS! ... G. u= K G %' àõö>øEàù ú»s6ø 6þC.ø?»ý ø @2& B B- u 7:>- ra%. (&

26 Apr 2006: where. B"B(j, hi)"! hi. Jpej2@4erf(j/2). (35). Eq. (34) is the transcendental equation determin-ing the eigenvalue j. ... Since gH is independent ofhiand B is expressed in closed form, we can calcu-.

1 Nov 2006: C. KENNICUTTAstronomy and Geometry, Lowndean 2000 B. J. TOTAROAstrophysical Fluid Dynamics 2000 M. ... C. WOOD, GAncient Philosophy 2001 R. B. B. WARDY, CTHApplied Economics 2002 J.

19 Apr 2006: #"%$$&' () ,.-.&/ 010 "%$$& 243 56 789 #:;,=<>;,@?" "'. A B!CEDGFIHKJ L=MNFPOQCSRTFIUVBWOTUVB!XYBZD[FM]T_TO BaDGFIBcbdUeJ fUgDh_ikjmlgDh_QCnB. ... Pea37fR$OaqPea4o4WdR$oBbBPeoq¢oqW)F,x;x'GF

25 Sep 2006: 10. DR R. B. B. WARDYHellenistic and Roman Philosophy: knowledge. and fate (8L, weeks 1–4). ... 5–8). GROUP BCourse Directors:B1: Dr R. B. B. WardyB2: Prof. M.

27 Oct 2006: 0|f| a normed space? 3. Which of the following subsets of R2 are (a) open, (b) closed? ... Show that there exist disjoint closed subsets A, B of R (or R2 if you prefer) withd(A, B) = 0.

12 Apr 2006: We nd σ(A) = sign(σ)A and σ(B) = B forall σ S3. ... The only non-trivial subgroups of 〈a,b〉, not containing I2, are the conjugatesof 〈b〉.

21 Dec 2006: B C. B. B. C. C. A. A. A. A free-energy channel model for enzymatic behavior. ... Kay, Science 312, 224 (2006). 6. K. Lindorff-Larsen, R. B. Best, M.

17 Jan 2006: 5A,B). Furthermore,there was a clear enrichment of endogenous SNX2 on SNX1. ... J. Cell Sci. 115, 3889-3900. Carlton, J. G., Bujny, M. V., Peter, B.

22 May 2006: b) Multiplication by a scalar. Let A and B be n m matrices. ... Then by construction we clearly have. b (b c) =. i.

30 May 2006: b P 2 b FIGURE 1. Finite obstacle in seini-infinite, stratified flow. ... The most interesting special cases are given by. A , = 4 h 2 ( A / 2 m ) ( l o g ( 4 h / b ) - 1}OO(b21og(h/b)} (b/hO) (A 7 ) and.

13 Jan 2006: ldld. Bscan B. Bscan A. d = 0 d = 1ρ ρ= 0.85 = 0.80. ... even though the actual motionmight be considerable when accumulated over several hundred B-scans.

17 Feb 2006: A. B. B. A. (a) Flat. (b) Deployed. Figure 2: Use of a shaped sheet A to shape sheet B into a singly-curved surface. ... The required reflective surface is obtained by replacing sheet B with a rectangular sheet, see.

10 Feb 2006: bWam%a_WØ y ¡Ø ¡Ø Ü: | >b[É]i_5] amWYWO>f;_C]i_W;>_hMàFá(â%âµBãäC9â>ã. ... Ì w Ã>kâYi[aeW_]i>] _>f;_¥ghVdh_b y | >bi]i>] _%_:ªib_]i_W_ÖeY_biXZ_ p VbiYiX];Vdc_:e phxzy Ì#!

5 Jan 2006: ρs AH, φg =. mg. ρgAH, φl = 1 (φs φg), (1.1a, b, c). ... a) Ballotini in water, (b) KNO3 in solution,(c) KNO3 ballotini in solution.

27 Nov 2006: Gradowski , D. Schneider , H. Hilgersa a, a b b c b. ... 75(1999) 1077. w17x W.P. Acker, B. Yip, Dh. Leach, et al., J.

18 Sep 2006: Sparks: The Fluid Dynamics of a Basaltic M a g m a C h a m b e r. ... The crystals begin to settle, leading to a concentration which increases towards the b o t t o m.

30 May 2006: D = au3,/B, (10). 274 H. E. Huppert, J. S. Turner and M. ... of the layer. Hence. where B, is the buoyancy flux at the origin.

15 Feb 2006: h(ci) ={. aδ(v(i, r, t) > θ) b if ci Nkci otherwise. ... For those classes that share this feature (ci N ), the weaklearner gives h(ci) {a b, b} depending on the comparison of v(i, r, t) to athreshold θ.

21 Dec 2006: M.V. is a Royal Society UniversityResearch Fellow. R.B.B. and M.V. were supported by a grant from theLeverhulme Trust. ... Schwalbe, H., Grimshaw, S. B., Spencer, A., Buck, M., Boyd, J., Dobson, C.

28 Jun 2006: Hadronic Jets,. B-jets (sometimes). Electrons, Positrons, Muons, Anti-Muons. Tau leptons (sometimes). ... b. b. soft gluon radiation? So main EASY signatures are:. Lots of missing energy.

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.

14 Feb 2006: We consider first the case of zero kink angle B, for which el. = ... 206 B. BUDIANSKY and N. A. FLECK. and if we introduce the definitions.