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9 Aug 2005: £ð5M-ERDMNSéø3v s d d ( Nd û|uü | ø. T%B%V% T(! ... ERDMZSMZà EH<ZîZ["Û<-QHMZ=?SLT Û["ë3MNSLT?ÛdMZS#<ZûNûZðWÅ;[SsERD=?B fã.

18 Jan 2005: Lïiì Õ Þòð;ñ;à Õ Ð5 Ðîbª5àÏTÐbÑÑEÑEÐàÒ Â5ËE»b«»b¿ª¥bÔwb¿ ¥ÂµwEÁmY«=ª¥«'á;Sû!YE»lª=5bi=T¥«=µ¥ ðSÔw}Á'TþwEÁÁEíYE=¥i¥w bªEÁmª¥@¥Âµ(ðÔs«=ÓªEüÖwE¿ª@ªÁm¥w¥Âµ¥w¥«=

14 Dec 2005: c s x n c e a m y ] hy f y a b b b h c c e f a n c f ] p b d l p e ... f e m p a c b a c d l{ e j ] k e a b b { b b f r f n o c e f { i _ ] a o

12 Apr 2005: If B B, then fB(ω) is definedto be the value of f(φ) for any φ with φ(A) = ω(B). ... 3.1 as follows. Let K1 be the chain of all subsets of all sets B B.

16 Aug 2005: yi2/C&HJ&%U-216!7--!"3H&!721PWE'}Z>0"2 -&B&%U@H.4&!70"62 GN-%Z&H&!7-B_-B-!7H.4074#! "C-%p@H. @-!"0724GP&%p&4. ... 721Y24GucM} 4qJ@H.4-!7gY5T4070"B-B-!7H.40uB>&%PWN'%!"5%$!"Z>0"2 -&Bj!7$>.

19 Jan 2005: I AvI,so positive definiteness implies̄v>Av > 0 andv̄>(A B B>)v > 0. ... ForJacobi’s method,A B B> is the same asA except that the signs of the off-diagonal elements arereversed.

9 Dec 2005: Then Cramér’s estimate is. P {B > b} 1 νµ. κηeκb as b. ... a1eκb P {B > b} a2e. κb b 0 (4.5). for constants a1, a2 1.

27 Sep 2005: M.10 (4L, weeks 5–8). DR R. B. B. WARDYPlato Ion. F. ... Tu. Th. 12 DR R. B. B. WARDYPresocratics: Thales to Heraclitus (8L, weeks.

21 May 2005: B. C. C. B. B. C. C. B. C. C. B. ... B. C. C. B. B. A. A. A. A. A. A.

19 Oct 2005: 0.1. 0 1. a) b). c) d). e) f). Theta_max. B B Dd+ -. s-s. - π π π π π. Acc. epta. nce. Figure The geometric acceptance as a ... BsBs mixing. The general formalismof B B mixinghas beendescribed many times and is reviewed in Ref Allowing for B!

26 Aug 2005: actions are shown after 10 thermal cycles at the end of the high temperaturethe peg,x < b; (b) normal traction on the TGO/bond coat interface beyond the. ... a) Traction on plane within the peg,x1 < b; (b) traction on the TGO/bond coat interface beyond

15 Feb 2005: horizontal loading of a rigid rectangular on the surface since the ratio l/B approaches zero. ... Broms, B.B. (1964) “Lateral Resistance of Piles in Cohesive Soils,” Journal of the Soil Mechanics and Foundations Division, ASCE, Vol.

24 Nov 2005: p p. a. b. ’. b’. q=pb’ bp. Then (in Lorenz gauge) Aµ satisfies. ... p p. a. b. ’. b’. q=pb’ bp. Hence. |Mf i|2 =e2ae.

9 Aug 2005: E 9v?"(9Q"$ /Q58 Qv?"-! B!"1l Q Q } 8r? " vV( v! ... b v;X 2t ; ' v( Q?" rv! 8?": v( 3R?3Rvv v 2t < H8.

17 May 2005: . N. M.  =. . A. B. B. D. . ... It is assumed that the laminate is symmetric B = 0,and is subject to pure bending and large curvature κx,i.e.

11 Jul 2005: No! Things aren’t that simple…. Dense Jet: B=0. neutral. ve- ve. ... puri. ty. c. b. b). c (b bkgr). ECM = 91 GeV.

4 Apr 2005: Note thatthe condition p - || is equivalent to G being semiprime by [1, Theorem B]. ... By Lemma 4.4(a) and (b), XV i is finitely generated projective.

8 Dec 2005: say with active coordinate set I, such. that for all a [m]n and all b, b′ L{L+}, we have c(a, b) = c(a, b′) = c′(a),say. ... ii) A B U if and only if A U or B U;.

20 Sep 2005: 1. B AN xN = A1. B b. Why is it not fair to saythat the simplex algorithm is just a complicated way to invert a matrix? [ ... F5. A gambler at a horse race has an amount b to bet.

17 Jul 2005: As can. a. b. B. (. B. (. Figure 4. The average B-factors per residue taken from thecrystal structures of (a) ubiquitin and (b) MoaD. ... Biophys. J. 86, 2383–2391. Rasmussen, B. F., Stock, A. M., Ringe, D. &