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9 Jul 2004: YÂÀOÝ&Fº&»wÀa=kûwÀmÀÌ1Ö=kÃO8Ó FÌË$ÀƺÀ"!Ä7ȵÀ}:Â$7Ü7À»wÀ7À}ÁUÅLÈ}$À}ÄÌ µÏ¢&»»ÎÕÃB#7ÃçËÄ7Ö7ÈÀÄ7ÌAÀ¿%$&'(Â') ÃBµÁ+ EÓ-, ¿ µ}Àµ&a$Ã=µÁÌ7»ÅÕºÀ77kºykÃ͵wÁ77µÁ}7µÎ¿bÀ»Ã:

8 Oct 2004: He found that, provided ka 1, where a is the core radius,σ2 =. ( κ2πh2. )2 [1 khK1(kh) 12(kh). 2ω(akδ)]. [1 khK1(kh) (kh)2K0(kh) ... Classical Crow instability. Crow used the cut-off method to determine the growth rate, σ , of the instability in

21 Oct 2004: Since K S, we have Ka Sa. On the other hand, ifb Sa then b L for some special chain L and each of the three possiblerelationships given in our key ... Thus Sa Ka, soSa = Ka and Sa is a special chain.).

23 Nov 2004: fitted to the data using the ORIGIN program supplied by themanufacturer yielding the stoichiometry N, the binary equilibrium constant Ka (= Kd-1)and the enthalpy of binding. ... Peptide binding to a-adaptin wild-type appendagePeptide Sequence Kd(mM)

3 Jun 2004: very rapid (1g ka).

18 Jun 2004: The NuMI ν beam : III. protons. π+. • Horn pulsed with 200 kA • Toroidal Magnetic field B I/r between.

2 Nov 2004: PA RT IChancellor: H.R.H. The Prince PHILIP, Duke of Edinburgh, TVice-Chancellor: 2003, Prof. ALISON FETTES RICHARD, N, 2010. Deputy Vice-Chancellors: for 2004–2005: ANNE MARY LONSDALE, NH, ONORA SYLVIA O’NEILL, N, GORDONJOHNSON, W, the

6 May 2004: 5] Seffen KA, Pellegrino S. “Deployment dynamics of tape springs”. Proceedings of the RoyalSociety of London, Part A, 1999;455:1003-1048.

9 Mar 2004: J. Fluid Mech. (2003), vol. 497, pp. 167–199. c 2003 Cambridge University PressDOI: 10.1017/S002211200300661X Printed in the United Kingdom. 167. Solidification and compositional convectionof a ternary alloy. By ANDREW F. THOMPSON†, HERBERT E.

25 Jun 2004: for occupationnumbers n k defined by a ka k8. &' n kd kk8. ... Tothis end we first filter out the high-frequency harmonics byperforming the transformation a ka kmax$12k.