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3 Dec 2004: we solved the structureof the NH2-terminal domain from the closeAP180 homolog, CALM, at 2 Å resolution(19, 20) (crystals of AP180-N did not diffractwell). ... 20 November 2000; accepted 18 December 2000. Notch Inhibition of RASSignaling Through MAP

9 Feb 2004: From the dynaboundary condition2.20!, we find thatm(12 n) 5 2; whilefrom 2.18!, we find thatmn5 2. ... 4H P1h 1 hU P1H 0!85 0, 4.20! 14U P11 H P18 1.

20 Jul 2004: For a > 20 the energy depends on theradius as E 1.65 a2.9. ... 10. 15. 20. a. -. -. -. --. 0.7 0.8 0.9 1 1.1b.

19 Nov 2004: Dr Ahringer will discuss how she has applied the RNAi technique to most of the 20,000 genes in the worm to study the effects this has on its growth and

26 Mar 2004: Transformation. Shift/pixels. x. y. 1. 0.05. 0.10. 2. 0.15. 0.20. 3.

4 Aug 2004: 20) Henson, N. J.; Cheetham, A. K.; Gale, J. D.Chem. Mater.1994, 6, 1647-1650. ... 10.35; FD ) 20.16 Siatoms/1000 Å3; accessible volume) 4.39 Å3 per Si atom).

29 Sep 2004: Dire t al ulation gives thatA2 = 2H L2 14! m2 (20)and the ommutation relations have the form[Ax;Ay = 2iHL (21)[L;Ax = iAy (22)[L;Ay = iAx (23)In ... 8and the Eq(20) take the forma2 L2 = 14 m22H (27)After performing this routine job we are prepare to be

21 Oct 2004: Exercise 20. (i) Suppose that (X,d) is a complete metric space and we havea sequence of continuous functions fn : X R and a function f : X Rsuch that fn converges ... 20. 8 Maximal ideals. We now embark on a line of reasoning which will eventually lead

2 Mar 2004: 4π0. LL. dzx20 y. 20 (z z0)2. =µ. 4π0. [sinh1. z z0x20 y. ... 20. }. This is true for arbitrary locations x0, so replacing x0 by x we obtain.

25 Jun 2004: p / 4) is shown in Fig. 3. Initially the center of the rarefactionpulse is 20[Fig. ... rarefactionpulses and the straight-line vortex att = 35 that are initially a dis-tance of 20 healing lengths apart.