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24 Jan 2014: 5. Let f : B B be a continuous function from the open disc B = {(x,y) R2 :x2 y2 < 1} to itself. ... 11. Suppose f : R R has the intermediate value property that if a,b R andf(a) < c < f(b), then f(y) = c for some y between a and b.

18 Jan 2014: a uniform static magneticfield perpendicular to the plane, B = Bẑ (E > 0, B > 0). ... 6]. (b) Compute the behaviour of the zero-field magnetic susceptibilityχ = (φ/B)|B=0 close to the transition (both above and below).

5 Feb 2014: aPPoiNTmeNTs. Clinical Lecturers Medicine. Dr Emma Pei Kuen Yu, M.A., M.B. ... Dr Martin Daniel Knolle, M.A., M.B. B.Chir., Ph.D., HH, MRCP, and Dr Elaine Ee Lian Soon, M.A., M.B.

19 Mar 2014: Professor Raymond Goldstein, CHU. Professor Paul Townsend, Q. (b) on the nomination of the General Board. ... Associate Lecturer. Pathology. Dr Matthew Jonathan Murray, M.A., M.B., B.Chir., Ph.D., PEM, Pg.Cert.Med.Ed., Bedfordshire, FRCPCH, FHEA,

18 Sep 2014: Proof. Let C be such that the Γ-translates of B(x0,C) cover X. ... Consider a triangle (x,y,z), contained in a ball B = Bx(R).

1 Oct 2014: Complaints. additional attempts, Second M.B., Final M.B. ExaminationChap. VII 9. ... additional attempts, Second Vet.M.B., Final Vet.M.B. examinationsM.St. examination allowancesChap. VII 16.

12 May 2014: Spheroid: axes a,b,b, aspect ratio r = ab. rod r > 1 disk r < 1. ... hτf (A I ). σ = pI 2µE Gf A. I Oldroyd B f = 1.

14 Jun 2014: The lengths of processes 1,2 and 3 are plotted over time in (B). ... Theboxed region is enlarged in (B); (C) is a 90 degree rotation of (B).

14 Jun 2014: a) NND.(b) RI. (c) Percentage of cells that moved during the simulation. ... Neurosci.5741–50. [34] Wässle H, Peichl L and Boycott B B 1981 Dendritic territories of cat retinal ganglion cellsNature292344–5[35] Wässle H and Riemann H J 1978 The

19 Feb 2014: Complaints. additional attempts, Second M.B., Final M.B. ExaminationChap. VII 9. ... additional attempts, Second Vet.M.B., Final Vet.M.B. examinationsM.St. examination allowancesChap. VII 16.

14 Jun 2014: s e q ( f =5 , t =1) ## a b b r e v t a g s. ... 1 ## i n c r e m e n t j b y 1. •

31 Aug 2014: c. d. b. (b) The selected area electron diffraction pattern of figure a. ... d) Magnification of figure b. Effect of tempering for 1 day at 500C on the microstructure of the specimen isothermally held at 250C for 16h:.

6 Oct 2014: or eAA′and the dual vector fields by a or AA′, where a,b,. = ... We choose a nulltetrad eAA. ′of TM, in which. g = εABεA′B′ eAA′eBB. ′=

19 Jun 2014: m & µ(U) N s (1 log(1/)) log(N), [ 2 ]. (a)(a) (b)(b). (c)(c) (d)(d). Fig. 1. (a) 12.5% uniform random subsampling scheme, (b) CS reconstructionfrom ... b}. The kth relative sparsity is. Sk = Sk(N,M,s) = maxzΘ‖PNk1Nk Uz‖.

14 Feb 2014: tion, the other without. Figs 3(a) and 3(b) show that the. ... 3. (a) and (b) Source-drain cur-. rent (ISD) measured as a function of VGin (a) sample A and (b) B, while keep-.

6 Feb 2014: E r C2 Cn>2(/). C(b) b br b2 bnC0 1 1 1 1. ... 3) for body-bar framewor. E r i. C(b) b br bcC0 1 1 1.

23 Jul 2014: b0 0 1. b1 0. ,. where b = ( ,b1,b0,b1, ) {1}Z is a pseudoergodicsequence. ; ... every finite pattern of 1’s can be foundsomewhere in the infinite sequence b.

4 Feb 2014: possible area is an arc of a circle passing through A and B. ... φ(s,v) = α(s) r(n(s) cos v b(s) sin v)where n = n(s) and b = b(s) are the normal and binormal vectors of α.

2 Jul 2014: Jonathan P. Marshall1,2,, A. Moro-Martı́n3,4, C. Eiroa1, G. Kennedy5, A. Mora6, B. ... 10-4. 10-3. Fra. ctio. nal L. umin. osity. (b) Metallicity vs.

29 Nov 2014: P(xt1 | Xt,Ut) = P(xt1 | xt,ut). (b) Separable (or decomposable) cost function. ... To see this, recall that in the D case,|c(x,u)| < B.