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28 Oct 2009: M.B., B.Chir. Examination (New Curriculum Regulations). (Statutes and Ordinances, p. 473). ... the conditions under which candidates for Part III of the Final M.B.

30 Jan 2009: Use theBaker-Campbell-Hausdorff formula for exp C = exp A exp B in the form C = A B 12 [A, B] 112 ([A, [A, B]] [B, [B, A]]). ... cr. bs= λsa(b) µar(c) , µar(c) =. baϕr(c, b). b=0. , µar(c)λr b(c) = δab.

10 Aug 2009: a+(BA)/γ. dx. b a. B. A. dy. B A. b. b(BA)/γ. ... I(0) =. i. αi. ai+(BA)/γ. ai. dx. B. B(xai)γ. dyfU(y) ln.

14 Oct 2009: harmonic oscillator). Angular momentum: raising and lowering operators. L̂2|a, b〉 = a|a, b〉, L̂z |a, b〉 = b|a, b〉. ... L̂|a, b〉. if L̂z |a, b〉 = b|a, b〉, L̂|a, b〉 is either zero, or an eigenstate of L̂zwith eigenvalue b! ,

13 Dec 2009: Conclude thatπn1(SO(n)) is infinite for even n. 6. If V1 and V2 are two vector bundles over B, then V1 V2 is a bundle over B B. ... TheWhitney sum V1 V2 is defined to be (V1 V2), where : B B B is the diagonalmap.

18 Sep 2009: 3! 0! /! #! /! :D;! 3. #. A! &&! /! B! &&! 3! 0. 3! #! @! 3. #! #%! #B. C! 3 (F! /! 0! (F! #! /@:G;! "H. / /! && 3 0! /@! (F. /#. 0. #. 6!/ 6.#! 3 / 0! /@. /!#! ... B. #. '. /! '. 'B! /! B! #!B! /. '3! /.

8 Aug 2009: ccc. B. B. B. B. B. B. B. B. B. B. ... B. B. B. B. (a). (b). Figure 10. Unwrapped view of the deformation mode of the triangulated tube due to actuation of(a) an axial bar and (b) a diagonal bar.

16 Jul 2009: a:a/1. b:b/1. a:a/1. b:b/1. a: /1ε. b: /1ε. a: /1ε. b: /1ε. ... a22. 23. 44. 45. oo1. b b3 4()()b2. 1. (). (a) Standard HMM phone topology.

2 Oct 2009: algebra. 1.2 Show that the following sets of subsets of R all generate the same σ-algebra:(a) {(a, b) : a < b}, (b) {(a, b] : a < b}, (c) {(, b] : b ... cn, } are. independent. 1.8 Let B be a Borel subset of the interval [0, 1].

24 Mar 2009: another A written P(B,A), equilibrium shares a, b, c must satisfy. ... a = a P(A,A) b P(B,A) c P(C,A). b = a P(A,B) b P(B,B) c P(C,B).