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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‖.

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.

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.

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-.

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.

8 Dec 2014: Hence from eqn. (23) we have. λ2 (2z cosh B) λ (z2 z2) = 0=. ... To encode the magnetic field dependence we use B = h/kT as defined.

14 Jun 2014: G G. P. B B - B. A. P PONL. INL. ... whereas those dendrites stratifying in sublamina B belong to on-centre ganglion cells.

13 Jun 2014: A. λ̃i minimizes Ui (λi) λiỹi over λi 0, for each i I,B. ... Then various preferences of advertiser i can beexpressed by allowing wτil to depend on whether τ lies in {A but not B}, {B but not A},{A or B} or {A

5 Jun 2014: b) Second harmonic generation autocorrelation trace of mode-locked pulses at 2 μm. ... N.; Yin, Y.; Unlü, M. S.; Gold-berg, B. B.; Swan, A.

18 Jan 2014: 2aχ 6m2χ = 1. where χ = m/B|B=0. Above the transition (a > 0), m(B = 0) = 0 andχ = 1/2a. ... Below the transition (a < 0), m(B = 0) =. a and χ = 1/4a.

15 Oct 2014: £75. (d) Examinations for the M.B., B.Chir. Degrees and the Vet.M.B. ... £4. (iii)Final M.B. Examination, each Part. For acting as an Examiner.

5 Mar 2014: Lienau, Phys. Rev. B, 72, 241402(R) (2005). 5. S. G. Chou, F. ... Ünlü, B. B. Goldberg, A. K. Swan, S. B. Cronin, Nano Lett.

27 Apr 2014: aperfect Huffman code is possible with codewords {A = 0, B = 10, C = 11}. ... b b bb c aa a a. where b indicates pixels coded before c, and a indicates pixels coded after c.

30 Aug 2014: b) An organism flapping its straight rigid tail (recip-rocal motion) cannot swim either. ... 1.18a) gives B = U2 = 1/2. Therefore, the second-order solution reads.

8 Oct 2014: Wireless network coverage has been greatly improved throughout the College. Work is now in progress to strengthen our ability to handle further increases in conference and ‘B&B’ business during the ... S e n i o r M e m b e r s.

19 May 2014: 0P G F P G FD D D B B B      . ( ... F F G PD B X M r D D     .

7 Oct 2014: An interesting result is the restriction of class B metrics due to the diagonalisability. ... isomonodromic construction to study a particular class of ASD non-diagonal class B.