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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.