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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.

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: 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

14 Jun 2014: andcells of opposite type B! The vertical line indicatesthe effective radius of the central dip Rodieck,1991! ... B! Like A, for the W81S1dataset. Again statistical independence is rejected P 0.006!

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.

14 Jun 2014: C, D) Autocorrelogram of mosaics in (A) and (B), with 25 lm annuli. ... Only the large black dots were analyzed in panel (B); small black dots werediscarded.

25 Jul 2014: PA B A′ B′ = A B A′ B′ A BA′ B′transforms as. ... A(A′ B′)C ′ A B B(A′B′)C ′ = 0,. which in turn uses the vanishing of the SD Weyl spinor.

14 Jun 2014: The RI of this field is 5.1. (b) Autocorrelation plot of the field shown in (a). ... Cells in (b) are not drawn to scale for clarity.) Data kindly provided by Dr Lucia Galli-Resta.

14 Jun 2014: M. Grzywacz, J. Neurosci., 1994, 14,. 7426–7439.34 M. B. Feller, D. ... Shatz, Neuron, 1997, 19, 293–306.35 K. B. Godfrey and N. V.

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 Jun 2014: Wave propagation is much slower. S25 A, B, andD exhibit complicated, “zigzagging” propagation patterns. ... B,GABA-induced wave in a DR4 retina (conventions as in Fig. 6 B).

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. •

20 Jul 2014: G S D (r ; a, b) = (b.0)G S(r ; a), (15). ... G Q (r ; a, b) = (b.0)G D (r ; a), (18)where the notation 0 is used to denote a gradient taken with respect to the singularity location, x0.A

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 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. •

24 Sep 2014: This is evaded by:. (a) Confinement for gluons. (b) Higgs mechanism for W,Z. ... 20 c c = b20 b b = 1. Thus we see that the left action of g defines an.

28 Nov 2014:   . 2. 0. B. b. k T. gt   2. ... Polymer cannot reach a new equilibrium configuration during translocation of each segment b. •

28 Nov 2014: A b B. |ψyb |φy. “. A|ψy. b. B|φy. and extend by linearity. ... The general multiparticle statesbelong to. V1 b V2 b. b VN , (5.3.1)with basis states.

24 Jun 2014: a] [b], b R(B1). Definition 2.5 (Optimal ordering). Given the setup above, then any element of the optimal equivalence classis called an ‘optimal ordering of the basis pair ... Theorem 2.14. Let U B(l2(N)) be an isometry. ThenN µ(QNU) diverges.

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).

4 Nov 2014: values ofTh and ho:> given in Table 1 ofHodgkin & Huxley (1952c) (method B). ... Thetime scale changes between d, D and e, E. The current scale changes after b, B; c, C; d, Dandf, F.

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.

21 Feb 2014: a] [b], b R(B1). Definition 2.5 (Optimal ordering). Given the setup above, then any element of the optimal equivalence classis called an ‘optimal ordering of the basis pair ... Theorem 2.14. Let U B(l2(N)) be an isometry. ThenN µ(QNU) diverges.

24 Jun 2014: a] [b], b R(B1). Definition 2.5 (Optimal ordering). Given the setup above, then any element of the optimal equivalence classis called an ‘optimal ordering of the basis pair ... Theorem 2.14. Let U B(l2(N)) be an isometry. ThenN µ(QNU) diverges.

23 Mar 2014: xn of a real valuedcontinuous function f : [a,b] R defined on [a,b]. ... Theorem 1.9. Let pnPn interpolate fC[a,b] at n1 distinct points x0,.

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. ′=

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.

9 Dec 2014: 2006) and in Showman (2007), or. b = b(ζ) = bmax ρ(ζ) (3.5). ... The run with b = 1, included forcomparison and contrast with Li et al.

9 Sep 2014: Figure 1. Sketches of microscopic swimmers, to scale. (a) E. coli.(b) C. ... In fact, symmetryimplies that the swimming speed U must be an even functionof b.

6 Nov 2014: The Frobenius integrability condition yields. [X,Y ] = aX bY. for some a and b. ... 2.14). Let ΣA′B′ be the usual basis of SD two forms.

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.

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.

10 Jan 2014: totalvolume V an amount proportional to the number of particles N,with an effective excluded volume per particle b. ... eβUip(r) = exp(2zizpe2/bkBT) = r. 2zizpλB/b. where λB is the Bjerrum length we previously introduced.