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10 Apr 2011: 3(a) and 3(b). Since the BB bonding is stronger than that. ... n A, with M = 1. j It) tiJ: e/eB et/eB A A 200 1 0.15 -4.2 B B 200 1 0.15 -7.2 A B 200

11 Dec 2017: A B B, ,-------_. D a C, Consider the prism AC in motion relatively to the ether in direction AB with velocity 0. ... the velocity in the free ether; or if f1= then t=fla b.

8 Mar 2012: b) Pψ(x) = λψ(x) and P 2ψ(x) = ψ(x) λ2 = 1. ... This gives. Aκ cos κa. A sin κa=. B k cos (ka δ0).

8 Jun 2013: a. b. c. e. f. g. d. HoloceneYDB–AODLGM. Figure 4 | Hemispheric temperatures. ... 33. Stephens, B. B. & Keeling, R. F. The influence of Antarctic sea ice on glacial-interglacial CO2 variations.

25 Aug 2022: Preprint typeset in JHEP style - HYPER VERSION. F́ısica Estad́ıstica. David Tong. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical Sciences. Wilberforce Road,. Cambridge, CB3 OBA, UK.

10 Apr 2011: 21<b). B. Hydrogen bond strength. With the proviso given above for the interpretation of the trends in the parameter R, given our simplified fitting procedure, we can still make several ... C. Wheeler, and B. Widom, J. Am. Chem. Soc. 90. 3064 (1968); J.

26 Jul 2023: A and. B are both self-adjoint and that. Bis positive and invertible. ... We take the completion of this space,. HB1. D(B) is dense in.

5 Oct 2013: The degree ofan operator A B(H) is defined by. deg(A) = supn1. ... Let A B(H) and let {ej} be an orthonormal basis for H.

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).

5 May 2015: Θ′(h) = dexp1Θ(h)A(h) =. m=0. Bmm! admΘ(h)A(h), (2.4). where Bm are Bernoulli numbers and the adjoint map is recursively defined by ad0A(B) =. B, ... adk1A (B) = [A, adkA(B)]. Magnus (1954) resorted to solving the dexpinv equation.

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).

10 Jul 2009: Combination Particles Fluid Tube ξ(0.1)1 A a 1 2.302 A b 1 2.153 D a 1 3.354 B a 2 1.805 B b 2 ... 30 2.84 0.02 0.615 0.590 0.5455 B b 2 16 17.4 0.40 3.65 0.10 0.600 0.565 0.5206 C a

7 Apr 2021: A natural choice is symmetric. gauge. A = 12x B = B. ... B = 0. Third, this particular Maxwell equation would appear to be non-negotiable.

13 Apr 2007: The degree ofan operator A B(H) is defined by. deg(A) = supn1. ... Let E B and F B be closed subspaces of a Banachspace B.

18 Nov 2010: The concept in a more relaxed form. 176 B. H. Zimm and S. ... 1987) and by Jonsson et al. (1988). 188 B. H. Zimm and S.

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.

15 Jul 2011: 12 f ). Allow fora sloping bottom boundary z = b(x, y), taking care to distinguish between the layer depth h andthe free-surface elevation ζ(x, y, t). ... b = b(y) =. {. ǫa, y > aǫy, |y| < a.

10 Jul 2009: a) Gravity acts on the fundamental mode to create the firstharmonic in (b). ... b) Capillary pressure gradients act to create the phase-shifted first harmonicin (c).

21 Jan 2015: Using (2.14a,b) to evaluate P1 and P2 in (2.11), we obtain. ... its asymptotic value isdependent on all the parameters M, B, D and XF.

8 Nov 2015: Let E B and F B be closedsubspaces of a Banach space B. ... Pk(T z)Pk))2nPmH. (6.2). 13. and the fact that for self-adjoint A,B B(H) we have dH(σ(A),σ(B)) ‖AB‖ it suffices to show

24 Aug 2009: 3A(sin4 8, sin 24,) - 2(A - B)(sin28, sin 24,)}, of, = of. = ... A , B, F, 211, would not be related to the particle aspect ratio in 6he manner described for spheroids.

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.

13 Dec 2018: f(x,y,y′) dx. [using a Taylor expansion to first order]. =. b. ... to travel from A to B, B. A. dl. c, (1.32).

1 Sep 2011: 2.2.2 The matrices B, B′, C. Setyν := D(hν )qν, ν < N; yN := D(hN1)qN,. ... By definition (2.2.9),. C := CNν := ADγ1ADγ2 ADγN ν A,B := Bν := ADδ1ADδ2 ADδν ,B′ := B′ν := D0BD0,.

16 Aug 2023: a (b c) = (a c)b (a b)c. (0.11e). Line integrals. ... Further examples. (i) As another example consider the equation (a b)c = d.

7 Apr 2017: M i t 25 T e x t a b b i l d u n g e n. ... die GELEIschen A b b i l d u n g e n fiber Paramevium-Ln'gssehnitte m i t d e m y o n WETZET, a n Flaehschnitten.

5 Jun 2013: above, i.e. compass-wise, in the northern hemisphere, corresponding to up-. ward B. ... waves. The background rotation and azimuthal magnetic field B point. toward the viewer.

17 Jun 2019: a = a(x;y;t); b = b(x;y;t) ; (2.4). when inserted into (2.2), expresses h(a; t) as another function. ... the general 2-dimensional Monge{Ampere equation. A B 2C D& E(&. 2. ) =

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. ′=

29 Jul 2017: AB =.  0 11 0.  and A′B′ = 0 11 0. ... kernels of the span of the frame eA′B′C′D′. 30 CHAPTER 2.

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‖.

3 Sep 2009: Bernard, B. Hambrecht, P. Lugan, D. Clement,L. Sanchez-Palencia, P. Bouyer, A. ... Rev. Lett. 101 (2008)080401. [65] Th. Anker, M. Albiez, B. Eiermann, M.

2 Oct 2016: b. B( 41t'l. kT -KL. fJ. kT 2 [' 2 Jb 4 -;] K- 2 ,B-ln (I-e) 2 roo. ... Values of b that were derived in the previous section are listed in Table 1.

13 Jul 2009: As a model problem we take. %(x) = U_[l - exp( -x/b)], (1). ... As indicated above, to make the calculation tractable we shall, however, assume that b B a so that the flow is almost unidirectional almost everywhere and lubrication methods can be employed.

24 Jul 2018: a)(a) (b)(b). (c)(c) (d)(d). Fig. 1. (a) 12.5% uniform random subsampling scheme, (b) CS reconstructionfrom uniform subsampling, (c) 12.5% multilevel subsampling scheme, (d) CS ... b}. The kth relative sparsity is. Sk = Sk(N,M,s) = maxzΘ‖PNk1Nk Uz‖.

3 Oct 2008: a b) (c d) = (a b)i(c d)i= (ǫijkajbk)(ǫilmcldm). = ǫijkǫilmajbkcldm. = ( ... Eliminate E:. 2B. t2= E. t= 1. µ0ǫ0 ( B). Now use the identity ( B) = ( B) 2B and Maxwell’sequation B = 0 to obtain the (vector) wave equation.

11 Dec 2017: F Y Y G1 m b J b —B = a Positive quantity. ... A S x KS l > J p - B’<P$d eb a y - k.

27 Jan 2018: d B dB' _ - B --B '. Aus dieser und aus der zuletzt gefundenen Gleichung folgt aber J = J '. Es ist somit erwiesen, da0 J weder von F noch von. ... 8 (P 4 - B Gmmm a x. oder a v - D- 8 X.

4 Nov 2013: ηN =[. 2π 1. 0. f0. s[ B f (y), z]yd zd y. ... s0( f B) B f (33a)and. F( f B) 2. 4(2 ) ( f B)3 , (33b).

27 Jun 2010: In such a basis, a full 2. PHYSICAL REVIEW B 81, 235302 2010. ... with the analogous equation for R following by replacingL R and B B.

4 Nov 2013: the current first reaches the sink, as illustrated in figure 2(a, b). ... B). The results of this more detailedmodel are also shown in figure 6.

20 Dec 2013: a µ, b ν etc.). For example, consider the quantity ηaXa in theabstract index notation. ... Aµνfν, e′µ = B. νµeν (2.25). for some matrices Aµν and Bνµ.

10 Oct 2011: D(g) =(D̂(g) B(g). 0 C(g). )for u =. (û0. ), (1.19). ... v1,v2) a. (e2πki. n v1,e 2πki. n v2) = (v1,v2)A, (v1,v2) b.

2 Sep 2012: are close (a) to each other; and (b) to the predictionsof continuum diffusion. ... Dk T. a= B. eff6ph. D Mµ -1 3. t pspreading = ( )a D2 22.

4 Nov 2013: vf (x, t) = kf. μ. ρg(h b). b= φγ kf. ... xf = 11 cm. Balance Balance. PumpW = 1.1 cm. b = 2.1 cm.

3 Mar 2020: Let A have r = rA and B have r = rB where rB > rA. ... Now imagine that we are considering light waves propagating from A to B.

22 Jul 2010: Further properties of J and K j j. Appendix B. Derivation of theorem I. ... v?,, = (v,tF (v,jF q , t , m,i = (v,$ q , i 9 (2.4u, b ). B(x, t ) = x E(X, t ) , (2.6). (vii) The mapping (2.2)

5 Oct 2013: The degree ofan operator A B(H) is defined by. deg(A) = supn1. ... Let A B(H) and let {ej} be an orthonormal basis for H.

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 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.