Search

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.

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.

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.

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

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.

10 Jul 2009: away from the (collapsed) numerical results. and secularity is averted at order O(β1) if T0 B 0, whence B = B(T1) and. ... B(T ) ={. 1 T. 24β. }1/2. (5.2). Thus, for T 1,.

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.

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,.

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.

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.

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. ′=

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. ) =

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.

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

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.

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.

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‖.

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.

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).