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28 Jan 2016:

2 Nov 2016: Breaking the coherence barrier: A new theory forcompressed sensing. B. AdcockSimon Fraser Univ. ... Yet they areoften asymptotically incoherent, and thus fall within the remit of the new framework.

28 Jan 2016:

28 Jan 2016:

28 Jan 2016:

12 Aug 2016: This. new nonlinear optimal is demonstrably more efficient in triggering turbulence than the linear optimal. ... 8 OCTOBER 2010. 154502-2. the possibility that a further new optimal may emerge.

12 Aug 2016: From another perspective, the edge-tracking technique can beviewed as a powerful new approach to finding nonlinear solutions of the Navier-Stokesequations. ... 18] J. Vollmer, T.M. Schneider & B. Eckhardt, Basin boundary, edge of chaos and edgestate in a

12 Aug 2016: The structure of the new 3Doptimal is much more complicated: see Figure 8. ... It should be clear that there is much to exploreand understand in this promising new variational approach.

5 Jul 2016: 1. Turbulence without cascades – new insightsfrom Jupiter’s unearthly jets. By Michael Edgeworth McIntyre. ... REFERENCES. Thomson, S. I. & McIntyre, M. E. 2016 Jupiter’s unearthly jets: a new turbulent modelexhibiting statistical steadiness

12 Aug 2016: This new relationship still implied that no finite value for Rec existed (see Figure 8: notethe last Re considered and the later work of [1] discussed below).

6 Oct 2016: Ourgoal is to propose a new method to compute the update times forST control of diagonalizable linear systems. ... is a sequence of update times at which a new measurement istransmitted to the controller and input signals are applied tothe system.

6 Oct 2016: 13 / 14. Conclusion. I A new lower bound on rank+(M) using convex optimization andsum-of-squares techniques. ... Conclusion. I A new lower bound on rank+(M) using convex optimization andsum-of-squares techniques.

22 Jan 2016: Building an ARW from passiveparticles leads to no new behavior, but motile particlesalso have a stochastic velocity term. ... Kessler, A new continuum model forsuspensions of gyrotactic micro-organisms, J. Fluid Mech.212, 155 (1990).

3 Oct 2016: 11 x. meiω g(x)dx, m 0, are explicitly available, the new integral can be com-puted easily. ... Adaptive Filon, though,re-evaluates f afresh for every ω and subsequently forms a new interpolating poly-nomial.

26 Feb 2016: We then tested the network on a new random-dot stereogram and found that the correlation between the network output and disparitywas maintained (|r| > 0.89) (see figure 2(c)). ... In figure 3(b) (right) it can beseen that when the trained network is

6 Oct 2016: In our previous work [1] we adopted a novel point ofview inspired from error-correction over the reals [10] whichallowed us to propose a new estimation algorithm that isrobust against the ... In this section we ask if one can also enforce the numberof

17 Aug 2016: In this paper we propose to ex-tend FCC to a new method, FCC+, which can attain an arbitrarily high asymptoticorder while preserving the advantages of FCC.

7 Jun 2016: to a dynamical gauge field. This, in turn gives rise to a new topological current? ... new background gauge field through a BF coupling takes us back to the duality (2.9).

12 Jul 2016: J. New Journal of Physics 16(10), 103039(2014). [50] Solnyshkov, D. D., Johne, R., Shelykh, I.

20 Jan 2016: In (Bader et al. 2014), the current authors established a new framework for a numericalapproach to the linear time-dependent problem with an autonomous potential,.