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  2. lecture9.dvi

    www.damtp.cam.ac.uk/user/rrk26/Papers/lecture9.pdf
    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.
  3. 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.
  4. lecture10.dvi

    www.damtp.cam.ac.uk/user/rrk26/Papers/lecture10.pdf
    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).
  5. VOLUME 79, NUMBER 22 P H Y S I ...

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/Fygenson_etal.pdf
    3 Oct 2016: 2NEC Research, 4 Independence Way, Princeton, New Jersey 08540(Received 30 September 1996). ... 89, 11 547 (1992). [12] R. R. C. New,Liposomes: a Practical Approach(Oxford,New York, 1990), pp.
  6. Demas2003

    www.damtp.cam.ac.uk/user/sje30/waverepo/fourplot/Demas2003/zzz/Demas2003_p21_ctrl_2a_short_new.html
    28 Jan 2016:
  7. Motility of Colonial Choanoflagellates and the Statistics of…

    www.damtp.cam.ac.uk/user/gold/pdfs/choanowalks.pdf
    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).
  8. The Quantum Hall Effect Trinity Mathematical Society, October 2016 ...

    www.damtp.cam.ac.uk/user/tong/talks/quantumhall.pdf
    11 Oct 2016: that we will meet in Section 3. It is common to introduce some new notation to describe. ... opens up a whole new world of interesting physics involving non-Abelian anyons.
  9. J. Fluid Mech. (2016), vol. 799, R5, doi:10.1017/jfm.2016.408…

    www.damtp.cam.ac.uk/user/lauga/papers/121.pdf
    28 Jun 2016: New J. Phys. 9, 126. 799 R5-10. Phoretic flow induced by asymmetric confinement.
  10. An Adaptive Filon Algorithm for HighlyOscillatory Integrals Jing Gao…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2016_05.pdf
    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.
  11. NE7405

    www.damtp.cam.ac.uk/user/sje30/papers/network97.pdf
    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
  12. Security for control systems under sensor and actuator attacks ...

    www.damtp.cam.ac.uk/user/hf323/security_cdc2012.pdf
    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
  13. PHYSICAL REVIEW FLUIDS 1, 053202 (2016) Flow analysis of ...

    www.damtp.cam.ac.uk/user/lauga/papers/123.pdf
    1 Oct 2016: The resulting flow fields can be used to probe properties of both theswimmer and fluid, providing new insights into the physics of undulatory propulsion [11–15,18–20].
  14. Instabilities of a thin coating on a vertical fibre; Newtonian,…

    www.damtp.cam.ac.uk/user/hinch/talks/Vancouver2016a.pdf
    22 Feb 2016: I Second normal stress difference = tension in vortex lines new instability.
  15. Self-scaled bounds for atomic ranks: applications to nonnegative…

    www.damtp.cam.ac.uk/user/hf323/talks/tau_lower_bound_slides_SIAM_OPT_2014.pdf
    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.
  16. 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).
  17. A generalization of Filon-Clenshaw-Curtis quadrature for highly…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2016_04.pdf
    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.
  18. PHYSICAL REVIEW E 94, 052401 (2016) Filter-feeding, near-field flows, …

    www.damtp.cam.ac.uk/user/gold/pdfs/filter_feeding.pdf
    1 Nov 2016: Ryu, N. Matsumoto, M. Nagai, andH. A. Stone, A new angle on microscopic suspension feedersnear boundaries, Biophys.
  19. Sensing in the Mouth: A Model for Filiform Papillae as Strain…

    www.damtp.cam.ac.uk/user/lauga/papers/124.pdf
    1 Oct 2016: Cellular nanomechanics. In: Bhushan B,. editor. Springer Handbook of Nanotechnology. New York, NY: Springer (2010).
  20. INVITED ARTICLES PHYSICAL REVIEW FLUIDS 1, 060503 (2016) Soap-film ...

    www.damtp.cam.ac.uk/user/gold/pdfs/soap-film_prf.pdf
    19 Oct 2016: 406(Springer, New York, 1995). [8] F. Maggioni and R. L. Ricca, Writhing and coiling of closed filaments, Proc.
  21. P:\TEX\SIAP\70-7\76047\76047.dvi

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/old_literature/Keller2010.pdf
    18 Feb 2016: REFERENCES. [1] J. J. Stoker, Nonlinear Vibrations, Interscience, New York, 1950.[2] W. ... Magnus and S. Winkler, Hill’s Equation, Interscience, New York, 1966.[3] A.

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