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  2. New technique to synthesise nanostructured nanowires | University of…

    https://www.cam.ac.uk/research/news/new-technique-to-synthesise-nanostructured-nanowires
    Thumbnail for New technique to synthesise nanostructured nanowires | University of Cambridge 16 Jul 2015: To unravel the complexities of this process, the research team used two customised electron microscopes, one at IBM’s TJ Watson Research Center and a second at Brookhaven National Laboratory.
  3. Dr Zuehlsdorff

    www.tcm.phy.cam.ac.uk/profiles/tjz21/
    7 Oct 2015: TJ Zuehlsdorff, ND Hine, JS Spencer, NM Harrison, DJ Riley and PD Haynes,TCM Group, 19 JJ Thomson Ave, Cambridge, CB3 0HE, UK  Privacy policy  Design by Drs .
  4. MAXIMUM ENTROPY PROPERTY OF DISCRETE-TIME STABLE SPLINE KERNEL Tohid…

    sigproc.eng.cam.ac.uk/foswiki/pub/Main/TA417Publications/ArdeshiriC2015.pdf
    9 Apr 2015: Furthermore, let 0 tj < ti,. Var[g(ti) g(tj)] = E.  ir=j1. ... h(tr)tr tr1. 2. =. ir=j1. λ(tr tr1) = λ(ti tj). (15).
  5. Mathematics of Operational Research Example Sheet 2 R. Weber ...

    www.statslab.cam.ac.uk/~rrw1/mor/examples2.pdf
    2 Dec 2015: maximizesi,tj. { i. si j. tj : αiβj si tj 0, i, j}.
  6. Introduction to Cost-Effectiveness Analysis

    https://cscs3.medschl.cam.ac.uk/wp-content/uploads/GAM_slides1.pdf
    2 Mar 2015: Solution• For fixed αj. , the solution to minimizing the penalized least squares in the AM is whereˆ Hyβ = 1 ( )T Tj. ... AM). (GAM). 1 ( )T Tj jj. F X X S X X HXα = = 1 ( )T Tj j.
  7. https://www.hep.phy.cam.ac.uk/~lester/dtm662/mt2/Releases/oxbridgekine…

    https://www.hep.phy.cam.ac.uk/~lester/dtm662/mt2/Releases/oxbridgekinetics-0.8/README
    2 Mar 2015: Mt2_332_Calculator that expose the splitting at the MT2 minimum (used by MAOS methods and some top-quark mass reconstruction methods) 0.8 2nd March 2015 - At request of TJ
  8. baseline.eps

    https://www.cl.cam.ac.uk/~ey204/pubs/2015_HOTPLANET.pdf
    22 Jul 2015: u1. u2. ui…. …. t1t2. tj…. …Li. apply. gather scatter… …. apply. apply. u1. u2. ui…. …. t1. t2. tj…. …. gather scatter. ... Li. applyu1u2. ui…. …. t1. t2. tj…. …Li. gatherapply. scatter. (a) (b) (c).
  9. ANALYSIS II—EXAMPLES 4 Mich. 2014 The questions marked with ...

    https://www.dpmms.cam.ac.uk/study/IB/AnalysisII/2014-2015/14sheet4revised.pdf
    27 Feb 2015: Nj=1 ‖γ(tj) γ(tj1)‖ where the sup is taken over all. finite partitions 0 = t0 < t1 <. < tN = 1. (i) Give an example for which (γ) =. If γ is continuously
  10. The effect of flow capacities on the burstiness ofaggregated ...

    https://www.cl.cam.ac.uk/research/srg/netos/events/pam2004/papers/177.pdf
    22 Aug 2015: If the energy of a traffic process Xj atscale Tj=2. jT0 is higher than the energy of a Poisson process that has the same. ... average rate with Xj, then we say that Xj is bursty at scale Tj.
  11. Distributed systems Lecture 5: Consistent cuts, process groups, and…

    https://www.cl.cam.ac.uk/teaching/1415/ConcDisSys/DistributedSystems-1B-L5.pdf
    12 Feb 2015: Pj’s local state is WANT) – If (Tj, Pj) < (Ti, Pi) then queue request from Pi – Otherwise, reply with OK, and con@nue wai@ng. • ... Variant scheme (due to Lamport): – To enter, process Pi mul@casts request(Pi, Ti) [same as before] – On

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