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  2. Particle Flow and ILC Detector Design

    https://www.hep.phy.cam.ac.uk/~thomson/talks/HepForumRALFinal.pdf
    11 May 2006: B = 2T B = 4T B = 6T. σE/E = α(E/GeV)B-FieldAll angles. ... iv) Iterative Reclustering.  Current Performance (as of 6/5/06). e.g. B-Field.
  3. The Structural Engineer Journal

    www-civ.eng.cam.ac.uk/cjb/papers/p56.pdf
    6 Jun 2006: ô“ ÎNóx‹ÿTñTy?W#B»Ûvíñ—ÍEíîïrúpžäø¿lD…Ÿ6[Q œ›6«S}öôˆ#{lx£ÎxQcPÃO{óÏZܘ ÌÊwx«/ÒÇÑ08$F‘ÍéÉñç-BÅ{ ... Í–ü
  4. 1 Metric & Topological Spaces, sheet 2: (2006) 1. ...

    https://www.dpmms.cam.ac.uk/study/IB/MetricTopologicalSpaces/2005-2006/2006sheet2.pdf
    4 May 2006: Prove that X+ is a topological space and prove that it is compact (N.B. ... 18. A continuous surjective map p : E B is a covering if every point b B has an openneighbourhood V such that the connected components of p1(V ) are open in
  5. tiqit_complete_notes.dvi

    www.tcm.phy.cam.ac.uk/~sea31/tiqit_complete_notes.pdf
    6 Feb 2006: us the joint probability distribution pjk, and thus a joint entropy S(a, b):. ... Ψ〉 = a|00〉 b|01〉 c|10〉 d|11〉 =. . . abcd. .
  6. doi:10.1016/j.cell.2006.10.032

    https://www2.mrc-lmb.cam.ac.uk/groups/hegde/download/43_Kang_SW_Cell_2006.pdf
    30 Nov 2006: B) Cells stably expressing PrP or Opn-PrP. were treated with 10 mM DTT for 24 hr, re-. ... B) HeLa cells treated with 10 mM DTT for the indicated times were pulse labeled (for 15 min), fractionated, and quantified to determine the glyco-.
  7. EXPLICIT n-DESCENT ON ELLIPTIC CURVESI. ALGEBRA J.E. CREMONA, T.A. ...

    https://www.dpmms.cam.ac.uk/~taf1000/papers/n-descent-I.pdf
    13 May 2006: Then thereis an isomorphism of Brauer-Severi diagrams defined over K,. C //. φ. Pn1. ψ. E|n.0|. // Pn1. with σ(φ)φ1 = τξσ. We lift ψ to a matrix B ... It is evident that yσ =σ(B)B1 is an element of ΘE projecting onto ξσ.
  8. Particle Flow and ILC Detector Design

    https://www.hep.phy.cam.ac.uk/~thomson/talks/ALCPG_Fermilab.pdf
    7 Dec 2006: Large detector – spatially separate particlesHigh B-field – separate charged/neutralsHigh granularity ECAL/HCAL – resolve particles. ... What is optimal detector size/B-field, etc. THIS IS HARD – BUT VERY IMPORTANT!
  9. Osman, A. S., Mair, R. J. & Bolton, M. ...

    www-civ.eng.cam.ac.uk/geotech_new/people/bolton/mdb_pub/176.pdf
    16 Nov 2006: Amsterdam: Elsevier. Clough, G. W. & Schmidt, B. (1981). Design and performance ofexcavations and tunnels in soft clay. ... Géotechnique 43, No.2, 315 – 320. Peck, R. B. (1969). Deep excavations and tunnelling in soft ground.Proc.
  10. This isa super vis or’ sco py ofth enote ...

    www.damtp.cam.ac.uk/user/sjc1/teaching/NSTIB/notes.pdf
    28 Oct 2006: b) Suppose that B = 0; the vector field B(r) is said to be solenoidal. ... Then there exists anon-unique vector potential, A(r), such that. B = A.
  11. 1 Model-Based Hand Tracking Using a HierarchicalBayesian Filter…

    mi.eng.cam.ac.uk/reports/svr-ftp/thayananthan_pami06.pdf
    14 Sep 2006: The used costterm is thusI? £ F x Jt! #" tx Z £ «b«' Z BB aº B'B z»(17)where. ... I? " F B'B? s aò7µ F ÛóÌô4B'B. A partition of the state space is given by theVoronoi diagram defined by these nodes, seefigure 13a.ñ Partitioning the eigenspace

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