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  2. Part III. The rheology of suspensions

    www.damtp.cam.ac.uk/user/hinch/teaching/CISMejh56.pdf
    12 May 2014: Spheroid: axes a,b,b, aspect ratio r = ab. rod r > 1 disk r < 1. ... hτf (A I ). σ = pI 2µE Gf A. I Oldroyd B f = 1.
  3. Part III. The rheology of suspensions

    www.damtp.cam.ac.uk/user/hinch/teaching/CISMejh56handout.pdf
    12 May 2014: Spheroid: axes a,b,b, aspect ratio r = ab. rod r > 1 disk r < 1. ... hτf (A I ). σ = pI 2µE Gf A. I Oldroyd B f = 1.
  4. D:EJSNE0106.DVI

    www.damtp.cam.ac.uk/user/sje30/papers/eglen2000.pdf
    14 Jun 2014: a) NND.(b) RI. (c) Percentage of cells that moved during the simulation. ... Neurosci.5741–50. [34] Wässle H, Peichl L and Boycott B B 1981 Dendritic territories of cat retinal ganglion cellsNature292344–5[35] Wässle H and Riemann H J 1978 The
  5. No Job Name

    www.damtp.cam.ac.uk/user/sje30/papers/eglen2005.pdf
    14 Jun 2014: andcells of opposite type B! The vertical line indicatesthe effective radius of the central dip Rodieck,1991! ... B! Like A, for the W81S1dataset. Again statistical independence is rejected P 0.006!
  6. On Spectral Inclusion Sets and Computing theSpectra and Pseudospectra …

    www.damtp.cam.ac.uk/research/afha/workshops/cid2014/ChandlerWilde.pdf
    23 Jul 2014: b0 0 1. b1 0. ,. where b = ( ,b1,b0,b1, ) {1}Z is a pseudoergodicsequence. ; ... every finite pattern of 1’s can be foundsomewhere in the infinite sequence b.
  7. S0952523812000338 283..299

    www.damtp.cam.ac.uk/user/sje30/papers/hore2012.pdf
    14 Jun 2014: C, D) Autocorrelogram of mosaics in (A) and (B), with 25 lm annuli. ... Only the large black dots were analyzed in panel (B); small black dots werediscarded.
  8. 25 Jul 2014: PA B A′ B′ = A B A′ B′ A BA′ B′transforms as. ... A(A′ B′)C ′ A B B(A′B′)C ′ = 0,. which in turn uses the vanishing of the SD Weyl spinor.
  9. dql003

    www.damtp.cam.ac.uk/user/sje30/papers/eglen2006.pdf
    14 Jun 2014: The RI of this field is 5.1. (b) Autocorrelation plot of the field shown in (a). ... Cells in (b) are not drawn to scale for clarity.) Data kindly provided by Dr Lucia Galli-Resta.
  10. b907213f 1527..1535

    www.damtp.cam.ac.uk/user/sje30/papers/godfrey2009_review.pdf
    14 Jun 2014: M. Grzywacz, J. Neurosci., 1994, 14,. 7426–7439.34 M. B. Feller, D. ... Shatz, Neuron, 1997, 19, 293–306.35 K. B. Godfrey and N. V.
  11. On asymptotic structure in compressed sensingBogdan Roman ∗, Ben ...

    www.damtp.cam.ac.uk/user/abr28/Asymptotic_10a.pdf
    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‖.
  12. Development/Plasticity/Repair Developmental Modulation of Retinal…

    www.damtp.cam.ac.uk/user/sje30/papers/sernagor2003_jn.pdf
    14 Jun 2014: Wave propagation is much slower. S25 A, B, andD exhibit complicated, “zigzagging” propagation patterns. ... B,GABA-induced wave in a DR4 retina (conventions as in Fig. 6 B).
  13. R Programming

    www.damtp.cam.ac.uk/user/sje30/rpc.pdf
    14 Jun 2014: s e q ( f =5 , t =1) ## a b b r e v t a g s. ... 1 ## i n c r e m e n t j b y 1. •
  14. PHYSICS OF FLUIDS 26, 071902 (2014) Dynamics of swimming ...

    www.damtp.cam.ac.uk/user/lauga/papers/92.pdf
    20 Jul 2014: G S D (r ; a, b) = (b.0)G S(r ; a), (15). ... G Q (r ; a, b) = (b.0)G D (r ; a), (18)where the notation 0 is used to denote a gradient taken with respect to the singularity location, x0.A
  15. On asymptotic structure in compressed sensingBogdan Roman ∗, Ben ...

    www.damtp.cam.ac.uk/research/afha/bogdan/Asymptotic_10a.pdf
    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‖.
  16. R Programming

    www.damtp.cam.ac.uk/user/sje30/rpc-4up.pdf
    14 Jun 2014: s e q ( f =5 , t =1) ## a b b r e v t a g s. ... 1 ## i n c r e m e n t j b y 1. •
  17. 24 Sep 2014: This is evaded by:. (a) Confinement for gluons. (b) Higgs mechanism for W,Z. ... 20 c c = b20 b b = 1. Thus we see that the left action of g defines an.
  18. Slide 1

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/140911-ufk-2-corr2.pdf
    28 Nov 2014:   . 2. 0. B. b. k T. gt   2. ... Polymer cannot reach a new equilibrium configuration during translocation of each segment b. •
  19. Part II Principles of Quantum MechanicsMichaelmas 2014 Prof. R.R. ...

    www.damtp.cam.ac.uk/user/rrh/notes/pqm14_281014.pdf
    28 Nov 2014: A b B. |ψyb |φy. “. A|ψy. b. B|φy. and extend by linearity. ... The general multiparticle statesbelong to. V1 b V2 b. b VN , (5.3.1)with basis states.
  20. On Asymptotic Incoherence and its Implications forCompressed Sensing…

    www.damtp.cam.ac.uk/research/afha/anders/1DCoherence_6.pdf
    24 Jun 2014: a] [b], b R(B1). Definition 2.5 (Optimal ordering). Given the setup above, then any element of the optimal equivalence classis called an ‘optimal ordering of the basis pair ... Theorem 2.14. Let U B(l2(N)) be an isometry. ThenN µ(QNU) diverges.
  21. PII: S1350-9462(00)00024-0

    www.damtp.cam.ac.uk/user/sje30/papers/sernagor2001.pdf
    14 Jun 2014: The lengths of processes 1,2 and 3 are plotted over time in (B). ... Theboxed region is enlarged in (B); (C) is a 90 degree rotation of (B).

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