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348_2007_387_43_5-web 737..753
www.damtp.cam.ac.uk/user/gold/pdfs/eif.pdf10 Apr 2011: R E S E A R C H A R T I C L E. Fluid dynamics of self-propelled microorganisms,from individuals to concentrated populations. Luis H. Cisneros Æ Ricardo Cortez ÆChristopher Dombrowski Æ Raymond E. Goldstein ÆJohn O. Kessler. Received: 13 February -
Phenomenological theory of multiply reentrant solubility Raymond E.…
www.damtp.cam.ac.uk/user/gold/pdfs/JChemPhys_83_1246.pdf10 Apr 2011: tJ.Se(T,Hcrit ) = Se(T,H--Hcrit ) - Se(T,H--Hcrit -). (17). where.tJ.Ms is the order parameter jump of the SM. ... tJ.Me(T ,Hcrit) = Me(T ,H--Hcrit ) - Me(T ,H--Hcrit -). (18). -
Papers by authors F to L
https://www.vhi.st-edmunds.cam.ac.uk/system/files/documents/2011-authorsF-L.pdf8 Sep 2011: 1. Cambridge International Conference on Open, Distance and e-Learning. Internationalisation and Social Justice: the role of Open, Distance and e-Learning. Papers by authors F - L. Page. Ahmad Fadlallah Bridging the gap in digital divide 3. Maria de -
msq280 1043..1056
www.jiggins.gen.cam.ac.uk/pdfs/obbard2010mbe.pdf4 Feb 2011: Recent and Recurrent Selective Sweeps of the Antiviral RNAiGene Argonaute-2 in Three Species of Drosophila. Darren J. Obbard,,1,2 Francis M. Jiggins,3 Nicholas J. Bradshaw,4 and Tom J. Little1,2. 1Institute of Evolutionary Biology, University of -
Monotonic and Insensitive Optimal Policies for Control of Queues with …
https://www.statslab.cam.ac.uk/~rrw1/publications/Stidham%20-%20Weber%201989%20Monotonic%20and%20insensitive%20optimal%20policies%20for%20control%20of%20queues%20with%20undiscounted%20costs.pdf15 Sep 2011: Now. Z7ji, i- 1) =tj(i, i - )c(y) hj(i, i - 1). ... 1, O)]/[tj(1, 0) X-'] < oo.). -
201019079 10940..10945
www.damtp.cam.ac.uk/user/gold/pdfs/noise.pdf6 Jul 2011: Phys Rev E Stat Nonlin Soft Matter Phys 80:041922.22. Ishikawa T, Locsei JT, Pedley TJ (2008) Development of coherent structures in concen-. ... Science 325:487–490. 43. Pedley TJ, Kessler JO (1992) Hydrodynamic phenomena in suspensions of -
Markov Chains, Computer Proofs, andAverage-Case Analysis of Best Fit…
https://www.statslab.cam.ac.uk/~rrw1/publications/Coffman%20-%20Johnson%20-%20Shor%20-%20Weber%201993%20Markov%20chains,%20computer%20proofs,%20and%20average-case%20analysis%20of%20best%20fit%20bin%20packing.pdf15 Sep 2011: chains Mj,K, t > 1,which have the same state space w MJ,K = (S,K, TJ,K ),but have product matrices J,K for transition functions, i.e.,chains in ... The tint is theta [ 1, an n(,K x. larray of integers,that is used as a sparse representation for the -
Microfluidics of cytoplasmic streaming and itsimplications for…
www.damtp.cam.ac.uk/user/gold/pdfs/streaming_pnas.pdf10 Apr 2011: Magar V, Goto T, Pedley TJ (2003) Q J Mech Appl Math 56:65–91.35. -
201019079 7..12
www.damtp.cam.ac.uk/user/gold/pdfs/noise_SI.pdf6 Jul 2011: 1. Pedley TJ, Kessler JO (1992) Hydrodynamic phenomena in suspensions of swimmingmicroorganisms. -
Stability of Flexible Manufacturing Systems
https://www.statslab.cam.ac.uk/~rrw1/publications/Courcoubetis%20-%20Weber%201994%20Stability%20of%20flexible%20manufacturing%20systems.pdf15 Sep 2011: In a similar manner as in the proof of Theorem 2, we have that for s = o-i and t = Tj,. ... T'E4 (X('Tj) E (Nk (st) -Nk (S))t). and therefore E(vi) is o(t). -
201019079 1..6
www.damtp.cam.ac.uk/user/gold/pdfs/PNAS-2011-Drescher-1019079108.pdf20 Jun 2011: Phys Rev E Stat Nonlin Soft Matter Phys 80:041922.22. Ishikawa T, Locsei JT, Pedley TJ (2008) Development of coherent structures in concen-. ... Science 325:487–490. 43. Pedley TJ, Kessler JO (1992) Hydrodynamic phenomena in suspensions of -
Effective Bandwidths for Stationary Sources
https://www.statslab.cam.ac.uk/~rrw1/publications/Courcoubetis%20-%20Weber%201995%20Effective%20bandwidths%20for%20stationary%20sources.pdf15 Sep 2011: P, = m, o(6). (3). PROOF: Suppose that we observe the contents of the buffer at the ends ofepochs (tj]1L_„, where t-, = / [ £ / £ ] , for some £ > 0. -
MMB160.indd
www.damtp.cam.ac.uk/user/gold/pdfs/spirochete_review.pdf10 Apr 2011: Nature 2001; 413: 39–44. Wilson DR, Beveridge TJ: Bacterial f lagellar fila-ments and their component f lagellins. -
Generalized sampling and the stable and accuratereconstruction of…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2011_12.pdf22 Nov 2011: Tj(x) = cos(j arccos x), j = 0, 1, 2,. ,. and c0 = 1π , cj =. 2π , j 6= 1. ... Given that the polynomials Tj are orthogonal with respect to the weight. -
PART I: Symmetries and particles. NOTES BY PROF. HUGH ...
www.damtp.cam.ac.uk/user/examples/3P2Lb.pdf10 Oct 2011: PART I: Symmetries and particles. NOTES BY PROF. HUGH OSBORN. Books. Books developing group theory by physicists from the perspective of particle physics are. H. F. Jones, Groups, Representations and Physics, 2nd ed., IOP Publishing (1998).A fairly -
msr124 2921..2933
www.damtp.cam.ac.uk/user/gold/pdfs/b12.pdf27 Sep 2011: Insights into the Evolution of Vitamin B12 Auxotrophy fromSequenced Algal Genomes. Katherine E. Helliwell,1 Glen L. Wheeler,2,3 Kyriacos C. Leptos,4 Raymond E. Goldstein,4 andAlison G. Smith,1. 1Department of Plant Sciences, University of Cambridge, -
CHAPTER 13 MONOTONE OPTIMAL POLICIES FOR LEFT-SKIP-FREE MARKOV…
https://www.statslab.cam.ac.uk/~rrw1/publications/Stidham%20-%20Weber%201999%20Monotone%20optimal%20policies%20for%20left-skip-free%20Markov%20decision%20processes.pdf18 Sep 2011: Pij (J1) = P { i K (tJ ) -] = j L1 i < j 1, pEA,. -
J. Phys. II France 6 (1996) 767-796 MAY 1996, ...
www.damtp.cam.ac.uk/user/gold/pdfs/gnps.pdf10 Apr 2011: J. Phys. II France 6 (1996) 767-796 MAY 1996, PAGE 767. Front Propagation in the Pearling Instability of Tubular Vesicles. Raymond E. Goldstein (), Philip Nelson (), Thomas Powers (>)and Udo Seifert (). () Joseph Henry Laboratory of Physics, -
Stability of On-Line Bin Packing with Random Arrivals and…
https://www.statslab.cam.ac.uk/~rrw1/publications/Courcoubetis%20-%20Weber%201990%20Stability%20of%20on-line%20bin%20packing%20with%20random%20arrivals%20and%20long-run%20average%20constraints.pdf15 Sep 2011: lim l-Z"(tJ)cJb=f. (l.Dt—co t j =. The model here is the same as that in Refs. -
DAMTP 2010/NA04 Beyond symmetric Broyden for updating quadratic…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2010_04.pdf13 Apr 2011: F(x) = 12xT{ n. j=1 100(j1)/(n1) vj v. Tj. }x, xRn. -
Continuum theory of critical phenomena in polymer solutions:…
www.damtp.cam.ac.uk/user/gold/pdfs/JChemPhys_90_7448.pdf10 Apr 2011: Continuum theory of critical phenomena in polymer solutions: Formalism and mean field approximation. Raymond E. Goldstein Laboratory of Atomic and Solid State Physics and Materials Science Center, Clark Hall, Cornell University, Ithaca, New York -
Physics of chemoreception
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/bergpurcell.pdf6 Oct 2011: 52 predicts for a single receptor if IJ = TJ(1 - p). -
g.dvi
www.damtp.cam.ac.uk/user/na/people/Alexei/papers/markov.pdf1 Sep 2011: APPROXIMATION THEORY:A volume dedicated to Borislav Bojanov(D. K. Dimitrov, G. Nikolov, and R. Uluchev, Eds.)additional information (to be provided by the publisher). Twelve Proofs of the Markov Inequality. Aleksei Shadrin. This is the story of the -
A survey of Markov decision models for control of networks of queues
https://www.statslab.cam.ac.uk/~rrw1/publications/Stidham%20-%20Weber%201993%20A%20survey%20of%20Markov%20decision%20models%20for%20control%20of%20networks%20of%20queues.pdf15 Sep 2011: N o t e that A is symmetric in i and j , since the operators Ti and Tj commute. -
THE ROTARY MOTOR OF BACTERIAL FLAGELLA
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/ufk_papers/membrane_proteins/bergreview.pdf27 Nov 2011: THE ROTARY MOTOR OF BACTERIALFLAGELLA. Howard C. BergDepartment of Molecular and Cellular Biology, Harvard University, 16 DivinityAvenue, Cambridge, Massachusetts 02138; email: hberg@biosun.harvard.edu. Key Words Escherichia coli, motility,
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