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  1. Results that match 1 of 2 words

  2. 26 Jan 2024: a) Subject to the above constraints, find the optimal achievable value of Fcl(j), and show thatif θ = π/4 then the optimal cloning fidelity is cos2(π/24).
  3. Publications | Disease Dynamics Research Group

    www.damtp.cam.ac.uk/research/dd/publications?page=4
    14 Jul 2024: Molecular biology and evolution. (2007). 24,. 1811. (doi: 10.1093/molbev/msm103). Campylobacter jejuni colonization and transmission in broiler chickens:: a modelling perspective.
  4. brum_mjc

    www.damtp.cam.ac.uk/user/mjc249/talks/Edinburgh_mjc.pdf
    21 Mar 2024: orthogonal projection. 24. Convergence theoryKey ingredient: unitary discretization. 25. Spectral measures. ... Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24.
  5. Opto-fluidically multiplexed assembly and micro-robotics

    www.damtp.cam.ac.uk/user/lauga/papers/223.pdf
    28 Feb 2024: With rapid implementation and advanced control,it might be feasible to position one particle every fewmicrometers, which is the typical length scale over whichthe flow fields exhibit significant decay22,24. ... eLight 1, 7 (2021). 24. Liao, W. et al.
  6. A3La.dvi

    www.damtp.cam.ac.uk/user/examples/A3La.pdf
    21 Oct 2014: Section 3. An obvious theme (I hope!). 21) 2x(3 x2) 24) xex2/2 27) tan x = sin xcos x. ... 22) cos x2 23) 14 sin4 x 24) ex. 2/2 25) 13 (1 x2)3/2 26) 12 tan.
  7. University of Cambridge, DAMTP: Goldstein Lab

    www.damtp.cam.ac.uk/user/gold/press.html
    16 May 2022: Department of Applied Mathematics. and Theoretical Physics. Goldstein Lab. Recent Press. 2006-2015 Department of Applied Mathematics and Theoretical Physics, University of Cambridge. Information provided by R.E.Goldstein@damtp.cam.ac.uk.
  8. Meetings | Maciej Dunajski | University of Cambridge

    www.damtp.cam.ac.uk/user/md327/meetings.html
    10 Feb 2023: Meetings I have (co)organized or I am (co)organizing.
  9. 5 Jan 2024: JHEP 0304 (2003) 031, hep-th/0303151. [24] Comments on Condensates in Non-Supersymmetric Orbifold Field Theories.
  10. Index of /user/mem/oldftp/HAY-LUCIDITY-SCIENCE-TALK

    www.damtp.cam.ac.uk/user/mem/oldftp/HAY-LUCIDITY-SCIENCE-TALK/
    2013-05-24 09:27. 327K. ... 2013-05-24 09:27. 138K.
  11. Professor Nigel Weiss FRS (1936-2020)

    www.damtp.cam.ac.uk/user/gio10/now.html
    22 Jul 2020: Professor Nigel Weiss FRS (1936-2020). Nigel Weiss, who died on 24 June 2020 after a fall at his home, was born on 16 December 1936, in South Africa.
  12. www.damtp.cam.ac.uk/user/mem/oldftp/lucidity-supplem.txt

    www.damtp.cam.ac.uk/user/mem/oldftp/lucidity-supplem.txt
    24 Oct 2016: Stuckness. the predecessor of all real understanding.'' [Near end of chapter 24, p.286 in the original edition.] Of course one can be getting on with other things, at least part
  13. 6 Jul 2020: action potential—which arises from nonlinear, excitabledynamics—analysis of the flashes [24] indicates a timecourse much like that of two coupled capacitors chargingand discharging on different timescales. ... exactly [24], thus enabling a global fit
  14. Microswimmers in vortices: dynamics and trapping

    www.damtp.cam.ac.uk/user/lauga/papers/214.pdf
    7 Dec 2023: KaðzÞ)ffiffiffiffiffip2z. re%z 1þ4a. 2 %18z. þð4a2 %1Þð4a2 %9Þ. 128z2! "; (24).
  15. clas

    www.damtp.cam.ac.uk/user/tong/dynamics/one.pdf
    13 Sep 2023: 2.4.1 Noether’s Theorem 24. 2.5 Applications 26. 2.5.1 Bead on a Rotating Hoop 26. ... kinetic energy,. T(t2)T(t1) =X. i. ZFexti dri. X. i 6=j. ZFij dri (1.24).
  16. Semidefinite approximations of matrix logarithm

    www.damtp.cam.ac.uk/user/hf323/talks/log_approx_slides.pdf
    4 May 2017: Thank you! 24/24. Conclusion. Approximation theory with convexity. Approach extends to other operator concave functions via their integralrepresentation (Löwner theorem). ... Thank you! 24/24.
  17. CV: Matthew J. ColbrookEMAIL: m.colbrook@damtp.cam.ac.ukWEBSITE:…

    www.damtp.cam.ac.uk/user/mjc249/pdfs/CV_MColbrook2024.pdf
    11 May 2024: 24. M.J. Colbrook, B. Roman, A.C. Hansen, How to compute spectra with error control, Physical Review Letters,2019.Cover highlight for issue.Prizes: Grade 1 Smith–Knight/Rayleigh–Knight
  18. Limits and Powers of Koopman LearningMatthew J. Colbrook* Igor ...

    www.damtp.cam.ac.uk/user/mjc249/pdfs/Koopman_foundations.pdf
    8 Jul 2024: man and von Neumann [21, 22], modern Koopman theory hasled to a renaissance of data-driven dynamical systems over thepast decade [7, 8, 23, 24, 25, 26, 27, 28].
  19. PowerPoint Presentation

    www.damtp.cam.ac.uk/user/mjc249/talks/CMStats.pdf
    18 Dec 2022: Slide 24. Slide 25. Slide 26. Slide 27.
  20. 1 Dec 2023: 24)]. 074001-14. IMBIBITION WITH SWELLING: CAPILLARY RISE IN. (a) (b) (c) (d). ... Fluids 17, 087104. (2005).[24] J. L. Sommer and A. Mortensen, Forced unidirectional infiltration of deformable porous media, J.
  21. J. Fluid Mech. (2017), vol. 829, pp. 89–111. c© ...

    www.damtp.cam.ac.uk/user/drh39/2017_stability3d.pdf
    1 Dec 2023: brar. y of. Mus. ic, o. n 24. Oct. 201. 7 at. ... ic, o. n 24. Oct. 201. 7 at. 14:. 02:3. 6, s.
  22. Part III - The Standard Model (Lent 2019)

    www.damtp.cam.ac.uk/user/cet34/teaching/SM/
    25 Mar 2019: There will be 24 lectures, 4 example sheets with associated examples classes and a revision class in Easter Term. ... Example sheet 4 (08/03/19). If you completed the attendance register in the lecture, you should have received an email about examples
  23. On two‐phase modeling of dewatering pulp suspensions

    www.damtp.cam.ac.uk/user/drh39/2021_pulp.pdf
    1 Dec 2023: 23 TMP (West Fraser) 112 580 1.59 36.4. 24 TMP (West Fraser) 229 390 1.50 35.6. ... found in Reference 24. At least four trials for each pulp suspension were.
  24. Part III Solitons and Instantons, Sheet Two Maciej Dunajski, ...

    www.damtp.cam.ac.uk/user/md327/SIsheet2.pdf
    7 May 2007: 24 = 1 and find its degree. By calculating. Tr((dg g1)3) at the point on S3 where x4 = 1, or otherwise deduce that the formula.
  25. PUBLICATIONS : NICHOLAS STEPHEN MANTON Research Papers 1. The ...

    www.damtp.cam.ac.uk/user/nsm10/Publications.pdf
    17 Jul 2020: 24. Classical and Quantum Dynamics of BPS Monopoles (with G.W. Gibbons), NuclearPhysics B274 (1986) 183-224. ... 3. LMS Annual General Meeting 19/11/04, London Mathematical Society Newsletter 333(2005) 23-24.
  26. covertex-epje150246.dvi

    www.damtp.cam.ac.uk/user/lauga/papers/112.pdf
    14 Nov 2019: This regularisationallows the use of simple, standard quadrature routines forall surface integrals in the regularised boundary integralequation [24]. ... Fauci, A. Medovikov, Phys. Fluids 17, 1. (2005).24. D.J. Smith, Proc.
  27. Preprint typeset in JHEP style - HYPER VERSION Michaelmas ...

    www.damtp.cam.ac.uk/user/tong/qft/qft.pdf
    20 Mar 2024: where Λµν satisfies. Λµσ ηστ Λντ = η. µν (1.24). For example, a rotation by θ about the x3-axis, and a boost by v < 1 along the x1-axis. ... The condition (1.24) for Λ to be a Lorentz transformation. becomes. (
  28. Halloween I

    www.damtp.cam.ac.uk/user/mem/papers/LHCE/halloween1.html
    19 Oct 2013: For example, when the TearDrop IP attack was first posted to the web, less than 24 hours passed before the Linux community had a working fix available for download.
  29. PHYSICAL REVIEW E 93, 023116 (2016) Flow-induced compaction of ...

    www.damtp.cam.ac.uk/user/drh39/2016_squishy.pdf
    1 Dec 2023: Received 24 June 2015; revised manuscript received 1 January 2016; published 24 February 2016). ... 24)] while the effective permeability decreases like H1(cf. (22)). The porosity also approaches an asymptotic profilewith φ0 0 as H.
  30. Part III Applications of Differential Geometry to Physics, Sheet ...

    www.damtp.cam.ac.uk/user/md327/PartIII_geom_2.pdf
    20 Jan 2020: 24 = 1 and find its. degree. By calculating Tr((dg g1)3) at the point on S3 where x4 = 1,or otherwise deduce that the formula.
  31. Dancing Volvox: Hydrodynamic Bound States of Swimming Algae Knut ...

    www.damtp.cam.ac.uk/user/gold/pdfs/waltzing.pdf
    10 Apr 2011: 24 APRIL 2009. 0031-9007=09=102(16)=168101(4) 168101-1 2009 The American Physical Society. ... 1) may be reduced, in rescaled coordinates r r=hand t tF=h2 with h R, to [24].
  32. J. Fluid Mech. (2024), vol. 978, R1, doi:10.1017/jfm.2023.849…

    www.damtp.cam.ac.uk/user/lauga/papers/222.pdf
    2 Jan 2024: 24, 313–358.PELLE, D.W., BROKAW, C.J., LESICH, K.A. & LINDEMANN, C.B. 2009 Mechanical properties of the.
  33. Nick_retirement_conference

    www.damtp.cam.ac.uk/user/mjc249/talks/Nick_NEP_mjc.pdf
    17 Aug 2023: Eval #Eval #. 24. Example: Ghost essential spectra. 𝑥. 𝜂(𝑥). truncated domain. ... Slide 24: Example: Instability. Slide 25: Example: Ghost essential spectra. Slide 26: Example: Ghost essential spectra.
  34. Fluid Mechanics of Mosaic Ciliated Tissues

    www.damtp.cam.ac.uk/user/gold/pdfs/mosaic.pdf
    2 Nov 2021: 1) aresurrounded by nonciliated cells: “goblet cells” that covermost of the tissue secreting mucus-like material [24],mosaically scattered small cells [25,26] secreting serotoninvesicles that modulate the ciliary beat frequency ... 24] S. Nagata,
  35. Stochastic Voronoi Tessellations as Models forCellular Neighborhoods…

    www.damtp.cam.ac.uk/user/gold/pdfs/Srinivasan_etal110324.pdf
    11 Mar 2024: 33, 958–972 (1962). [24] P. Rathie, On the volume distribution of the typi-cal Poisson–Delaunay cell, J.
  36. 2 Jan 2024: 1B), owing to the cell-to-cell variations inmetabolism and the number and morphology of flagella (24).Thanks to the large sample size of our experiments, we are able tomeasure the
  37. Lect08.dvi

    www.damtp.cam.ac.uk/user/na/PartII/Lect08.pdf
    31 Jan 2005: Theorem 2.24 (The bottom row ofAk1) Suppose that the conditions of Remark 2.23 are satisfied. ... If|λr| is tiny then usually the rightmost sum in (2.5) tends to zero rapidly ask increases, so the convergence result of Theorem 2.24 can be useful for
  38. Traveling waves are hydrodynamically optimal for long-wavelength…

    www.damtp.cam.ac.uk/user/lauga/papers/182.pdf
    14 Dec 2020: Fluid Mech. 24, 313 (1992).[17] J. S. Guasto, R. Rusconi, and R. ... Fluid Mech. 762,. (2015). 123101-9. ERIC LAUGA. [24] T. D. Montenegro-Johnson and E.
  39. www.sciencemag.org/cgi/content/full/325/5939/487/DC1 Supporting…

    www.damtp.cam.ac.uk/user/gold/pdfs/gears_SM.pdf
    21 May 2023: Goldstein. To whom correspondence should be addressed. E-mail: R.E.Goldstein@damtp.cam.ac.uk. Published 24 July 2009, Science 325, 487 (2009) DOI: 10.1126/science.1172667. ... Flagellar dynamics experiment. We analyzed 24 different cells and gathered
  40. Jerome A. NeufeldBP Institute, Bullard Laboratories,Madingley Road,…

    www.damtp.cam.ac.uk/user/jneufeld/JANeufeld_CV.pdf
    6 May 2019: Linden)6/24 lectures given on buoyancy-driven flows at the graduate levelPart III Mathematical Tripos, DAMTP, University of Cambridge. ... 737, 205–231. [24] S.S. Pegler, J.A. Neufeld, H.E. Huppert (2013) Topographic controls on gravity currents
  41. doi:

    www.damtp.cam.ac.uk/user/drh39/2013_thixo.pdf
    1 Dec 2023: in figures 11 and 12. Figure 11 shows profiles of samples with different ageing timesTage on inclines of 20; figure 12 shows profiles on slightly steeper inclines of 24.As a
  42. Swirling Instability of the Microtubule Cytoskeleton

    www.damtp.cam.ac.uk/user/lauga/papers/185.pdf
    17 Jan 2021: actin. Here, through a combination of direct computationson the coupled filament-flow problem [24] and studies of acontinuum theory for dense filament suspensions [28], weconfirm this hypothesis by showing the existence ... ffiffiffiffiffiffiffiffiffiffif
  43. Front-back asymmetry controls the impact of viscoelasticity on…

    www.damtp.cam.ac.uk/user/lauga/papers/191.pdf
    8 Jul 2021: While recent numerical work reported that the elasticstresses in the wake of rigid cylinders depend on the orientation of the cylinder relative to its velocity[24], the dependence of the drag ... symmetry breaking, Phys. Fluids 24, 103102 (2012).[19] J. A
  44. 1 The Expanding Universe‣ Cosmology by David Tong

    www.damtp.cam.ac.uk/user/tong/cosmo/cosmohtml/S1.html
    18 Oct 2021: a. (. t. ′. ). (1.24). This is the size of the observable universe. ... Indeed, mathematically it could be that the integral on the left-hand side of (1.24) does not converge at.
  45. Biofilm Growth under Elastic Confinement

    www.damtp.cam.ac.uk/user/gold/pdfs/biofilms.pdf
    29 Apr 2022: Rev. 24, 661 (2000). [5] A. van Leeuwenhoek, An abstract of a letter from Mr.Anthony Leewenhoeck at Delft, dated Sep. ... Fluid Mech.778, 335 (2015). [24] R. E. Gibson, R. L. Schiffman, and S.
  46. Hypergeometric function - series representation Claim: F (a, b; ...

    www.damtp.cam.ac.uk/user/bg268/Hypergeometric%20function%20as%20a%20series.pdf
    11 Mar 2020: Hypergeometric function - series representation. Claim:. F (a, b; c; z) =n=0. (a)n(b)n(c)n. zn. n!,. where (x)n = x(x 1).(x n 1), (x)0=1, is the Pochhammer symbol. The series is convergent in |z| < 1. The RSP at z = 1 prohibits the series
  47. Instability of an active fluid jet

    www.damtp.cam.ac.uk/user/lauga/papers/212.pdf
    9 Nov 2022: III and IV. The setup of downward jets is relevant to range of biological situations,including a falling plume of a cell suspension, i.e., bioconvection [22–24]. ... Pedley, Bioconvection, Fluid Dyn. Res. 37, 1 (2005).[24] M. A. Bees, Advances in
  48. 4.6 Monodromy: the reason for the logarithmic term in ...

    www.damtp.cam.ac.uk/user/bg268/Monodromy%20-%20need%20in%20log%20term.pdf
    11 Mar 2020: 4.6 Monodromy: the reason for the logarithmic term in the solution. Recall that forw′′ p(z)w′ q(z)w = 0, (1). in the vicinity of a RSP at z = 0 (WLOG - other points obtained by translation),there exist two linearly independent solutions of (1),
  49. The non-Gaussian tops and tails of diffusing boomerangs

    www.damtp.cam.ac.uk/user/lauga/papers/136.pdf
    29 May 2017: DOI: 10.1039/c6sm02649d. rsc.li/soft-matter-journal. Soft Matter. PAPER. Publ. ishe. d on. 24. ... L. Ekiel-Jeżewska and E. Wajnryb, J. Chem. Phys., 2015, 142, 214902.24 B.
  50. Collective stiffening of soft hair assemblies

    www.damtp.cam.ac.uk/user/lauga/papers/178.pdf
    6 Jul 2020: For apoint force located at a distance h above the flat bottom sur-face, and assuming no-slip boundary conditions, the flow canbe obtained using the hydrodynamic image method ... Like us, they interpreted theirresults using the models of Refs. [24,25].
  51. University of Cambridge, DAMTP: Quantum Fluids Laboratory Berloff

    www.damtp.cam.ac.uk/user/ngb23/lectures.html
    23 Nov 2017: LecturesSeptember 17-24, 2011 - Maratea (Italy). LecturesSao Paulo, Brazil, April 4-14, 2011.

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