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  1. Results that match 2 of 3 words

  2. Diagonalising Infinite-Dimensional Operators 2mmComputing spectral…

    www.damtp.cam.ac.uk/user/mjc249/talks/mjc_AustMS
    10 Dec 2020: 24] McMullen, C. (1987) "Families of rational maps and iterative root-finding algorithms." Annals of mathematics 467-493. ... 1.29:. 1.28:. 1.27:. 1.26:. 1.25:. 1.24:. 1.23:. 1.22:. 1.21:. 1.20:. 1.19:.
  3. 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
  4. 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),
  5. 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.
  6. 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.
  7. 4. Non-Abelian Quantum Hall States The vast majority of ...

    www.damtp.cam.ac.uk/user/tong/qhe/four.pdf
    5 Oct 2020: 12, 34) (13, 24) = (z1 z2)21423. Then, using the definition of the Pfaan (4.3), we have. ... Pf(13),(24)(z) = A(13, 24). z1 z2(13, 24). z3 z4. = A(12, 34) (z1 z2)21423.
  8. Moments and Angular Spectrum for Rough Surface Scattering At Grazing…

    www.damtp.cam.ac.uk/user/ms100/PAPERS/JASA95stats.pdf
    4 Feb 2020: From Eqs. (24) and (25) this becomes. Mn( O,x;,O ) = ( - 1 )ne ilmsx. ... a• = - 2ikh(x)/2 0(/23) (47). and similarly from (13) and (24),.
  9. 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].
  10. 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.
  11. Gauge/Gravity Duality Mathematical Tripos, Part IIIAron C. Wall…

    www.damtp.cam.ac.uk/user/aw846/AdSCFT/GGexamples_1.pdf
    1 May 2020: 23). ds2 = dT 2 cos(T)2[dr2 sinh(r)2d2D2. ]; (24). 5. ... Note that (24) looks like a recollapsing FLRW cosmology with k = 1 (negativecurvature), but the apparent ‘Big Bang’ and ‘Big Crunch’ singularities areactually just coordinate artifacts.

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