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  2. Riemann-Hilbert problems, Toeplitz operators and ergosurfaces M.…

    https://api.newton.ac.uk/website/v0/events/preprints/NI23031
    Riemann-Hilbert problems, Toeplitz operators. and ergosurfaces. M. Cristina Câmara and Gabriel Lopes Cardoso. Center for Mathematical Analysis, Geometry and Dynamical Systems,Department of Mathematics, Instituto Superior Técnico, Universidade de
  3. Notices by Faculty Boards, etc. - Cambridge University Reporter 6354

    https://www.reporter.admin.cam.ac.uk/reporter/2013-14/weekly/6354/section4.shtml
    2 Jul 2014: A31. Ancient India II: Early historic cities of South Asia. A32. ... Ancient India II: Art and architecture of ancient India. A33. Ancient South America.
  4. On the Solvability Complexity Index hierarchy, the computational…

    www.damtp.cam.ac.uk/user/mjc249/talks/SCI_colbrook.pdf
    21 Aug 2019: a21 a22 a23. a31 a32 a33. Want to compute spectrum (generalisation of eigenvalues).
  5. Asymptotic theory of hydrodynamic interactions between slender…

    www.damtp.cam.ac.uk/user/lauga/papers/196.pdf
    10 Sep 2021: PHYSICAL REVIEW FLUIDS 6, 074103 (2021). Asymptotic theory of hydrodynamic interactions between slender filaments. Maria Tătulea-Codrean and Eric Lauga. Department of Applied Mathematics and Theoretical Physics, University of Cambridge,Cambridge
  6. Hex.dvi

    https://www.dpmms.cam.ac.uk/~twk/Hex.pdf
    8 Aug 2021: . a11 a12 a13a21 a22 a23a31 a32 a33. .  = det. ... . . a11 a12 a13a21 a22 a23a31 a32 a33. . .
  7. Asymptotic theory of hydrodynamic interactions between slender…

    www.damtp.cam.ac.uk/user/mt599/papers/2021-prf.pdf
    10 May 2022: Asymptotic theory of hydrodynamic interactions between slender. filaments. Maria Tătulea-Codrean and Eric Lauga. Department of Applied Mathematics and Theoretical Physics,. University of Cambridge, Cambridge CB3 0WA, United Kingdom. (Dated: July 7,
  8. Hölder regularity of the pressure for weak solutions ofthe ...

    https://api.newton.ac.uk/website/v0/events/preprints/NI21027
    s. ]). 1. b. [. s. (b. [a31. f. σ1+ a32. ... f. σ2+ a33. f. s. ]), (2.14). where (v1,v2,v3) are the components of the vector v in the coordinates (σ1,σ2,s).We recall that we showed earlier that
  9. IET IAM paper_info futureproofing_v7.4

    https://www-smartinfrastructure.eng.cam.ac.uk/system/files/documents/3.09Masood0086FinalPaper.pdf
    information. A32. Identify technical and organisational challenges that prevent meeting the retention. ... requirements. A33. Evaluate and prioritise risks involved in the challenges. A34.
  10. ∗-COMPATIBLE CONNECTIONS IN NONCOMMUTATIVERIEMANNIAN GEOMETRY E.J.…

    https://api.newton.ac.uk/website/v0/events/preprints/NI09036
    AB =.  A11 B A12 B A13 BA21 B A22 B A23 BA31 B A32 B A33 B.
  11. Supersymmetric extensions of Schrödinger-invariance Malte Henkela,b…

    https://api.newton.ac.uk/website/v0/events/preprints/NI06007
    Supersymmetric extensions of Schrödinger-invariance. Malte Henkela,b and Jérémie Unterbergerc. aLaboratoire de Physique des Matériaux,1 Université Henri Poincaré Nancy I,B.P. 239, F – 54506 Vandœuvre-lès-Nancy Cedex, France. bIsaac

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