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  2. D-Branes in Field Theories

    www.damtp.cam.ac.uk/user/tong/talks/dbrane.pdf
    23 Feb 2006: MotivationsTo understand the relationship between string and gauge theories for semi-classical, magnetic strings.To develop a new perspective on soliton scattering in field theory.
  3. D-Branes in Field Theory

    www.damtp.cam.ac.uk/user/tong/talks/cstring.pdf
    12 May 2006: They would provide a window onto new microscopicphysics that is not accessible in terrestrial experiments.
  4. caqcd.dvi

    www.damtp.cam.ac.uk/user/tong/talks/caqcd.pdf
    12 Sep 2006: qi eiσqi coincides with the gauge action and does not lead to any new physical state. ... action qi eiσqi with qi1 e. iσqi1 does now sweep out a new physical configuration.
  5. Moment-free numerical approximation of highly oscillatory…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2006_09.pdf
    27 Nov 2006: We begin with the derivation of a new asymptotic expan-sion, which has the property that the accuracy improves as the frequency of oscillationsincreases. ... We first present the Iserles and Nørsett expansion, to motivate the methodologybehind the new
  6. Cambridge NA Report NA2006/01 Joint Diagonalization on the Oblique ...

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2006_01.pdf
    24 Jan 2006: In a second step, an orthogonal matrix U issought that diagonalizes the new target set {W̃ T C1W̃ ,. , W̃. T C1W̃ }. This yields a separatingmatrix W = W̃ U ; see, for example, ... Com94] Pierre Comon, Independent component analysis, A new concept?,
  7. Numerical approximation of vector-valued highly oscillatory integrals …

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2006_06.pdf
    26 Jul 2006: the requisite order of error. We now show that this new Levin-type method is equivalent to the originalLevin-type method. ... Thus. D̄(P D̄1W D̄G)D̄1 = P W G,. It follows that, where B2 = P D̄1W D̄G is the matrix associated with the new Levin-type
  8. N13LBb.dvi

    www.damtp.cam.ac.uk/user/rrh/notes/N13LBb.pdf
    22 May 2006: we can form a new sequence S1,S2,S3,. , where. Sn = u1 u2. ... uk} in any manner to form a new series. The two series have the same sum.Not true for a divergent series.
  9. A Class of Integrable Geodesic Flows on the Symplectic ...

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2006_02.pdf
    20 Apr 2006: a new geodesic flow thatis not of rigid body type on the Lie group Sp(nR). ... Borisov, A.V., S.I. Mamaev, and V.V. Sokolov [2001], A new integrable case onso(4), Dokl.
  10. DAMTP 2006/NA03 Fast evaluation of polyharmonic splines in three ...

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2006_03.pdf
    31 Aug 2006: April, 2006. 1Department of Mathematics and Statistics, University of Canterbury, Private Bag 4800,Christchurch 8020, New Zealand. ... Anderson and C. Greengardeds, Lecture Notes in Mathematics 1360, Springer-Verlag, New York, 1988.
  11. berloff.dvi

    www.damtp.cam.ac.uk/user/ngb23/publications/warwick.pdf
    7 Sep 2006: Similarly to the three-dimensional case, in addi-tion to the VP-VP, VP-RP, and RP-RP complexes, there are new classes ofsolitary waves that have no analog in

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