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  2. D-Branes in Field Theory

    www.damtp.cam.ac.uk/user/tong/talks/cstring.pdf
    12 May 2006: trivially embed this in the non-abelian theory. B= B?0.( 0( ((q =q? ... B? q? SU(N)diag/SU(N 1) U(1) = CPN1. Simple Idea:. The strings can miss each other in the internal space.
  3. Shocking, the slow changes inHKM’s thin coat by HKM2 ...

    www.damtp.cam.ac.uk/user/hinch/talks/hkm3.pdf
    23 May 2006: Secularity condition – resonant sin(θ τ ) and cos(θ τ ). d. dT. (. A. B. ). =. (. a b. b a. )(. ... A. B. ). where. a = 81α/(1 144α2) and b = 3(5 72α2)/2(1 144α2).
  4. Bnew_BIT.dvi

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2006_04.pdf
    24 Nov 2006: b( ) b( ) b( ) = 0 nr rrrb( ) = 0 nr rrr. ... b( ) b( ) b( ) b( ) = 0 nr r rr rb( ) = 0 nr rrrr.
  5. N13LBa.dvi

    www.damtp.cam.ac.uk/user/rrh/notes/N13LBa.pdf
    22 May 2006: b) Multiplication by a scalar. Let A and B be n m matrices. ... Then by construction we clearly have. b (b c) =. i.
  6. A Class of Integrable Geodesic Flows on the Symplectic ...

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2006_02.pdf
    20 Apr 2006: for any S, S′ Sym(2p), A, A′ M(2p)d, and B, B′ Sym(d). ... Therefore,µa[R(N )]a,b [K(N )]a,bµb = 0, a, b = 1,. , n.
  7. This isa super vis or’ sco py ofth enote ...

    www.damtp.cam.ac.uk/user/sjc1/teaching/AandG/notes.pdf
    11 Nov 2006: OC. (2.2). (ii) Addition is commutative, i.e.a b = b a. ... b 0 = b , and from (2.3) 0 b = b.
  8. This isa super vis or’ sco py ofth enote ...

    www.damtp.cam.ac.uk/user/sjc1/teaching/NSTIB/notes.pdf
    28 Oct 2006: b) Suppose that B = 0; the vector field B(r) is said to be solenoidal. ... Then there exists anon-unique vector potential, A(r), such that. B = A.
  9. This isa super vis or’ sco py ofth enote ...

    www.damtp.cam.ac.uk/user/sjc1/teaching/NSTIB/Michaelmas/notes.pdf
    28 Oct 2006: b) Suppose that B = 0; the vector field B(r) is said to be solenoidal. ... Then there exists anon-unique vector potential, A(r), such that. B = A.

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