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1 - 10 of 51 search results for katalk:za33 24 |u:geometry.mrao.cam.ac.uk where 0 match all words and 51 match some words.

  1. Results that match 1 of 2 words

  2. Applications of Conformal Geometric Algebra inComputer Vision and…

    geometry.mrao.cam.ac.uk/wp-content/uploads/2015/02/05jl_china.pdf
    19 Feb 2015: Fig. 4. The Stanford Bunny[24] distorted by the same rotors. Applications of Conformal Geometric Algebra 343. ... In Proceedings of the IFIPTC5/WG5.10 DEFORM’2000 Workshop and AVATARS’2000 Workshop on De-formable Avatars, pages 24–34.

  3. arX iv:g r-qc /020 9090 v2 1 Mar 200 ...

    geometry.mrao.cam.ac.uk/wp-content/uploads/2015/02/05BoundStatesPRD.pdf
    19 Feb 2015: u1 7 u1eiEα u2 7 u2eiEα (24). 5. which together ensure that equation (22) is still satisfied. ... In this regime the spectrum will. 24. be quite different to that of the hydrogen atom.

  4. arXiv:gr-qc/9910099v3 31 Jan 2000

    geometry.mrao.cam.ac.uk/wp-content/uploads/2015/02/00NewKerr.pdf
    19 Feb 2015: ni =1. 2ρ2(r2 a2, (r2 a2). (. 2Mr(r2 a2))1/2. , 0, a) (24).

  5. arXiv:gr-qc/0211070v1 21 Nov 2002

    geometry.mrao.cam.ac.uk/wp-content/uploads/2015/02/03Axissymmetric1.pdf
    19 Feb 2015: 24). The coframe derivatives satisfy a set of bracket identities. [Li,Lj] = cijkLk.

  6. Rotating astrophysical systems and a gauge theoryapproach to gravity…

    geometry.mrao.cam.ac.uk/wp-content/uploads/1997/01/97Erice_Rotating.pdf
    16 Feb 2015: tension. The tension in this disk has precisely the form expected. 24.

  7. anl_paper_new.dvi

    geometry.mrao.cam.ac.uk/wp-content/uploads/2015/02/05anl_china.pdf
    19 Feb 2015: This pins down fto a combination of rotation and dilatation. To see how (23) is equivalent to (24) is also easy. ... As an example, choose δ = 2.24, and mapthe circle r = 1/4 again.

  8. Grassmann Calculus, Pseudoclassical Mechanicsand Geometric Algebra…

    geometry.mrao.cam.ac.uk/wp-content/uploads/2015/02/grass_jmp.pdf
    5 Feb 2015: 24. should look at the equations of motion for the fiducial frame σi = h1(ei),. ... andu = g1(u), (4.24). are conserved. This follows from. u = Enω (4.25)u = Enω.

  9. Classical and Quantum Dynamics in a Black Hole Background

    geometry.mrao.cam.ac.uk/wp-content/uploads/2015/02/MIT2.pdf
    22 Feb 2015:    0. MIT2 2003 24. Spacetime Vector Derivative• Define spacetime vector derivative. •

  10. In: J. Math. Phys., 34 (8) August 1993 pp. ...

    geometry.mrao.cam.ac.uk/wp-content/uploads/2015/02/LieGroupsAsSpinGroups.pdf
    5 Feb 2015: B Q) Q = 2(QB B) (4.24). 11. for any bivector B. ... eiSn eiRn , (5.24)eiSn Rnei , (5.25). 18. and the latter combines with Eq.

  11. arXiv:quant-ph/0106055v1 11 Jun 2001

    geometry.mrao.cam.ac.uk/wp-content/uploads/2015/02/02Parker_Entanglement.pdf
    19 Feb 2015: 0〉 1 and |1〉 Iσ2. (24). In this way ψ sits inside the space spanned by {1,Iσk}, (k = 1, 2, 3).

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