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11 - 20 of 1,563 search results for katalk:za33 24 where 0 match all words and 1,563 match some words.

  1. Results that match 1 of 2 words

  2. Fractional quantum Hall state at � = 14 in ...

    www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevB.79.245325.pdf
    12 Aug 2010: J. Thomson Avenue, Cambridge CB3 0HE, United Kingdom. 4Laboratoire Pierre Aigrain, Ecole Normale Supérieure, CNRS, 24 rue Lhomond, F-75005 Paris, FranceReceived 1 April 2009; published 23 June 2009.

  3. Trial wave functions for � = 12 +12 quantum ...

    www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevB.79.125106.pdf
    12 Aug 2010: 4 0.99082. 9 24 84 5 104 0.98816. 10 27 319 6 104 0.984311 30 1160 7 104 0.98428 16 8 4 105 0.99872.

  4. Composite fermions in a negative effective magnetic field: A ...

    www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevB.72.045344.pdf
    12 Aug 2010: 2Laboratoire de Physique Théorique et Mécanique Statistique, 91406 Orsay, FranceReceived 24 February 2005; published 19 July 2005. ... 498045 0.0531 0.065141 5 24 0.49761 0.0484 0.0584 7 18 0.497976 0.0502 0.0642 0.49682 0.0428 0.0608 0.49722 0.0413

  5. PHYSICAL REVIEW A 82, 063625 (2010) Condensed ground states ...

    www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevA.82.063625.pdf
    30 Dec 2010: 2This was also found in the studies of Ref. [24] (D.K.K. ... not gauge-invariant. Under the transformation (24) the single-particle density operator becomes.

  6. Pairing in ultracold Fermi gases in the lowest Landau ...

    www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevA.79.033609.pdf
    12 Aug 2010: 2Laboratoire de Physique Théorique et Modèles Statistiques, Université Paris-Sud, 91405 Orsay, France3Département de Physique, Laboratoire Pierre Aigrain, ENS, CNRS, 24 rue Lhomond, Paris F-75005, France. ... W. West,Phys. Rev. B 41, 7910 1990. 24 L.

  7. Tale 6 The Kramers’ Phase and Laplace’s Method The ...

    www.tcm.phy.cam.ac.uk/~dek12/tales/Tale-06.pdf
    11 Sep 2010: y′′ x2y = λy (24). The asymptote of its solution at |x| is. ... x2. 2. ). (26). into Eq (24) leads to the following equation for Hλ(x) :. {. d2. dx2+ 2x. d. dx λ 1. }. Hλ(x) = 0 (27).

  8. NATURAL SCIENCES TRIPOS Part II Wednesday 13 January 2010 ...

    www.tcm.phy.cam.ac.uk/~cc726/TP1/ExamFiles/exam10sol.pdf
    25 Jan 2010: g. aB , ω2B = 12ga. l2(AB). so. ω2B = 12gal2B 24. ... 11. g2. l2ω2B ,. ω4 12gal2ω2 24. 11. g2. l2= 0 ,. and therefore. ω2 = 6ga. l2. 1. 1 2. 33. l2.

  9. phmain

    www.tcm.phy.cam.ac.uk/~bds10/phase/tripans.pdf
    4 Apr 2010: 24. (a) Applying the Hubbard-Stratonovich transformation, the classical partition func-tion is given by.

  10. phmain

    www.tcm.phy.cam.ac.uk/~bds10/phase/gl.pdf
    4 Apr 2010: Phase Transitions and Collective Phenomena. 24 CHAPTER 2. GINZBURG-LANDAU PHENOMENOLOGY. Using Eq. ... 32 1.24 0.63Superconductors 0 1/2 1 1/2.

  11. arX iv:1 004. 1300 v1 [ mat h-ph ] ...

    www.statslab.cam.ac.uk/~yms/BCSS3.pdf
    16 Aug 2010: SUHOV. satisfies. (1.24) y /. K(x,n). =1. ΛL(l)(x(l)),. then boxes Λ(n)L (x) and Λ. ... Set β = 1/2, α = 3/2 (cf.1.24). GivenE I and v Znd, the n-particle box ΛL(v) and the corresponding lattice box BL(v)are called.

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