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11 - 19 of 19 search results for TALK:PC53 20 |u:www.tcm.phy.cam.ac.uk where 0 match all words and 19 match some words.

  1. Results that match 1 of 2 words

  2. Composite Fermion Theory for Bosonic Quantum Hall States on ...

    www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevLett.103.105303.pdf
    12 Aug 2010: J. Thomson Avenue, Cambridge CB3 0HE, United Kingdom2Laboratoire de Physique Théorique et Modèles Statistiques, Université Paris Sud, 91406 Orsay, France(Received 20 April 2009; revised manuscript received 13 August 2009; published ... R. Hofstadter

  3. Magnetic multipole analysis of kagome and artificial spin-ice dipolar …

    www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevB.80.140409.pdf
    12 Aug 2010: However, this is not yet quite the fullstory. In an appropriate low-temperature setting, there is inaddition an entropic interaction—which hence scales withT—between the monopoles.20,21 This interaction ... A. Moura-. Melo, and B. V. Costa, J. Appl.

  4. Paired composite-fermion wave functions G. Möller1 and S. H. ...

    www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevB.77.075319.pdf
    12 Aug 2010: J. Thomson Avenue, Cambridge CB3 0HE, United Kingdom. 2Bell Laboratories, Alcatel-Lucent, Murray Hill, New Jersey 07974, USAReceived 22 November 2007; revised manuscript received 18 December 2007; published 20 February 2008;. ... Lett. 99, 236807 2007.

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

    www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevB.79.245325.pdf
    12 Aug 2010: 0. 0.2. 0.4. 0.6. 0.8. 1. 0 5 10 15 20. ... 00.20.40.60.81. (c) HR. 0 2 4 6 8 10w/lB. 0. 0.02.

  6. 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: 37 4 1 20 0.48471 0.0523 0.0523 3 3 18 0.484675 0.0511 0.053244 2 24 0.48511 0.0503 0.0503 4 21 0.485257 ... 0.09394 0.12244 4 20 0.365011 0.02031 0.027616 5 15 0.449963 0.08374 0.11834 5 25 0.358001 0.01321 0.025117 6 18

  7. phmain

    www.tcm.phy.cam.ac.uk/~bds10/phase/tripans.pdf
    4 Apr 2010: 20. (a) Solving the Schrödinger equation, the wavefunctions obeying periodic boundaryconditions take the form ψm = eimθ, m integer, and the eigenvalues are given byEm = m2/2I.

  8. 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: We adopt the convention to measure energies in terms ofdensity corrected magnetic lengths 0 = 02S / N 20. ... 20 R. Morf, N. d’Ambrumenil, and B. I. Halperin, Phys. Rev.

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

    www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevB.79.125106.pdf
    12 Aug 2010: 12. where the electron density in each layer is such that n1 = n2= B / 20 with 0 = hc / e the flux quantum and B the mag-netic field. ... following, zi = xi iyi is the complex repre-sentation of the coordinates of particle i with the overbarrepresenting

  10. 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: J. Thomson Avenue, Cambridge CB3 0HE, United Kingdom. (Received 22 September 2010; published 20 December 2010). ... GW〉 =j. [cos θj sin θj eiφj â†j ]|0〉. (20). In the hard-core limit [as expressed by Eq.

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