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

    www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevB.79.125106.pdf
    12 Aug 2010: 3 numerical operations, whereas the wave func-tions from Ref. 34 require explicit antisymmetrization, anoperation that requires much computation power with an op-eration count scaling exponentially with the system size.
  3. Paired Composite Fermion Phase of Quantum Hall Bilayers at ...

    www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevLett.101.176803.pdf
    12 Aug 2010: Inbrief, we find a second order phase transition near d 1from the CF-BCS phase at larger d, which has zero 111order parameter (OP), to a phase with nonzero 111 OP ... mix with composite bosons (CB’s) and the presenceof CB’s yields nonzero 111 OP.
  4. 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: The loop pattern op-timizes the local dipolar energy, in that each dimer is ori-ented favorably with respect to its four nearest neighbors anddue to the convergent nature of the
  5. 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: As usual, the fermion op-erators have anticommutation relations ci. † , cj = i, j.

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