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phmain
www.tcm.phy.cam.ac.uk/~bds10/phase/preface.pdf4 Apr 2010: However,strong interactions frequently induce transitions and lead to new equilibrium phases ofmatter. ... 3] R. P. Feynman, Statistical Mechanics, Benjamin, New York, (1972). Another classic textby Feynman which covers the basic concepts. -
phmain
www.tcm.phy.cam.ac.uk/~bds10/phase/topol.pdf4 Apr 2010: Such cases admitthe existence of a new type of continuous phase transition driven by the proliferation oftopological defects. -
collection_45.ps.CFs1-1
www.tcm.phy.cam.ac.uk/~nrc25/SEMINARS/frustrated_mft_tsinghua.pdf28 Sep 2010: Are there new strongly correlated phases on the lattice for n nv 1? ... 1n. Do these new phases describe the exact groundstates? Numerical Methods. • -
phmain
www.tcm.phy.cam.ac.uk/~bds10/phase/rg.pdf4 Apr 2010: This procedure has transformed from a set of parameters S = {K, t, h} to a new set. ... Thus one caninvestigate which interactions will lead to new universality classes and which will not. -
Composite Fermion Theory for Bosonic Quantum Hall States on ...
www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevLett.103.105303.pdf12 Aug 2010: To our knowledge, there has been no previousevidence for new FQHE states induced by a lattice poten-tial. ... Heinonen (World. Scientific, New Jersey, 1998), for a review of CF’s.[13] N. -
Paired composite-fermion wave functions G. Möller1 and S. H. ...
www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevB.77.075319.pdf12 Aug 2010: E. Prange and S. M. Girvin Springer-Verlag, New York, 1987. 13 P. ... G. de Gennes, Superconductivity of Metals and Alloys Ben-jamin, New York, 1966. -
Paired Composite Fermion Phase of Quantum Hall Bilayers at ...
www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevLett.101.176803.pdf12 Aug 2010: 1] Perspectives in Quantum Hall Effects S. Das Sarma and A.Pinczuk (Wiley, New York, 1997). ... 9] P. G. de Gennes, Superconductivity of Metals and Alloys(Benjamin, New York, 1966). -
phmain
www.tcm.phy.cam.ac.uk/~bds10/phase/tripans.pdf4 Apr 2010: As a consequence, since the statistical weight of new con-figuration, W ′[m′] is the sum of the weights W [m] of old ones, the partitionfunction is preserved. ... 2. )|m′(q′)|2 zh m′(0). As a result of the RG procedure the set of parameters {K, -
Composite fermions in a negative effective magnetic field: A ...
www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevB.72.045344.pdf12 Aug 2010: Gunnar Möller1,2 and Steven H. Simon11Bell Laboratories, Lucent Technologies, Murray Hill, New Jersey 07974, USA. ... Note that our new trial wavefunctions show an excellent reproduction of the increasingly non-trivial features as = 1 / 2 is approached. -
PHYSICAL REVIEW A 82, 063625 (2010) Condensed ground states ...
www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevA.82.063625.pdf30 Dec 2010: This “gauge transfor-mation” leaves the fluxes (1) unchanged [53,54], which aretherefore said to be “gauge-invariant.” The new Hamiltonian(with A′ij in place of Aij ) can be brought -
Fractional quantum Hall state at � = 14 in ...
www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevB.79.245325.pdf12 Aug 2010: Fractional quantum Hall state at = 14 in a wide quantum well. Z. Papić,1,2 G. Möller,3 M. V. Milovanović,2 N. Regnault,4 and M. O. Goerbig11Laboratoire de Physique des Solides, Université Paris-Sud, CNRS UMR 8502, F-91405 Orsay Cedex, France. -
Trial wave functions for � = 12 +12 quantum ...
www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevB.79.125106.pdf12 Aug 2010: 2Bell Laboratories, Alcatel-Lucent, Murray Hill, New Jersey 07974, USA3Department of Physics, California State University–Los Angeles, Los Angeles, California 90032, USA. ... Diagonalizing the es-timator Hd yields a new set of variational
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