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4 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.

4 Apr 2010: Such cases admitthe existence of a new type of continuous phase transition driven by the proliferation oftopological defects.

28 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. •

4 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.

12 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.

12 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.

12 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).

4 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,

12 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.

30 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