Search

10 Nov 2010: n21 n. 22 n. 23 n. 24 = 1. Q = mn.

12 Aug 2010: n 0 1 2 3 4 12cjg<0 0.726(4) 0.86(1) 0.91(1) 0.93(1) 0.95(1) 12cjg>0 1.556(4) 1.24(1) ... This (incompressible) filled LL will appear as astep in the transverse density profile, as measured in situ orin an expansion measurement [24].

12 Aug 2010: function of a polarized filled LL times an additionalfactor describing the spin texture [24]. ... Finite Skyrmions of size K N=2 on thesphere have L S N=2 K [24].

12 Aug 2010: the relation between n andn remains linear [24,25], n n þ , with an offset. ... B. Laughlin, Phys. Rev. Lett. 59, 2095. (1987).[23] Time-reversal symm. is broken explicitly in the model.[24] F.

12 Aug 2010: 24 OCTOBER 2008. 0031-9007=08=101(17)=176803(4) 176803-1 2008 The American Physical Society. ... 24 OCTOBER 2008. 176803-2. CF-Fermi sea state is uniquely defined as filling two CFshells in each layer (at this flux, the pth CF shell has 2porbitals) [3,12]

12 Aug 2010: The data shown here arefor = 0.05 from Monte Carlo simulations on a lattice oflinear size L = 24, with the interaction summed over periodiccopies up to distance = 500 L.

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.

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.

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

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.