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11 Sep 2010: y′′ x2y = λy (24). The asymptote of its solution at |x| is. ... x2. 2. ). (26). into Eq (24) leads to the following equation for Hλ(x) :. {. d2. dx2+ 2x. d. dx λ 1. }. Hλ(x) = 0 (27).

25 Jan 2010: g. aB , ω2B = 12ga. l2(AB). so. ω2B = 12gal2B 24. ... 11. g2. l2ω2B ,. ω4 12gal2ω2 24. 11. g2. l2= 0 ,. and therefore. ω2 = 6ga. l2. 1. 1 2. 33. l2.

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

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]

4 Apr 2010: Phase Transitions and Collective Phenomena. 24 CHAPTER 2. GINZBURG-LANDAU PHENOMENOLOGY. Using Eq. ... 32 1.24 0.63Superconductors 0 1/2 1 1/2.

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: 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

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.