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12 Aug 2010: 2Laboratoire de Physique Théorique et Modèles Statistiques, Université Paris-Sud, 91405 Orsay, France3Département de Physique, Laboratoire Pierre Aigrain, ENS, CNRS, 24 rue Lhomond, Paris F-75005, France. ... W. West,Phys. Rev. B 41, 7910 1990. 24 L.

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.

4 Apr 2010: 24. (a) Applying the Hubbard-Stratonovich transformation, the classical partition func-tion is given by.

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.

16 Aug 2010: SUHOV. satisfies. (1.24) y /. K(x,n). =1. ΛL(l)(x(l)),. then boxes Λ(n)L (x) and Λ. ... Set β = 1/2, α = 3/2 (cf.1.24). GivenE I and v Znd, the n-particle box ΛL(v) and the corresponding lattice box BL(v)are called.

16 Aug 2010: arX. iv:0. 907. 1459. v1 [. mat. h-ph. ] 9. Jul. 200. 9. Anderson localization in a two-particle. continuous model with an alloy-type external. potential. A. Boutet de Monvel1, V. Chulaevsky2, P. Stollmann3, Y. Suhov4. 1Institut de Mathématiques

16 Aug 2010: Instead, we refer the reader to the monographs [6, 20, 23], the surveys[18, 24] and the recent papers [2, 11] where such bibliography is presented. ... Progress in Math. Phys., vol. 20. Birkhäuser, Basel (2001)24. Veselić, I.: Existence and Regularity

28 Apr 2010: j=31. xij 1,. 14. j=11. xij 26. j=24. xij 1,. 30. ... 36.1FI 31.2FF 27.7HA 22.6HC 38.6MS 12.5MI 73.7BS. 51.7PI 18.6OJ 29.7QP 4.0GS 24.6SM 30.4SE 5.7TK = CARB;.

28 Apr 2010: j=31. xij 1,. 14. j=11. xij 26. j=24. xij 1,. 30. ... 36.1FI 31.2FF 27.7HA 22.6HC 38.6MS 12.5MI 73.7BS. 51.7PI 18.6OJ 29.7QP 4.0GS 24.6SM 30.4SE 5.7TK = CARB;.