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15 Jun 2010: 0.1. 0.2. 0.3. 0.4. 0.1. 0.2. 0.3. 0.4. 0.0 0.2 0.4 0.6 0.8 1.0 1.20.0.

11 Sep 2010: representationχ(r). r J1(. r), (20). but we, really, do not need this.

12 Aug 2010: jgj23@vFn‘20lnFnkBT. : (4). Identical divergences occur in both particle-particle (p-p)and particle-hole (p-h) diagrams [20] and in diagrams ofhigher orders. ... 20] A. A. Abrikosov, J. Low Temp. Phys. 2, 37 (1970); 2, 175(1970).

4 Apr 2010: 20 CHAPTER 2. GINZBURG-LANDAU PHENOMENOLOGY. where Sd = 2πd/2/(d/2 1)! denotes the total d-dimensional solid angle.5 Hence〈[θ(x) θ(0)]2. 〉=

10 Nov 2010: sky. 2Q. Hs. 2Q. Es. 0. blue: Nφ=20 (σ=4). (a) N=12, ν=5/2, w=3λ.

12 Aug 2010: 20. 40. 60. 80. %. Type I Type II Type III Type IV. ... 0,. 0 1 2T [J]. -40. -20. 0. 0 1 2T [J].

16 Jun 2010: OutlineSuperfluid vs. Condensate FractionOptically Induced Gauge Potentials. Superfluid FractionSummary. Three-level system 0@ 2M (k k)2 δ R/2 0R/2 2M k2 R/20 R/2. ... g n̄ = 5kHz. 0 0.5 1 1.5 20. 0.005. 0.01.

12 Aug 2010: 2QH. s2Q. Es. 0. blue: Nφ=20 (σ=4). (a) N=12, ν=5/2, w=3λ. ... B 66, 075408 (2002). [20] A. Wójs, Phys. Rev. B 80, 041104(R) (2009).[21] M.

28 Sep 2010: Condensate depletion up to 50%. 0 10 20 30 40 50 60 70U [t].

12 Aug 2010: The varia-tional CF-BCS wave function for N 20 electrons wasobtained using an energy minimization technique [14]. ... eBCS. - eHund. , N=20. 0 0.05 0.1 0.15 0.2N. -1.

12 Aug 2010: J. Thomson Avenue, Cambridge CB3 0HE, United Kingdom2Laboratoire de Physique Théorique et Modèles Statistiques, Université Paris Sud, 91406 Orsay, France(Received 20 April 2009; revised manuscript received 13 August 2009; published ... R. Hofstadter

12 Aug 2010: However, this is not yet quite the fullstory. In an appropriate low-temperature setting, there is inaddition an entropic interaction—which hence scales withT—between the monopoles.20,21 This interaction ... A. Moura-. Melo, and B. V. Costa, J. Appl.

12 Aug 2010: J. Thomson Avenue, Cambridge CB3 0HE, United Kingdom. 2Bell Laboratories, Alcatel-Lucent, Murray Hill, New Jersey 07974, USAReceived 22 November 2007; revised manuscript received 18 December 2007; published 20 February 2008;. ... Lett. 99, 236807 2007.

12 Aug 2010: 0. 0.2. 0.4. 0.6. 0.8. 1. 0 5 10 15 20. ... 00.20.40.60.81. (c) HR. 0 2 4 6 8 10w/lB. 0. 0.02.

12 Aug 2010: 37 4 1 20 0.48471 0.0523 0.0523 3 3 18 0.484675 0.0511 0.053244 2 24 0.48511 0.0503 0.0503 4 21 0.485257 ... 0.09394 0.12244 4 20 0.365011 0.02031 0.027616 5 15 0.449963 0.08374 0.11834 5 25 0.358001 0.01321 0.025117 6 18

4 Apr 2010: 20. (a) Solving the Schrödinger equation, the wavefunctions obeying periodic boundaryconditions take the form ψm = eimθ, m integer, and the eigenvalues are given byEm = m2/2I.

12 Aug 2010: We adopt the convention to measure energies in terms ofdensity corrected magnetic lengths 0 = 02S / N 20. ... 20 R. Morf, N. d’Ambrumenil, and B. I. Halperin, Phys. Rev.

12 Aug 2010: 12. where the electron density in each layer is such that n1 = n2= B / 20 with 0 = hc / e the flux quantum and B the mag-netic field. ... following, zi = xi iyi is the complex repre-sentation of the coordinates of particle i with the overbarrepresenting

30 Dec 2010: J. Thomson Avenue, Cambridge CB3 0HE, United Kingdom. (Received 22 September 2010; published 20 December 2010). ... GW〉 =j. [cos θj sin θj eiφj â†j ]|0〉. (20). In the hard-core limit [as expressed by Eq.