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3 Aug 2016: A commonapproach in the literature [20–27] is to combine both u and pterms to give a composite Jastrow function. ... J. Conduit, Phys. Rev. B 92, 075106 (2015).[20] G. J. Conduit, A.

5 Apr 2016: kFrckFR. 100. 10. 20. 0 0.5 1. V/|E. b|. kFr. FIG. ... Rev. Lett. 92, 120403(2004). [20] C. Chin, R. Grimm, P. Julienne, and E.

15 Feb 2016: 20 sin. 2 θ (1 94 sin4 θ ) for small θ.

21 Mar 2016: Slide 16. Slide 17. Slide 18. Slide 19. Slide 20. Slide 21.

12 Aug 2016: Frequent 15:20 Bhavin Khatri MRC National Institute of Medical Research Emergent complexity, speciation and a simple genotype phenotype map15:50 Coffee. ... of biological individuality15:20 Matthew Turner University of Warwick Non-local models of

31 Aug 2016: 0.2. 0.4. 0.6. 0.8. 1.0. ρ j. (c). 1 10 20. ... e). 1 10 20. 1. 10. 20. j. i(f). 0. 0.2.

15 Jun 2016: relation to thepinch-point singularities in both in-field [20,21] and zero-fieldspin ice pyrochlores [22]. ... Inparticular, the observation of pinch points in neutron scatteringpatterns has provided direct experimental evidence for a field-induced and

13 Oct 2016: 2π)d1. (α s2k2)2(20). Eq (20) expresses the leading correction to specific heatbeyond the limits of the mean field approximation. ... is called the upper critical dimension dc. At d > 4, theintegral in the right-hand side of Eq (20) converges even atα

29 Sep 2016: layered structure is. F = B2cal σnshl. a. (20). The minimum of this free energy is reached at the equilib-.

4 Oct 2016: α. aα2η2α, aα > 0. (20). At T = Tc, one of rigidities aα vanishes (say, for α = 1).Therefore, at T < Tc the rigidity a1 < 1, which makessymmetric phase unstable with respect ... deformation η1. In order to determine the amplitude ofabove