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3 Aug 2016: This system has beenwidely studied using QMC [24,29–31] and serves as an analogfor electrons in a conductor. ... Holzmann,. Phys. Rev. Lett. 97, 076404 (2006).[24] G. G. Spink, R.

5 Apr 2016: Mueller, Phys. Rev. A 78,. 033607 (2008).[24] X. Li, J. Kolorenč, and L.

15 Feb 2016: Remarkably, even atmean-field level the nontilted (θ = 0) system with an isotropicpotential is predicted to display an inhomogeneous stripe phase[24,25] that is robust to the inclusion of perturbative

21 Mar 2016: Slide 22. Slide 23. Slide 24. Slide 25. Slide 26. Slide 27.

15 Jun 2016: The nanomagnets have an elongated shape. with a length of 62 nm and a width of 24 nm, and are placedon the nodes of a two-dimensional kagome lattice with latticevectors ... 24] G. Möller and R. Moessner, Phys. Rev. Lett. 96, 237202 (2006).[25] U.

29 Sep 2016: 24). The right-hand side of Eq (24) shows, in particular, thatthe total magnetic flux, associated with the single vortex,. ... 2The second part of Eq(24) can be obtained by integrating both its sides over asmall area near origin.

3 Nov 2016: c _ c 0 _1 ( av) Ta ( 1 3 )' P - P AA2 ' aT p = Ac" K0 4Jl '. =_!__()' - 1 =_!_!()___!_L_. (24) K Ko AA Ko 4f.l Kad Ko AA Ko 4Jl

16 Apr 2016: Tale 23. Tricomi Equation and Crossing of Discontinuities. Tale 24. Hall Conductance Quantisation.

2 Jun 2016: Slide 22. Slide 23. Slide 24. Slide 25. Slide 26. Slide 27.

2 Jun 2016: 4 8 12 16 20 24 28 32. Linear size of BZ grid. ... Thermal and optical band gaps of diamond. 4 8 12 16 20 24 28 32.