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11 Jan 2017: X = tp 12t2[p,k] 1. 6t3[k, [p,k]] t4. (1. 24[p.[p, [p.k]]] 1. ... 24[k, [k, [p,k]]]. )(20)265. t5(. 7. 360[k, [p, [p, [p,k]]]] 1.

13 Mar 2017: 2′. n=0 fn d. 2. 2(U α β). (24). Finally, to determine U , we impose that the force on the torus must vanish. ... 100 100.5 101. 0.24. 0.245. 0.25. s0. |U|. 0.8 1 1.2Concentration.

4 May 2017: Thank you! 24/24. Conclusion. Approximation theory with convexity. Approach extends to other operator concave functions via their integralrepresentation (Löwner theorem). ... Thank you! 24/24.

4 Sep 2017: One can also combine MBL with the above quantumorders to obtain MBL phases in which individual highly ex-cited eigenstates show SSB, SPT, or topological order [19–24].

8 Nov 2017: At large times, clearlythe time-independent terms in (24) can be neglected comparedto the logarithmic term. ... J. E 29, 27 (2009).[24] J. Brady, J. Fluid Mech. 667, 216 (2011).[25] B.

9 Jul 2017: I; Xi. miR2. 1. hðiÞ;i. 1. ðiÞ;. 1. þ ðĥ2i; ĥi2;Þ > 0; (24). ... Phys. 5, 56 (2003).[24] I. Bloch, J. Dalibard, and W. Zwerger, Rev.

3 Oct 2017: ζ0. ψ(h,ζ,ξ) dξ dζ = 0, (2.24). lending an extra power of h to terms featuring Λ [ψ]a,b(h).

20 Jan 2017: A 24.6 25.5 1.403 4 — 5.3 10.7 5.2B 43.6 24.7 1.4 4.7 20 6.3 13.3 3.4C 36.6

11 Mar 2017: In this regime, MBL is expected to persist even in the presence of long-range interactions23,24. ... Phys. Rev. B 92, 104428 (2015). 24. Yao, N. Y. et al.

3 Dec 2017: Received 16 July 2015; revised manuscript received 24 March 2016; published 12 May 2016). ... 24)See the right panel of Fig. 4. Again, F [rf ](ω) denotes theFourier amplitude at frequency ω.