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15 Feb 2017: A , [B, [A , C ]]] = 0, [B, [A , [B, G ]]] = 0, [C , [A , [C , E ]]] = 0, (3.24)[A , [B, [A , E ]]] = 0, [B, [B, [B, C ]]] = 0, [C , [A , [C , G ]]] =

9 Jul 2017: Thus we have a time quasicrys-tal, in analog of a conventional spatial quasicrystal [24].The persistent rotation of trapped ions can be detected. ... 24] D. Levine and P. J. Steinhardt, Phys. Rev. B 34, 596(1986).

13 Oct 2017: ON THE STABLE SAMPLING RATE FOR BINARY MEASUREMENTS AND WAVELETRECONSTRUCTION. A. C. HANSEN AND L. TERHAAR. ABSTRACT. This paper is concerned with the problem of reconstructing an infinite-dimensional signal from alimited amount of linear

19 Dec 2017: y(J) (r I,t l,r2,t2,r3,t3). == ( - i) (T{n(rl,tl)n (r2,t2)n(r3,t3)}), (2.24 ) as the time-order expectation of the electron ... This in tum gives. 24. k = 81T,Be2A i 3XI-'(0), (5.8).

4 Sep 2017: β. IL. βI. Lβ. IL. βI. Lβ. IL. β. β = 0.44ν = 1.24. ... 24] We note that this phase is related to the π spin glass phase[10,13] and is referred to as a Floquet time crystal in [11].

13 Feb 2017: Askey. 24. Jin, S., Markowich, P. & Sparber, C. (2011), ‘Mathematical and computational meth-ods for semiclassical Schrödinger equations’, Acta Numer.

29 Jul 2017: 24. 2.4 Canonical connections. 31. 2.4.1 The Ξ-connection. 32. 2.4.2 The torsion Ξ-connection. ... in [24]. Note that theorem 2.3.3 is a different construction of 4n-dimensional moduli spaces to.

1 Dec 2017: T(η,ω,X) = TabcηaωbXc. (2.24). This formula generalizes in the obvious way to a (r,s) tensor. ... Thisis easiest to demonstrate with an example. Part 3 GR December 1, 2017 24 H.S.

11 Dec 2017: ahX=0-07 exp (V/20), (23)and II V301). Ph --Jrx 10 I(24). 516. ... h=1/(exp V30 1). (24). Equation (26) is derived simply from eqns.

4 Sep 2017: 10]) that, forcontinuous time-translation symmetry, TTSB is impossibleso long as the eigenstate thermalization hypothesis [21–24] issatisfied.However,wecanbuilduponrecentdevelopmentsinthe study of Floquet-many-body-localized (Floquet-MBL)systems