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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 ]]] =

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.

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).

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].

30 Apr 2017: 2.5 -. 8. Douady. 2.0 4 I 23 24 25 26 21 28 29 30 31 32. ... Figure 24 presents a study of the mode n = 9, around 20 Hz.

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

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.

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

22 Nov 2017: Proc. Nat. Acad. Sci. USA 74, 2397–2401 (1977)24. LeBret, M.: Catastrophic variations of twist and writhing of circular DNA with constraint? ... Math. Methods Appl. Sci. 24, 1325–1335 (2001)37. Goriely, A., Tabor, M.: Nonlinear dynamics of filaments.

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

20 Jan 2017: Note that (2.24) implies thatui is independent of z in the interior of each isopycnal layer, hi1 < z < hi. ... interior of each layer, @ui/@z = 0,as implied by (2.24).

20 Jan 2017: Accepted article online 24 JUN 2016. Published online 13 JUL 2016.

4 Dec 2017: When the nutrient is essential for life, suchas oxygen for obligate aerobes, f (c) may vanish below somec [24,25]. ... μ̄ = 1λ. λ0. dx y(c)cb. (24). 022701-5. FRANÇOIS J. PEAUDECERF AND RAYMOND E.

3 Dec 2017: Oecologia118, 132–143. 24 Beyschlag, W. and Pfanz, H. (1992) A fast method to detect the occurrence ofnonhomogenous distribution of stomatal aperture in heterobaric plant leaves.Experiments with Arbutus unedoL.

9 Jul 2017: Received 28 March 2015; published 24 June 2015). In analogy with crystalline solids around us, Wilczek recently proposed the idea of “time crystals” asphases that spontaneously break the continuous time translation

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.

11 Mar 2017: of novel, out-of-equilibrium quantum phases3,5,24. ... LETTER RESEARCH. 24. Abanin, D. A., De Roeck, W. & Huveneers, F.