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7 Apr 2021: k 2h. a,. a. (2.22). We recognise this as the first Brillouin zone. ... function of k 2 [/a,/a). The spectrum that we previously saw in Figure 18 then.

7 Apr 2021: k 2h. a,. a. (3.22). We recognise this as the first Brillouin zone. ... function of k 2 [/a,/a). The spectrum that we previously saw in Figure 28 then.

18 Mar 2008: 2.2.1 Line integrals at the endpoints. The line integrals corresponding to the endpoints a and b are well behaved,and their asymptotic expansion can be deduced from Watson’s ... First, we deduce from Watson’s Lemma [24] that.

19 Jul 2019: The wavefunction above is normalisable whenever we. can find a > 0 such that. ... An imaginary energy may soundstrange, but it is has a very natural interpretation.

22 Nov 2011: ψj,k / a a k. 2j 0, a k. 2j,. φk / a a k 0, a k,. ... 48] G. N. Watson. A Treatise on the Theory of Bessel Functions.

17 Nov 2010: This introducedC39-endo puckering in the cytidine strand. When Watson–Crick hy-drogen bonding was maintained with distance constraints the energyrose rapidly beyond a twist of 70 (dotted line). ... We show here that a very similar structureapparently

21 Feb 2023: Foundations of spectral computations 17. (3) a.A/ lies in the essential spectrum but is an isolated point of the spectrum,. ... 4) a.A/ is a cluster point of Sp.A/. For example, if A is compact, self-adjoint and non-negative, only (3) or (4) can hold.

29 Jan 2008: 10. for a sequence of fixed values of λ Rm and µ R. ... be a provisional choice of γk, where the multipliers λi, i = 1, 2,. ,

26 Jul 2013: U. D2δ. D1δ. (a) (b)D0. n̂ Diδ. D0. FIG. 2. a A fluid-jetting body. ... 0.8. 1. b/a. b/a. (a) (b). E. E = 0.01. E = 0.12 = 1. =

4 Nov 2013: 244 J. A. Neufeld, D. Vella and H. E. Huppert. Volume t1/2. = ... Fluidwas injected at the centre of the cell (x = 0 cm) using a Watson Marlow 505Uperistaltic pump from a reservoir whose mass was recorded as a function of time.