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21 Aug 2019: Want tocompute spectra of a class B(l 2(N)). What attributes should an “algorithm” Γn(A) possess? ... Call this class1. Some notation:. If z / Sp(A) write. R (z, A) := (A zI )1 B(l 2(N)).

6 Dec 2019: hidden variables. Similarly, the result of measuring the positron’s spin along b is some. ... of polarizers and photomultipliers which read out 1 according to whether the photons arefound to be linearly polarized along some directions a and b.

6 Feb 2019: Calculating fB and fBs : some motivation. fBq parameterises weak decay of Bq mesons. ... Simulation. Some simulation details:. • NRQCD action - see also Rachel Dowdall’s talk:“B meson and Bottonium spectroscopy from radiativelyimproved NRQCD”.

4 Jun 2019: Ψpvq fpvq| ě 1{2, }v x}8 ď for some x P T. ... To simplify the learning andanalysis further we will assume that a P N, a ă K for some chosen K P N, and we let b “ aK1.

9 May 2019: If we set b to bethe identity then we obtain x = A1 (if it exists). ... Ly = b, Ux = y. Both latter systems are triangular and can be solved using forward/backward substitution.

6 May 2019: Some recent attempts have been made to model the impact of viscous fingeringon mixing beyond the onset. ... numbers smaller than some critical value Pec(R), the growth rate is only positive forwavenumbers smaller than 2p.

6 May 2019: 1 for axisymmetric spreading, = 1/2 fortwo dimensions), were derived in an appendix and some numerical solutions werepresented for the 2-D case. ... They derived a kinematic evolution equation for theinterfacial position, which we show bears some

6 Feb 2019: ΦQCD(m) Φ(µ). I m: mass of heavy quark (b) in some definition(all other masses zero for simplicity). ... Introduction. NLO. Renormalization and matching. match. Non-perturbative HQET. NPM. Some results in Non-perturbative HQET.

26 Feb 2019: Before we prove Theorem 2.1 we give some basic ideas in the proof. ... let θ parametrise the line then {θ : (1 θ)π(0) θπ B} = [0,α]for some α 1 (where α exists and is finite by convexity and compactness of B).

30 Nov 2019: Excitation of this state corresponds to performing a Lorentz boost. In thenon–relativistic limit, this amounts to replacing Φ0(x) with Φ0(xvt) for some v 1[53]. ... For V1(r) to return to zero at some finite r = r0, we would need that Φ(r0) =