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6 Feb 2019: Some SCET Jargon (for b-decays). ”hard modes“:virtual quarks and gluons with virtualities of order m2b ,will be integrated out by matching QCD SCET. ... A. Bharucha, TF, M. Wick, JHEP 1009 (2010) 090. [some overlap with A.

17 Jun 2019: construct more accurate balanced models that share at least some of the same. ... Let us return, however, to semigeostrophic theory in order to review some of.

6 Feb 2019: H′(x) = a cos H(x) b. for some real constant b. ... tanH(x). 2= ax c. for some real constant c. Hence there exist real constants A and B such that.

6 May 2019: although we note that physical properties are oftencorrelated in some manner, which reduces this variation (e.g. ... Webegin this section by presenting some snapshots (figure 5) from numerical solutionsto motivate the subsequent analysis.

29 Jan 2019: Suppose. that (a) holds for m < pµ with epµ = êµ together with (b) and (c) for j µ and some µ < M. ... b) ‖PQnej‖ C2(j)rn for any j Θ,. 16. for some constants C1(µ) and C2(j).

19 Jul 2019: It is called the magnetic length. lB =. sqB. To give you some sense for this, in a magnetic field of B = 1 Tesla, the magnetic length. ... At certain, very special values of B, we will find some number of Landau levels that.

27 May 2019: 1, 2), B = B(r){cos(ot),sin(ot),0}is the background magnetic field, ẑ is the normal to the air–water interface, B(r) is the strength of the ... 5a and b. When o is large, thesolution forms a stable oscillation around some mean value %h.As o decreases

18 Oct 2019: Julia Gog (jrg20@cam.ac.uk). (this version September 2019 - some typos corrected). ... for some constants A and B. Exercise 10 : show that.

7 May 2019: Solution. We first show (i) (ii). Assume dij = ‖xi xj‖2 for some x1,. ... This means that X = xxT for some x and so (u,v) =(xTAx,xTBx) R(A,B) as desired.

2 May 2019: Schrödinger and PDEs. Schrödinger operators: Bounded potential. φ : [0,) [0,) some increasing function. ... Resolvent II. Example 3: Back to Graphene. B. 0 200 400 600 800 1000.