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8 Jan 2020: McIntyre 1999. Last updated 24 Oct 2016.

9 Jan 2020: page 24 of the abovementioned Appendix III of the supplementary material for the Summer School), and in this paper with Tim Palmer written at a time when the idea was controversial.

18 Jan 2020: 3.1 SQM with a Potential 22. 3.1.1 Supersymmetric Ground States and the Witten Index 24.

20 Jan 2020: 24 = 1 and find its. degree. By calculating Tr((dg g1)3) at the point on S3 where x4 = 1,or otherwise deduce that the formula.

28 Jan 2020: xλW. ψ. (2.24). Now, the key point is that the ‘path’ integral8. ... f(X) = Xa(f(x)). yb. xa. xb= Y b(y). yb. – 24 –. at f(m). In particular, since the ψa are fermionic elements of the tangent bundle, under a.

30 Jan 2020: Λ = 〈Z2rZ20. 〉= σ2I 3σ4 (24). 7. In any case, when (20) and (21) are substituted back into equation (19) it is easily seen that the meanfield is equivalent to a solution

30 Jan 2020: η̄k1|eτ H(ˆ̄ψ,ψ̂)|ηk〉 = eτ H(η̄k,ηk) 〈η̄k1|ηk〉 = eτ H(η̄k1,ηk) eη̄k1ηk. (3.24).

2 Feb 2020: Since. and. ux= [ rx i&r] exp(W,. 24 xx = [ 2irx+, rxx i+,,r - (x)2r] exdih. ... U, = 24, e,_, Sl_le,_2. S,‘e,. Now, for kc n define r&= (AZ)-2e,, and #k= ,S$#Q_, and put 4, = (AZ)-2e,_,.

2 Feb 2020: u,(O) = u(O) = v,(O) = v2(0) = 0. (24). What follows is concerned, not with the general fourth moment at zr but rather with quantities involving intensities at two points

2 Feb 2020: 2n. ) γ. (24). 9. Provided the data is sufficiently well-resolved, we can use the assumption of continuity to resolveany phase ambiguities arising from this expression. ... 24] Michele D’Urso, Kamal Belkebir, Lorenzo Crocco, Tommaso Isernia, and