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26 Jan 2018: S k log G = kαN log E const. (1.24). and hence.

8 Aug 2018: The fingering of several branched struc-tures obtained from a conformal mappingapproach (16, 24) to the Hele-Shaw dy-namics is shown in Fig. ... M.McConnell, J. Phys. Chem. 96, 3167 (1992). 24. See, for example, D.

12 Feb 2018: Z. CT [y0,y1]Dx eS[x]/. nY. i=1. Oi(x(ti)). (3.24). – 47 –. for the n–point correlation function. The hats on the Ôi remind us that the

1 Nov 2018: 24 –. the commutator of the generator with the operator. ... U (b) U (a) = U (b a) = U (a b) = U (a) U (b) , (4.24).

25 Oct 2018: f 0(xi)|,. (6.24). where the first equality used equation (6.21) and the second (6.22).

14 May 2018: S[a] =. Z1. 2ab @. µa@µb. m2. 2ab. ab (ab ab)2 ddx (6.24).

14 May 2018: 7.24). where we’ve used the fact that, in a local trivialization, the covariant derivative acts.

14 May 2018: called a Nakanishi–Lautrup field) and write. [f ] =. ZDh eSgf [h,r]/ , (8.24). ... representation, h 2 0M (g). This does not imply that (8.24) is gauge invariant: indeed itcannot be if it is to fix a gauge!

23 Jan 2018: qq′). (1.24). Upon the substitution p′ = p m(qq′). t this becomes. ... Z0[J] =. d[ϕ] e. i2. ddx (µϕ(x)µϕ(x)m. 2ϕ2(x))iddx J(x)ϕ(x). (2.24). This is an integral with a highly oscillating integrand; if

8 Aug 2018: capillary waves in thepresence of coexisting monolayer phases.24 The more gen-eral treatment of boundary motion applicable to a domain ofany shape has, however, remained an open problem of ... un5 24. ph8. n2. 4n221fn unu>2!, 35! when the subfluid