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6 Feb 2019: Random wall sources in operator-meson correlators. • Correlators fitted between• tmin = 2 4 and tmax = 16 on coarse ensembles• tmin = 4 8 and tmax = 24 on fine ensembles. •

27 May 2019: Typical curves for the near-field capillaryforce, eqn (24), and the magnetic attraction, eqn (25), areshown in Fig. ... 6c. As expected eqn (25) shows a linear increase. while eqn (24) decreases monotonically allowing for a singlemean separation.

6 Feb 2019: C.R. Mafra (DAMTP) Non-linear SYM 25.03.2015 24 / 26. Simpler representation for the 3-loop k4f 4mn.

28 Aug 2019: in spacetime such that they satisfy the operator equation. @. @t= i[H, ] (5.24). ... Figure 23: An incoming anti-fermion Figure 24: An outgoing anti-fermion. • Each vertex gets a factor of i. •

6 Feb 2019: 24/26. Summary I. The superspace approach to supergravity forms is based onconsistent, soluble sets of Bianchi identities.

18 Dec 2019: The predominant approach to this problem has been througha Lagrangian formulation [3, 10], which is the most appropriate for computationalstudies [2, 24, 29, 30]. ... Phys. 203 (2005), no. 2, 539–571. doi:10.1016/j.jcp.2004.08.023. [24] Hou, T. Y.;

19 Jul 2019: qg = 2n with n 2 Z (1.24). This is the famous Dirac quantisation condition. ... qg = 2n with n 2 Z. This, of course, is the Dirac quantisation condition (1.24).

19 Jul 2019: ai bj = 2 ij (2.24)? is sometimes referred to as the dual lattice. ... 53 –. The condition (2.24) can also be stated as the requirement that.

11 Jul 2019: D′ψC′D′E′F′ψE′F′. A′B′ , (2.24). which are in general independent. We verify by explicit calculation that if ψABCD and ψA′B′C′D′ arise from ... Proposition 2.3. Let I, J, I′, J′ be the invariants (2.24) of the Weyl

2 Jun 2019: Re2L =1708. 24[2(1 2)](13). can be made. The minimum of ReL occurs when = 1/4 and is. ... un1 = un J1F(un,Re) (24). where Jij := Fi/uj is the Jacobian and is an NT NT sized complex matrix.