Erratum: Exponentiation of soft photons in Monte Carlo event generators: The case of the Bonneau-Martin cross section

Abstract

ERRATA FIG. 12. The experimental D t fragmentation distribution B d u / d x +. The curve is a fit to the distribution predicted by the Lund Monte Carlo procedure. fit (Sec. VI C) to the five fragmentation distributions change appreciably, although still within the combined statistical and systematic error of the original paper. The new values are /3=0.54+0.08f0.04 and B=0.53f0.03+0.03. The confidence level of the new fit changes to 3.670. The corresponding Monte Carlo fragmentation distribution is shown in the corrected Fig. 12. We do not show the new Monte Carlo fragmentation distributions for the other charmed particles because they are barely distinguishable from those published in the original paper.

α-Cluster States in Intermediate Mass Nuclei

“…We will follow the approach of Yennie, Frautschi and Suura in Ref. [35][36][37][38][39][40][41][42][43][44][45][46][47][48][49][50][51][52][53][54]. This choice is made possible by the formulation of Feynman for Einstein's theory, as the entire theory is a local, point particle field theory, albeit with an infinite number of interaction vertices.…”

“…[119], it also follows that the value of nj for the graviton and its attendant ghost is 42. For c 0, we have found the approximate representation (35) If we use the standard Fourier transform of the respective graviton propagator we obtain the improved Newton potential (36) where with (37) we have that (38) We note that the implied behavior of the running Newton constant, GN(k), that corresponds 11 to our resummed graviton propagator denominator, 11 We recall for the reader the Ward-Takahashi identities for the 1PI scalarscalar-graviton3pt function which follow from the conservation of T : if the matter incoming 4-momentum is , the matter outgoing 4-momentum is k, and the outgoing graviton 4-momentum is p = k, the conservation law…”

“…[33,34], its extension to Monte Carlo event generators in Refs. [35][36][37][38][39][40][41][42][43][44][45][46][47][48][49][50][51][52][53][54], and the QCD and QED QCD exponentiation in Refs. [55][56][57][58][59][60][61][62][63][64][65], which are extensions of the YFS theory to non-Abelian gauge theories.…”

“…For the record, the results in Refs. [26][27][28][29][30][31][32][35][36][37][38][39][40][41][42][43][44][45][46][47][48][49][50][51][52][53][54] have played significant roles in precision tests of SM physics.…”

Resummed Quantum Gravity: A Review with Applications

“…In what follows, the YFS [30][31][32][33][34][35][36][37][38][39][40][41][42][43][44][45] version (YFS-type soft resummation and its extension to quantum gravity were also worked-out by Weinberg in Ref. [46]) of the exact example is extended to resum the Feynman series for the Einstein-Hilbert Lagrangian for quantum gravity.…”