arXiv Analytics

Sign in

arXiv:1509.01789 [hep-ph]AbstractReferencesReviewsResources

Binding energy of the $X(3872)$ at unphysical pion masses

V. Baru, E. Epelbaum, A. A. Filin, J. Gegelia, A. V. Nefediev

Published 2015-09-06Version 1

Chiral extrapolation of the $X(3872)$ binding energy is investigated using the modified Weinberg formulation of chiral effective field theory for the $D \bar{D}^*$ scattering. Given its explicit renormalisability, this approach is particularly useful to explore the interplay of the long- and short-range $D \bar{D}^*$ forces in the $X(3872)$ from studying the light-quark (pion) mass dependence of its binding energy. In particular, the parameter-free leading-order calculation shows that the $X$-pole disappears for unphysical large pion masses. On the other hand, without contradicting the naive dimensional analysis, the higher-order pion-mass-dependent contact interaction can change the slope of the binding energy at the physical point yielding the opposite scenario of a stronger bound $X$ at pion masses larger than its physical value. An important role of the pion dynamics and of the 3-body $D\bar{D}\pi$ effects for chiral extrapolations of the $X$-pole is emphasised. The results of the present study should be of practical value for the lattice simulations since they provide a non-trivial connection between lattice points at unphysical pion masses and the physical world.

Related articles: Most relevant | Search more
arXiv:1210.5072 [hep-ph] (Published 2012-10-18)
Chiral extrapolation of nucleon magnetic moments at next-to-leading-order
arXiv:hep-ph/0703147 (Published 2007-03-14)
Nucleon propagation through nuclear matter in chiral effective field theory
arXiv:1701.05871 [hep-ph] (Published 2017-01-20)
Transverse densities of octet baryons from chiral effective field theory