<?xml version="1.0"?>
<rdf:RDF xmlns:rdf="http://www.w3.org/1999/02/22-rdf-syntax-ns#" xmlns:dc="http://purl.org/dc/elements/1.1/"><rdf:Description rdf:about="https://repozitorij.uni-lj.si/IzpisGradiva.php?id=156370"><dc:title>Toward the quark mass dependence of $T_{cc}^+$ from lattice QCD</dc:title><dc:creator>Collins,	Sara	(Avtor)
	</dc:creator><dc:creator>Nefediev,	Alexey	(Avtor)
	</dc:creator><dc:creator>Padmanath,	M.	(Avtor)
	</dc:creator><dc:creator>Prelovšek,	Saša	(Avtor)
	</dc:creator><dc:subject>physics of elementary particles</dc:subject><dc:subject>lattice QCD</dc:subject><dc:description>The $DD^*$ scattering phase shifts in the $T_{cc}^+ = cc\bar{u}\bar{d}$ channel are extracted from lattice QCD for five different charm quark masses and a fixed light-quark mass corresponding to $m_{\pi} \simeq$ 280  MeV. The phase shifts are analyzed employing two approaches: effective range expansion and Lippmann-Schwinger equation derived in the effective field theory. In the latter case, the results imply an attraction at short range parametrized by contact terms and a slight repulsion at long range mediated by one-pion exchange with $m_{\pi} &gt; m_{D^*}-m_D$. The poles in the amplitude across the complex energy plane are extracted and their trajectories are discussed as the charm quark mass is varied. Two complex conjugate poles corresponding to a resonance below threshold are found for $m_c$ close to the physical value. They turn into a pair of virtual states at the largest $m_c$ studied. With further increasing $m_c$, one virtual pole representing $T_{cc}^+$ is expected to move towards the two-body threshold and turn into a bound state. The light-quark mass dependence of the $T_{cc}^+$ pole is briefly discussed using the data on $DD^*$ scattering from other lattice collaborations.

</dc:description><dc:date>2024</dc:date><dc:date>2024-05-22 14:49:47</dc:date><dc:type>Članek v reviji</dc:type><dc:identifier>156370</dc:identifier><dc:language>sl</dc:language></rdf:Description></rdf:RDF>
