# Charmed Baryon $\Lambda_c$ in Nuclear Matter

## TL;DR

This study investigates how the mass and self-energies of the charmed baryon Λc change in nuclear matter using QCD sum rules, highlighting the importance of four-quark condensates and their density dependence.

## Contribution

It introduces a detailed analysis of Λc in nuclear matter considering different hypotheses for four-quark condensate density dependence, revealing weak attraction effects.

## Key findings

- F-type dependence leads to Λc repulsion in nuclear matter.
- QM-type dependence predicts a weak attraction (~20 MeV) for Λc.
- Weak density dependence of four-quark condensates is more consistent with observed hyperon binding energies.

## Abstract

Density dependences of the mass and self-energies of $\Lambda_c$ in nulear matter are studied in the parity projected QCD sum rule. Effects of nuclear matter are taken into account through the quark and gluon condensates. It is found that the four-quark condensates give dominant contributions. As the density dependences of the four-quark condensates are not known well, we examine two hypotheses. One is based on the factorization hypothesis (F-type) and the other is derived from the perturbative chiral quark model (QM-type). The F-type strongly depends on density, while the QM-type gives a weaker dependence. It is found that, for the F-type dependence, the energy of $\Lambda_c$ increases as the density of nuclear matter grows, that is, $\Lambda_c$ feels repulsion. On the other hand, the QM-type predicts a weak attraction ($\sim 20$ MeV at the normal nuclear density) for $\Lambda_c$ in nuclear matter. We carry out a similar analysis of the $\Lambda$ hyperon and find that the F-type density dependence is too strong to explain the observed binding energy of $\Lambda$ in nuclei. Thus we conclude that the weak density dependence of the four-quark condensate is more realistic. The scalar and vector self-energies of $\Lambda_c$ for the QM-type dependence are found to be much smaller than those of the light baryons.