Abstract

We study the Kondo effect for a $\Sigma_{c}$ ($\Sigma_{c}^{\ast}$) baryon in nuclear matter. In terms of the spin and isospin ($\mathrm{SU}(2)_{\mathrm{spin}} \times \mathrm{SU}(2)_{\mathrm{isospin}}$) symmetry, the heavy-quark spin symmetry and the S-wave interaction, we provide the general form of the Lagrangian for a $\Sigma_{c}$ ($\Sigma_{c}^{\ast}$) baryon and a nucleon. We analyze the renormalization equation at the one-loop level, and find that the coexistence of spin exchange and isospin exchange magnifies the Kondo effect in comparison with the case where the spin-exchange interaction and the isospin-exchange interaction exist separately. We demonstrate that the solution exists for the ideal sets of the coupling constants, including the $\mathrm{SU}(4)$ symmetry as an extension of the $\mathrm{SU}(2)_{\mathrm{spin}} \times \mathrm{SU}(2)_{\mathrm{isospin}}$ symmetry. We also conduct a similar analysis for the Kondo effect of a $\bar{D}$ ($\bar{D}^{\ast}$) meson in nuclear matter. On the basis of the obtained result, we conjecture that there could exist a "mapping" from the heavy meson (baryon) in vacuum onto the heavy baryon (meson) in nuclear matter.

Highlights

  • III, we carefully investigate the solutions of the renormalization group (RG) equation, and point out that the simultaneous flipping of the spin and the isospin is important for magnifying the Kondo effect

  • We have studied the Kondo effect for a c ( c∗) baryon in nuclear matter

  • By adopting the RG equation at one-loop order, we have found that the coexistence of the spin exchange and the isospin exchange magnifies the Kondo effect

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Summary

Introduction

Kondo explained why the electrical resistance in the metal which contains some impurity atoms with a nonzero spin increases logarithmically at low temperatures [1]. The logarithmic increase of the electrical resistance with the heavy impurity occurs when the following conditions are satisfied: (i) Fermi surface (degenerate state), (ii) particle-hole creation (loop effect), and (iii) non-Abelian interaction (e.g., the spinexchange interaction) [2,3,4]. The Kondo effect is not studied in condensed matter physics, but is applicable to the nuclear physics where the strong interaction plays a role of the main fundamental Since his work was recognized, the Kondo effect has had wider implications for theoretical approaches in quantum systems: the renormalization group method [5], the numerical renormalization group [6], the Bethe ansatz [7,8,9], the boundary conformal field theory [10,11,12,13,14,15,16], the bosonization method [17,18,19,20,21], the mean-field approximation (the large N limit) [22,23,24,25,26,27,28,29,30,31,32,33,34,35,36], and so on.

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