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
Summary
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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