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Isospin asymmetry in holographic baryonic matter

by Nicolas Kovensky, Andreas Schmitt

Submission summary

As Contributors: Nicolas Kovensky
Arxiv Link: https://arxiv.org/abs/2105.03218v2 (pdf)
Date accepted: 2021-07-16
Date submitted: 2021-07-13 14:34
Submitted by: Kovensky, Nicolas
Submitted to: SciPost Physics
Academic field: Physics
Specialties:
  • High-Energy Physics - Theory
  • High-Energy Physics - Phenomenology
  • Nuclear Physics - Theory
Approach: Theoretical

Abstract

We study baryonic matter with isospin asymmetry, including fully dynamically its interplay with pion condensation. To this end, we employ the holographic Witten-Sakai-Sugimoto model and the so-called homogeneous ansatz for the gauge fields in the bulk to describe baryonic matter. Within the confined geometry and restricting ourselves to the chiral limit, we map out the phase structure in the presence of baryon and isospin chemical potentials, showing that for sufficiently large chemical potentials condensed pions and isospin-asymmetric baryonic matter coexist. We also present first results of the same approach in the deconfined geometry and demonstrate that this case, albeit technically more involved, is better suited for comparisons with and predictions for real-world QCD. Our study lays the ground for future improved holographic studies aiming towards a realistic description of charge neutral, beta-equilibrated matter in compact stars, and also for more refined comparisons with lattice studies at nonzero isospin chemical potential.

Published as SciPost Phys. 11, 029 (2021)



Author comments upon resubmission

We thank both referees for their positive report and referee 2 for the constructive questions and comments. Our replies to her/his points are as follows (in the same order as in the report)

(1) Our strategy was, firstly, to discuss the simplest possible version of the model (Secs 2 & 3: confined geometry, antipodal separation, YM approximation) in order to focus on a transparent discussion of the main conceptual issues. Secondly, we used the "most realistic" version (Sec 4, deconfined geometry, allowing for temperature effects and chiral symmetry restoration). The referee's suggestion, a square root-type action analogous to that of Eq. (78) in the context of the confined geometry, would be something "in between", computationally challenging but probably of limited value for real-world QCD. This would clearly be possible and the large-density behavior would be somewhat different, but we do not expect the main results to change substantially compared to what we found in Sec 4, at least in the interesting regimes of the phase transitions to baryonic matter. This expectation is based on our observations in the deconfined geometry, where we do use the square-root action and the phase diagram in the $\mu_B$-$\mu_I$ plane (not shown in the paper) is qualitatively the same.

(2) We agree with the referee that the explanations in Sec 2.4 are relatively brief, but we think that the main idea comes across. Therefore, and given that this is merely a recapitulation of the arguments given in Ref [52], we have decided to keep this section as it is.

(3) We have modified the sentence as follows, to make the statement clearer: "Most importantly, the energy differences between baryonic states with different isospin values go to zero as $N_c\to \infty$, such that the spectrum becomes continuous with respect to isospin."

(4) We thank the referee for this question, there is indeed a slight inaccuracy in our statement. As we explain in the manuscript, the problem about working with an expansion in powers of the field-strengths is that one does not get rid of the square roots in the Lagrangian due to the presence of the embedding function $x_4(u)$ (in which we obviously cannot expand). This problem, together with the higher-order terms in $F^2$, leads to equations of motion more complicated than Eqs. (81). In general, they do not allow one to solve algebraically for the derivatives of $x_4$ and $\hat{a}_0$ in a simple way. One would then have to implement a fully numerical evaluation. Now, as suggested by the referee, truncating at order $F^2$, i.e., using the YM Lagrangian, does lead to a set of equations of motion which can be solved for the derivatives of $x_4$ and $\hat{a}_0$ algebraically. In this sense, our statement regarding the "purely numerical evaluation" is not accurate. However, the actual solutions obtained in this way are much more complicated than those presented in the manuscript.

To be more precise, we have deleted the part about the "purely numerical evaluation" in the sentence the referee refers to, which now reads,

"Truncations of the resulting infinite series at ${\cal O}(F^2)$ or ${\cal O}(F^4)$ are possible, but also lead to a relatively complicated action due to the presence of the embedding function",

and we have changed the last sentence of this section to

"Had we used the YM approximation, which can be obtained by expanding the square root in Eq. (78) to second order in the field strengths, the resulting expressions would have been much more complicated."

(5) Yes, the referee is correct that this connection was already made in Ref [50], and we agree that our quote is not precise. We actually had in mind the analogue of Eq (92), which can be found in Ref [9]. We have now changed the sentence to

"..., was already pointed out in Ref. [50], see also Eq. (73) in Ref. [9]."

(6) We thank the referee for pointing this out. We have replaced "a_0(\infty)" by "$a_0(\infty) = \mu_I$".

(7) We have made several changes in the formulations in the first part of the paragraph that includes the sentence mentioned by the referee. We think the new version is clearer.

Submission & Refereeing History

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Resubmission 2105.03218v2 on 13 July 2021

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