2022
DOI: 10.1103/physrevd.105.034022
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Building a realistic neutron star from holography

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Cited by 34 publications
(21 citation statements)
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“…The reason for this contradiction turns out [46] to be the classification of nuclear matter: our setup predicts exceptionally low values of the adiabatic index γ = d log p/d log for dense nuclear matter which are below the limit value of 1.75 used in [74] so that our dense nuclear matter would be classified as quark matter in their setup. Interestingly, such low values of γ were also found recently for nuclear matter in the Witten-Sakai-Sugimoto model [28]. Apart from this small detail, we remark that our band in Fig.…”
Section: Discussionsupporting
confidence: 88%
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“…The reason for this contradiction turns out [46] to be the classification of nuclear matter: our setup predicts exceptionally low values of the adiabatic index γ = d log p/d log for dense nuclear matter which are below the limit value of 1.75 used in [74] so that our dense nuclear matter would be classified as quark matter in their setup. Interestingly, such low values of γ were also found recently for nuclear matter in the Witten-Sakai-Sugimoto model [28]. Apart from this small detail, we remark that our band in Fig.…”
Section: Discussionsupporting
confidence: 88%
“…It is therefore significantly increased from the bound of 230 from [46] which assumed no input from radius measurements. Interestingly, the same number, 230, was also found recently in the Witten-Sakai-Sugimoto model in [28]. Furthermore, we note that the latent heat ∆ associated with the first order transition to the quark matter phase are in excess of 740 MeV/fm 3 for all hybrid EoSs, which together with the fact that core pressures needed to support the existence of quark matter within NSs are in the unstable branch of solutions for the TOV equations, means that the hybrid EoSs do not support the existence of quark matter cores within quiescent NSs.…”
Section: Resultssupporting
confidence: 77%
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“…There exist arguments that suggest a universal bound c 2 s < 1/3 (see, e.g., [8,9]), thus favouring scenario i) and ii). However, a number of counter examples to this bound are known in QCD at large isospin density [10], two-color QCD [11], quarkyonic matter [12][13][14][15], models for high-density QCD [16][17][18][19][20][21][22][23][24][25][26][27][28][29][30] and models based on the gauge/gravity duality [31][32][33][34][35][36][37]. All of these example favour scenario iii).…”
mentioning
confidence: 99%
“…Beyond the shaded region at least one of the constraints is violated. As a consequence, for this particular value of the 't Hooft coupling, we obtain 2.11 M M max 2.40 M and new bounds for Λ 1.4 , R 1.4 , Λ 2.1 , R 2.1 , for instance 288 Λ 1.4 580.tion and see that indeed all known astrophysical constraints can be satisfied (in contrast to the simple pointlike approximation of baryons within the same holographic model[22,30]).…”
mentioning
confidence: 52%