2022
DOI: 10.48550/arxiv.2212.00385
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Kaon condensation in skyrmion matter and compact stars

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“…Similarly, ∆ a = 0 in the purely barionic phase, and its third component acquires a non-zero value in the condensate phase, ∆ cond = (0, 0, ∆). The explicit expressions for Λ 3 and ∆ in the condensed phase can be found in [49]. One can check that in the non-condensed phase, φ = 0 and the results of the previous section are recovered, namely, Λ 3 = Λ, ∆ = 0.…”
Section: Quantum Corrections To the Effective Potentialmentioning
confidence: 69%
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“…Similarly, ∆ a = 0 in the purely barionic phase, and its third component acquires a non-zero value in the condensate phase, ∆ cond = (0, 0, ∆). The explicit expressions for Λ 3 and ∆ in the condensed phase can be found in [49]. One can check that in the non-condensed phase, φ = 0 and the results of the previous section are recovered, namely, Λ 3 = Λ, ∆ = 0.…”
Section: Quantum Corrections To the Effective Potentialmentioning
confidence: 69%
“…Next, in Section 4, we take into account the strangeness degrees of freedom by extending the Skyrme field to a SU(3)-valued matrix field. In particular, we compute the kaon condensation in the semiclassical Skyrme crystal, briefly reviewing the very recent results of [49]. In Section 5, we apply all the previously investigated crystal solutions to the description of neutron stars.…”
Section: Skyrme Mattermentioning
confidence: 99%
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