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Hyperfine Splittings of Baryons Containing a Heavy Quark in the Skyrme Model

Elizabeth Jenkins, Aneesh V. Manohar

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Abstract

The Σ ∗ c − Σc and Σ ∗ b − Σb hyperfine mass splittings are computed in the Skyrme model. The hyperfine splittings are suppressed by both 1/Nc and by 1/mQ, where Nc is the number of colors and mQ is the mass of the heavy quark. The Σc, Σ ∗ c, Σb, Σ ∗ b

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What this paper is about

The Σ ∗ c − Σc and Σ ∗ b − Σb hyperfine mass splittings are computed in the Skyrme model. The hyperfine splittings are suppressed by both 1/Nc and by 1/mQ, where Nc is the number of colors and mQ is the mass of the heavy quark. The Σc, Σ ∗ c, Σb, Σ ∗ b

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Available abstract

The Σ ∗ c − Σc and Σ ∗ b − Σb hyperfine mass splittings are computed in the Skyrme model. The hyperfine splittings are suppressed by both 1/Nc and by 1/mQ, where Nc is the number of colors and mQ is the mass of the heavy quark. The Σc, Σ ∗ c, Σb, Σ ∗ b

Key concepts: Hyperfine structure, Physics, Baryon, Particle physics, Quark, Nuclear physics, Atomic physics

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