2005
DOI: 10.1016/j.physletb.2005.08.097
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Spinning skyrmions and the Skyrme parameters

Abstract: The traditional approach to fixing the parameters of the Skyrme model requires the energy of a spinning Skyrmion to reproduce the nucleon and delta masses. The standard Skyrme parameters, which are used almost exclusively, fix the pion mass to its experimental value and fit the two remaining Skyrme parameters by approximating the spinning Skyrmion as a rigid body. In this paper we remove the rigid body approximation and perform numerical calculations which allow the spinning Skyrmion to deform and break spheri… Show more

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Cited by 70 publications
(126 citation statements)
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“…As discussed earlier, the value g = 96.7 is taken from [5], which involves g = 96.7 fitting properties of the single Skyrmion to the nucleon and delta, whilst treating F π as a free parameter. However, it is known that this method of parameter fitting can be problematic, in any Skyrme model, because of difficulties associated with the rigid rotor approximation [23]. Access to the properties of multi-Skyrmions allows the following alternative procedure to be applied.…”
Section: Constructing Multi-skyrmionsmentioning
confidence: 99%
“…As discussed earlier, the value g = 96.7 is taken from [5], which involves g = 96.7 fitting properties of the single Skyrmion to the nucleon and delta, whilst treating F π as a free parameter. However, it is known that this method of parameter fitting can be problematic, in any Skyrme model, because of difficulties associated with the rigid rotor approximation [23]. Access to the properties of multi-Skyrmions allows the following alternative procedure to be applied.…”
Section: Constructing Multi-skyrmionsmentioning
confidence: 99%
“…In work based on the conventional semiclassical quantization the pion mass term has in contrast to be introduced by way of an explicit chiral symmetry breaking term. In that method the requirement of rotational stability requires a value for the pion mass that is considerably larger than the empirical value [26]. With such large values for the pion mass the chiral symmetry breaking term leads to spatial configurations for the ground state solution of the Skyrme model with baryon number larger than 4, which differ significantly from those obtained in the chiral limit [27].…”
Section: Discussionmentioning
confidence: 99%
“…In the standard Skyrme model there are many ways to calibrate the model, with the original calibration obtained by matching the masses of the nucleon and delta resonance using a rigid rotor quantization [33,34]. However, the delta is a broad resonance that strongly radiates pions, which is related to the fact that the spin of the delta strongly deforms the B = 1 Skyrmion and this has a rather complicated effect on the calibration of the model [35]. Furthermore, the calibration using the B = 1 sector does not provide an accurate fit for the properties of JHEP05 (2018)174 nuclei with larger values of B, so alternative calibrations have been proposed to provide a better match for larger nuclei [36].…”
Section: Jhep05(2018)174 4 Conclusionmentioning
confidence: 99%