The origin of the mass of the Nambu-Goldstone bosons
arXiv:1803.02680 · doi:10.1142/S0217751X18500410
Abstract
We explain the origin of the mass for the Nambu-Goldstone bosons when there is a chemical potential in the action which breaks explicitly the symmetry. The method is based on the number of independent histories for the interaction of the pair of Nambu-Goldstone bosons with the degenerate vacuum (triangle relations). The analysis suggests that under some circumstances, pairs of massive Nambu-Goldstone bosons can become a single degree of freedom with an effective mass defined by the superposition of the individual masses of each boson. Possible mass oscillations for the Nambu-Goldstone bosons are discussed.
arXiv commentPublished, 15 pages pre-print, 16 pages Journal
References in corpus (8)
- On the number of Nambu-Goldstone bosons and its relation to charge densities
- Redundancies in Nambu-Goldstone Bosons
- Massive Nambu-Goldstone Bosons
- A relativistic non-relativistic Goldstone theorem: gapped Goldstones at finite charge density
- Shape versus Volume: Making Large Flat Extra Dimensions Invisible
- Spontaneous breaking of continuous translational invariance
- Review of AdS/CFT Integrability, Chapter I.1: Spin Chains in N=4 Super Yang-Mills
- Spontaneous symmetry breaking as a triangular relation between pairs of Goldstone bosons and the degenerate vacuum: Interactions of D-branes
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