Effective field theory of Bose-Einstein condensation of clusters and Nambu-Goldstone-Higgs states in C
arXiv:1411.6353 · doi:10.1103/PhysRevC.94.014314
Abstract
An effective field theory of cluster condensation is formulated as a spontaneously broken symmetry in quantum field theory to understand the raison d'etre and nature of the Hoyle and cluster states in C. The Nambu--Goldstone and Higgs mode operators in infinite systems are replaced with a pair of canonical operators whose Hamiltonian gives rise to discrete energy states in addition to the Bogoliubov--de Gennes excited states. The calculations reproduce well the experimental spectrum of the cluster states. The existence of the Nambu--Goldstone--Higgs states is demonstrated and crucial. The decay transitions are also obtained.
8 pages, 8 figures
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- Supersolidity of the cluster structure in the nucleus C
- Thermal and quantum fluctuations of confined Bose-Einstein condensate beyond the Bogoliubov approximation
- Supersolidity of cluster structure in Ca
- Bose-Einstein condensation of five clusters in Ne and supersolidity