An ideal charged boson-antiboson gas condenses only in the charge-dominant component, and the zero-temperature switch from an empty to a charged ground state is classified as a first-order, externally induced transition.
massive” ground state of the system. As we saw, in this case the energy density of the ground state of the system is εgs = ncondm. Therefore, to create a “massive
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Ideal Boson Particle-Antiparticle System at Finite Temperatures
An ideal charged boson-antiboson gas condenses only in the charge-dominant component, and the zero-temperature switch from an empty to a charged ground state is classified as a first-order, externally induced transition.