Q-balls

E24266

Q-balls are hypothetical, stable, non-topological solitons predicted in certain quantum field theories, often considered as exotic candidates for dark matter or new physics beyond the Standard Model.

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Statements (49)

Predicate Object
instanceOf dark matter candidate
hypothetical particle-like object
non-topological soliton
theoretical construct in quantum field theory
canBeProducedIn early Universe phase transitions
fragmentation of scalar condensates
non-equilibrium dynamics after inflation
canDecayInto fermions carrying same global charge
standard model particles in unstable scenarios
consideredAs candidate for new physics beyond the Standard Model
exotic dark matter candidate
hasProperty arise from attractive self-interactions of scalar fields
can be absolutely stable in some models
can be energetically favored over free quanta
can be long-lived
can be macroscopically large
can be metastable in some models
can have large quantum number Q
can have thick-wall regime
can have thin-wall regime
carry scalar field charge
classically stable
conserved global charge
localized field configuration
minimize energy at fixed global charge
non-topological
time-dependent phase
mathematicalDescription nonlinear solutions of scalar field equations with global symmetry
mayContributeTo baryon asymmetry of the Universe in some models
cosmological dark matter density
predictedIn Affleck–Dine baryogenesis scenarios
certain relativistic quantum field theories
supersymmetric extensions of the Standard Model
theories with complex scalar fields
theories with global U(1) symmetry
relatedTo Affleck–Dine condensate fragmentation
baryogenesis
baryon number carrying objects in some models
dark matter phenomenology
early Universe cosmology
global charge conservation
lepton number carrying objects in some models
non-topological soliton solutions of scalar field equations
searchesVia astrophysical constraints
direct detection experiments for exotic massive particles
indirect detection through decay products
stabilityCondition energy per unit charge less than mass of corresponding free particle
existence of suitable scalar potential with attractive self-interactions
theoreticalOrigin minimization of energy functional at fixed conserved charge

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