2001
DOI: 10.1103/physrevd.63.125015
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Quantum field theory of boson mixing

Abstract: We consider the quantum field theoretical formulation of boson field mixing and obtain the exact oscillation formula. This formula does not depend on arbitrary mass parameters. We show that the space for the mixed field states is unitarily inequivalent to the state space where the unmixed field operators are defined. We also study the structure of the currents and charges for the mixed fields.

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Cited by 116 publications
(169 citation statements)
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“…[8], the difficulty lies in the fact that the Hilbert spaces for particles with definite flavor and those with definite mass are actually orthogonal in the infinite volume limit. This result has been subsequently generalized for any number of generations and for different types (fermionic or bosonic) of fields [10,16,17]. It has also emerged that the use of the correct Hilbert space (i.e.…”
Section: Introductionmentioning
confidence: 99%
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“…[8], the difficulty lies in the fact that the Hilbert spaces for particles with definite flavor and those with definite mass are actually orthogonal in the infinite volume limit. This result has been subsequently generalized for any number of generations and for different types (fermionic or bosonic) of fields [10,16,17]. It has also emerged that the use of the correct Hilbert space (i.e.…”
Section: Introductionmentioning
confidence: 99%
“…In this framework, there has been recently a remarkable progress in the study of the problem of field mixing in Quantum Field Theory (QFT) [8,9,10,11,12,13,14,15,16,17,18,19,20]. It is important to remark that, in spite of the fact of being usually treated in Quantum Mechanics (QM), the mixing between states of different masses is not even allowed in a non-relativistic theory due to the Bargmann superselection rules [21].…”
Section: Introductionmentioning
confidence: 99%
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“…The matter is far from pedantic and corrections to the usual formula for neutrino oscillations arise [21]. Flavor states constructed in this way are eigenstates of the flavor charge and the momentum operators but are not eigenstates of the Hamiltonian [21][22][23][24][25][26]. Nonetheless one can compute the expectation value of the Hamiltonian H on the flavor states and define from it dispersion relations.…”
Section: Introductionmentioning
confidence: 99%
“…In this paper, we report the recent results [40] showing that the vacuum condensate structure of many phenomena, such as particle mixing and fields in curved space [41][42][43][44][45][46][47][48][49][50][51][52][53][54], generates non trivial contributions to the energy of the universe [40], which can represent new components of dark energy and dark matter. In particular, dark matter components can be provided by the thermal vacuum of the hot plasma present at the center of a galaxy cluster, by the vacuum of fields in curved space [55] and by the flavor neutrino vacuum.…”
Section: Introductionmentioning
confidence: 99%