2010
DOI: 10.1142/s0217751x10050445
|View full text |Cite
|
Sign up to set email alerts
|

On Flavor Conservation in Weak Interaction Decays Involving Mixed Neutrinos

Abstract: In the context of quantum field theory (QFT), we compute the amplitudes of weak interaction processes such as W + → e + + νe and W + → e + + νµ by using different representations of flavor states for mixed neutrinos. Analyzing the short time limit of the above amplitudes, we find that the neutrino states defined in QFT as eigenstates of the flavor charges lead to results consistent with lepton charge conservation. On the contrary, the Pontecorvo flavor states produce a violation of lepton charge in the vertex,… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

1
18
0

Year Published

2011
2011
2023
2023

Publication Types

Select...
9
1

Relationship

4
6

Authors

Journals

citations
Cited by 27 publications
(19 citation statements)
references
References 28 publications
1
18
0
Order By: Relevance
“…In particular, a nontrivial vacuum structure has been discovered in connection with mixing [2], as briefly shown in the Appendix. In this approach, though flavor states for mixed particles are consistently defined as eigenstates of the flavor charges [3,4], it turns out that these states are not representations of the Poincaré group [5].…”
Section: Introductionmentioning
confidence: 99%
“…In particular, a nontrivial vacuum structure has been discovered in connection with mixing [2], as briefly shown in the Appendix. In this approach, though flavor states for mixed particles are consistently defined as eigenstates of the flavor charges [3,4], it turns out that these states are not representations of the Poincaré group [5].…”
Section: Introductionmentioning
confidence: 99%
“…Flavor states are defined as eigenstates of such charges and have the form of SU (2) generalized coherent states [13]. In fact, according to Standard Model (SM), the flavor charge is always conserved -at tree level -in the production and detection processes, a feature which is violated by the usual Pontecorvo flavor states [14]. In addition, the exact flavor states cannot be generally phrased as a simple superposition of mass eigenstates, because of the unitary inequivalence of mass and flavor Hilbert spaces [8].…”
mentioning
confidence: 99%
“…The formalism retrieves the standard Pontecorvo formula for neutrino oscillations [22,23] and gives consistent results in the evaluation of the production-detection vertices of Fig. 1 [16,24] but the demonstrations are highly non-trivial. Finally, the flavor vacuum is not Lorentz invariant being explicitly time-dependent.…”
Section: Flavor Statesmentioning
confidence: 55%