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Limits on Neutrino Mixing with new Heavy Particles
High Energy Physics - Phenomenology · Submitted 3 Feb 1994
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim If no assumption on the type of neutrinos involved in the mixing is made, we find $\snue^2<0.0071$, $\snumu^2<0.0014$ and $\snutau^2<0.033$.
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The abstract, sentence by sentence
We study the effects induced by new neutral fermions below their mass threshold, due to their possible mixing with the standard neutrinos. We use as experimental constraints the recent results on lepton universality, together with the measurement of the $\mu$ decay rate and the updated LEP data. In particular, the inclusion in our data set of the most recent determinations of the $\tau$ branching fractions, mass and lifetime implies that a previous indication of a non-vanishing mixing for $\nu_\tau$ is no longer present. We obtain new stringent limits on the mixing parameters between $\nu_e$, $\nu_\mu$, $\nu_\tau$ and heavy neutral states of different weak isospin. If no assumption on the type of neutrinos involved in the mixing is made, we find $\snue^2<0.0071$, $\snumu^2<0.0014$ and $\snutau^2<0.033$.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We study the effects induced by new neutral fermions below their mass threshold, due to their possible mixing with the standard neutrinos. | contribution 0.99 | 0.81 | 0.04 | asserted 0.47 |
| s1 | We use as experimental constraints the recent results on lepton universality, together with the measurement of the $\mu$ decay rate and the updated LEP data. | method 1.00 | 0.54 | 0.02 | asserted 0.99 |
| s2 | In particular, the inclusion in our data set of the most recent determinations of the $\tau$ branching fractions, mass and lifetime implies that a previous indication of a non-vanishing mixing for $\nu_\tau$ is no longer present. | result 0.59 | 0.72 | 0.13 | asserted 0.96 |
| s3 | We obtain new stringent limits on the mixing parameters between $\nu_e$, $\nu_\mu$, $\nu_\tau$ and heavy neutral states of different weak isospin. | result 0.82 | 0.95 | 0.58 | asserted 1.00 |
| s4 | If no assumption on the type of neutrinos involved in the mixing is made, we find $\snue^2<0.0071$, $\snumu^2<0.0014$ and $\snutau^2<0.033$. | result 1.00 | 0.97 | 0.78 | asserted 1.00 |
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The paper
Original abstract
We study the effects induced by new neutral fermions below their mass threshold, due to their possible mixing with the standard neutrinos. We use as experimental constraints the recent results on lepton universality, together with the measurement of the $\mu$ decay rate and the updated LEP data. In particular, the inclusion in our data set of the most recent determinations of the $\tau$ branching fractions, mass and lifetime implies that a previous indication of a non-vanishing mixing for $\nu_\tau$ is no longer present. We obtain new stringent limits on the mixing parameters between $\nu_e$, $\nu_\mu$, $\nu_\tau$ and heavy neutral states of different weak isospin. If no assumption on the type of neutrinos involved in the mixing is made, we find $\snue^2<0.0071$, $\snumu^2<0.0014$ and $\snutau^2<0.033$.
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References
How the literature uses it
32 arXiv papers cite this in 41 sentences
Papers citing it · 25 sentences without a confident label
Uses its data or values 4 papers
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A combined analysis of an old set of unitarity bounds [ref] , which does not include the one from the CKM matrix determination, leads to the following limits at 90% C.L. $|V_e4|^2 < 0.012, |V_μ4|^2< 0.0096 |V_τ4|^2 <0.016.$ If the CKM matrix constraint is included and partial cancellations between the contributions of different flavors are taken into account, a previous combined study [ref] then gives the more robust limits at $90%$ C.L., $|V_e4|^2 < 0.0066, |V_μ4|^2< 0.0060$ and $|V_τ4|^2 <0.018$.
The Search for Heavy Majorana Neutrinos · Electroweak Precision Tests · 0.85
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If we parametrize the non-unitary leptonic mixing matrix $N$ as [ref] [equation] where $η$ is Hermitian and $U$ is unitary, then $η_αβ$ is related to the coefficient matrix $c_αβ^d=6$ by [equation] In [ref] , the following constraints on these parameters at the $90 %$ C.L. were derived: $η_ee<2.0 ·10^-3$, $η_e μ<5.9 ·10^-5$, $η_e τ<1.6 ·10^-3$, $η_μμ<8.2 ·10^-4$, $η_μτ<1.0 ·10^-3$ and $η_ττ<2.6 ·10^-3$.
Non-unitary Leptonic Mixing and Leptogenesis · Non-unitarity relation to high-energy observables in the I seesaw model · 0.96
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They are constrained by global fits to high precision electroweak data at the level of $δ_e ≲2×10^-3$, $δ_μ≲2×10^-4$ and $δ_τ≲5×10^-3$ [ref] .
Testing the unitarity of the light neutrino mixing matrix · Introduction · 0.92
Compares with it 1 paper
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In the cases that had been analyzed before [ref] , we find more stringent limits (at the few per cent level).
Effects of new leptons in Electroweak Precision Data · Conclusions · 0.98
Cites it as background 10 papers
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Universality constraints derived from the CKM matrix elements [ref] as well as from pion decay [ref] has been extensevily analyzed and dedicated studies have been devoted to this subject [ref] .
Neutrino oscillations and the seesaw origin of neutrino mass · Weak universality bounds · 0.97
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Commonly, the non-unitary effects are searched in the oscillation experiments, searching an anomaly in the number of neutrino species that are detected [ref] .
Non-unitary limits on different textures for low-scale seesaw models · Non-unitary effects · 0.93
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The non-unitarity of the leptonic mixing matrix induced by the presence of heavy neutrinos has been studied in several works (see for instance [ref] ).
New Weinberg operator for neutrino mass and its seesaw origin · Introduction · 0.92
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