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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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arXiv IDhep-ph/9402224 (version 2)
Pith IDK264PKOR, Pith's permanent record of this paper and its review
CitationD. Tommasini, E. Nardi, E. Roulet. "Limits on Neutrino Mixing with new Heavy Particles." arXiv:hep-ph/9402224 (1994). https://pith.science/paper/K264PKOR
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Compiled by classifier-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 4,421 input tokens, $0.0002 reported.

What the abstract itself states, as probabilities: claims first 0.03 · states limitation 0.39 · human participants 0.02 · controlled comparison 0.07 · randomized assignment 0.01 · states quantitative result 0.99 · compares with prior results 0.85 · mentions code or data availability 0.02.

The abstract, sentence by sentence

arXiv listing abstract v2. Results and the main claim are underlined; .

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

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
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

What kind of paper the classifier reports this is: theoretical result 0.90 · evidence from analysis of existing data 1.00.

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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

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

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

Papers citing it · 25 sentences without a confident label

Uses its data or values 4 papers
  • 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

  • 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

  • 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

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