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Neutrino Masses and Mixing: Evidence and Implications
High Energy Physics - Phenomenology · Submitted 7 Feb 2002
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Measurements of various features of the fluxes of atmospheric and solar neutrinos have provided evidence for neutrino oscillations and therefore for neutrino masses and mixing.
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The abstract, sentence by sentence
Measurements of various features of the fluxes of atmospheric and solar neutrinos have provided evidence for neutrino oscillations and therefore for neutrino masses and mixing. We review the phenomenology of neutrino oscillations in vacuum and in matter. We present the existing evidence from solar and atmospheric neutrinos as well as the results from laboratory searches, including the final status of the LSND experiment. We describe the theoretical inputs that are used to interpret the experimental results in terms of neutrino oscillations. We derive the allowed ranges for the mass and mixing parameters in three frameworks: First, each set of observations is analyzed separately in a two-neutrino framework; Second, the data from solar and atmospheric neutrinos are analyzed in a three active neutrino framework; Third, the LSND results are added, and the status of accommodating all three signals in the framework of three active and one sterile light neutrinos is presented. We review the theoretical implications of these results: the existence of new physics, the estimate of the scale of this new physics and the lessons for grand unified theories, for supersymmetric models with R-parity violation, for models of extra dimensions and singlet fermions in the bulk, and for flavor models.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Measurements of various features of the fluxes of atmospheric and solar neutrinos have provided evidence for neutrino oscillations and therefore for neutrino masses and mixing. | background 0.99 | 0.06 | 0.56 | asserted 0.97 |
| s1 | We review the phenomenology of neutrino oscillations in vacuum and in matter. | contribution 0.93 | 0.38 | 0.04 | unclear 0.67 |
| s2 | We present the existing evidence from solar and atmospheric neutrinos as well as the results from laboratory searches, including the final status of the LSND experiment. | contribution 0.98 | 0.23 | 0.05 | asserted 0.79 |
| s3 | We describe the theoretical inputs that are used to interpret the experimental results in terms of neutrino oscillations. | method 0.70 | 0.55 | 0.03 | asserted 0.75 |
| s4 | We derive the allowed ranges for the mass and mixing parameters in three frameworks: First, each set of observations is analyzed separately in a two-neutrino framework; Second, the data from solar and atmospheric neutrinos are analyzed in a three active neutrino framework; Third, the LSND results are added, and the status of accommodating all three signals in the framework of three active and one sterile light neutrinos is presented. | contribution 0.48 | 0.86 | 0.23 | asserted 0.91 |
| s5 | We review the theoretical implications of these results: the existence of new physics, the estimate of the scale of this new physics and the lessons for grand unified theories, for supersymmetric models with R-parity violation, for models of extra dimensions and singlet fermions in the bulk, and for flavor models. | interpretation 0.98 | 0.45 | 0.24 | asserted 0.59 |
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The paper
Original abstract
Measurements of various features of the fluxes of atmospheric and solar neutrinos have provided evidence for neutrino oscillations and therefore for neutrino masses and mixing. We review the phenomenology of neutrino oscillations in vacuum and in matter. We present the existing evidence from solar and atmospheric neutrinos as well as the results from laboratory searches, including the final status of the LSND experiment. We describe the theoretical inputs that are used to interpret the experimental results in terms of neutrino oscillations. We derive the allowed ranges for the mass and mixing parameters in three frameworks: First, each set of observations is analyzed separately in a two-neutrino framework; Second, the data from solar and atmospheric neutrinos are analyzed in a three active neutrino framework; Third, the LSND results are added, and the status of accommodating all three signals in the framework of three active and one sterile light neutrinos is presented. We review the theoretical implications of these results: the existence of new physics, the estimate of the scale of this new physics and the lessons for grand unified theories, for supersymmetric models with R-parity violation, for models of extra dimensions and singlet fermions in the bulk, and for flavor models.
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References
How later papers used it
62 later papers cite it
1 later paper by other authors is listed below: 1 used its method or tool.
Uses its method or tool 1 paper
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Followed this paper's derivation closely to switch to the basis of instantaneous mass eigenstates in matter.
Leptonic CP Violation and its Origin (2020) · 0.90 · paraphrased: the licence does not allow quoting
How the literature uses it
55 arXiv papers cite this in 72 sentences
Papers whose main result relates to this one's
States the same result 2 papers
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Data on solar and atmospheric neutrinos provide evidence for neutrino masses and mixings.
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Solar, atmospheric and relic neutrinos give the indications of existence of nonzero neutrino masses and mixing.
Neutrino Masses and Mixing · 0.83
Papers citing it · 43 sentences without a confident label
Contests it 1 paper
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This practice has been violated in recent papers [ref] claiming that the anomalous oscillatory time modulation of the electron-capture decays [equation] observed in a GSI experiment [ref] is due to neutrino mixing (see Refs. [ref] ).
Rates of Processes with Coherent Production of Different Particles and the GSI Time Anomaly · Introduction · contest 0.83
Uses its method or tool 1 paper
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To solve this equation,[The derivation here closely follows Refs. [ref] .] we first switch to the basis of instantaneous mass eigenstates in matter, i.e., the eigenstates of the full Hamiltonian [ref] for a fixed $x$, [equation] where the relationship between instantaneous mass eigenstates $[ ν_1^m … ν_n^m ]^T$ and flavour eigenstates $[ ν_α … ]^T$ can be written as [equation] with $Ũ(x)$ an effective mixing matrix in matter.
Leptonic CP Violation and its Origin · Non-uniform density: the MSW effect · 0.90
Uses its data or values 1 paper
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This is compatible with the observation of solar and reactor neutrino oscillations due to the squared-mass difference $Δm^2_SOL = ( 7.59 ±0.21 ) ×10^-5 eV^2$ [ref] and the observation of atmospheric and accelerator neutrino oscillations due to the squared-mass difference $Δm^2_ATM = ( 2.74 ^+0.44_-0.26 ×10^-3 ) ×10^-3 eV^2$ [ref] if there are at least four massive neutrinos (see Refs. [ref] ).
nu_e Disappearance in MiniBooNE · Introduction · 0.86
Cites it as support 1 paper
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The observation of neutrino oscillations provided evidence that charged lepton must experience lepton-flavor-violating contact interactions [ref] .
Charged Lepton Flavor Violation · Introduction · 0.96
Cites it as background 23 papers
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The GALLEX [ref] and SAGE [ref] solar neutrino detectors (see Refs. [ref] ) have been tested in so-called "Gallium radioactive source experiments" which consist in the detection of electron neutrinos produced by intense artificial $^51Cr$ and $^37Ar$ radioactive sources placed inside the detectors.
Limits on nu_e and anti-nu_e disappearance from Gallium and reactor experiments · Gallium · 0.82
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The most general gauge invariant renormalisable Lagrangian one can add to the SM is then [ref] [equation] where $Y^ν$ and $M_N = M_N^T$ are complex $m ×3$ and $m ×m$ matrices, respectively.
Leptonic CP Violation and its Origin · Massive neutrinos · 0.82
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Neutrinos, as the most elusive particles in the standard model, can oscillate between flavor states during propagation due to their non-zero masses [ref] .
Quantum Correlations of Neutrinos in the Kerr-Newman Space-time · Introduction · 0.94
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