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Precision spectroscopy with reactor anti-neutrinos
High Energy Physics - Phenomenology · Submitted 2 Jul 2004
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We find that with a 3 month exposure of a one ton detector the isotope fractions and the thermal reactor power can be determined at a few percent accuracy, which may open the possibility of an application for safeguard or non-proliferation objectives.
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The abstract, sentence by sentence
In this work we present an accurate parameterization of the anti-neutrino flux produced by the isotopes 235U, 239Pu and 241Pu in nuclear reactors. We determine the coefficients of this parameterization, as well as their covariance matrix, by performing a fit to spectra inferred from experimentally measured beta spectra. Subsequently we show that flux shape uncertainties play only a minor role in the KamLAND experiment, however, we find that future reactor neutrino experiments to measure the mixing angle $\theta_{13}$ are sensitive to the fine details of the reactor neutrino spectra. Finally, we investigate the possibility to determine the isotopic composition in nuclear reactors through an anti-neutrino measurement. We find that with a 3 month exposure of a one ton detector the isotope fractions and the thermal reactor power can be determined at a few percent accuracy, which may open the possibility of an application for safeguard or non-proliferation objectives.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | In this work we present an accurate parameterization of the anti-neutrino flux produced by the isotopes 235U, 239Pu and 241Pu in nuclear reactors. | contribution 1.00 | 0.93 | 0.07 | asserted 1.00 |
| s1 | We determine the coefficients of this parameterization, as well as their covariance matrix, by performing a fit to spectra inferred from experimentally measured beta spectra. | method 0.98 | 0.96 | 0.04 | asserted 1.00 |
| s2 | Subsequently we show that flux shape uncertainties play only a minor role in the KamLAND experiment, however, we find that future reactor neutrino experiments to measure the mixing angle $\theta_{13}$ are sensitive to the fine details of the reactor neutrino spectra. | result 0.72 | 0.94 | 0.22 | asserted 1.00 |
| s3 | Finally, we investigate the possibility to determine the isotopic composition in nuclear reactors through an anti-neutrino measurement. | contribution 0.99 | 0.77 | 0.07 | hedged possibility 0.83 |
| s4 | We find that with a 3 month exposure of a one ton detector the isotope fractions and the thermal reactor power can be determined at a few percent accuracy, which may open the possibility of an application for safeguard or non-proliferation objectives. | result 0.90 | 0.95 | 0.40 | asserted 0.66 |
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The paper
Original abstract
In this work we present an accurate parameterization of the anti-neutrino flux produced by the isotopes 235U, 239Pu and 241Pu in nuclear reactors. We determine the coefficients of this parameterization, as well as their covariance matrix, by performing a fit to spectra inferred from experimentally measured beta spectra. Subsequently we show that flux shape uncertainties play only a minor role in the KamLAND experiment, however, we find that future reactor neutrino experiments to measure the mixing angle $\theta_{13}$ are sensitive to the fine details of the reactor neutrino spectra. Finally, we investigate the possibility to determine the isotopic composition in nuclear reactors through an anti-neutrino measurement. We find that with a 3 month exposure of a one ton detector the isotope fractions and the thermal reactor power can be determined at a few percent accuracy, which may open the possibility of an application for safeguard or non-proliferation objectives.
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References
How the literature uses it
11 arXiv papers cite this in 14 sentences
Papers citing it · 5 sentences without a confident label
Uses its method or tool 5 papers
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The reactor fluxes are parameterized as in Ref. [ref] and the inverse beta-decay cross section is taken from Ref. [ref] .
Neutrino oscillation bounds on quantum decoherence · Reactor experiments: KamLAND, Daya Bay and RENO · 0.82
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In performing the fit we follow the description given in Refs. [ref] but we do not include contributions from the error on $Z̅$ and WM since they are correlated between isotopes and do not change the fit appreciably.
On the determination of anti-neutrino spectra from nuclear reactors · Application to $^235$U, $^239$Pu and $^241$Pu · 0.99
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[ref] and corresponding to 3 yrs of data taking.
Fuzzy Dark Matter and Non-Standard Neutrino Interactions · Introduction · 1.00
Uses its data or values 2 papers
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We use reactor fluxes as parameterized in Ref. [ref] and the inverse beta-decay cross section from Ref. [ref] .
Probing neutrino quantum decoherence at reactor experiments · Current Constraints from RENO and Daya Bay · 0.97
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We take the $^235$U flux from [ref] and form factors from [ref] , although the suppression from form factors are negligible since $F(q^2)∼1$ for relevant energies.
A Plan to Rule out Large Non-Standard Neutrino Interactions After COHERENT Data · Reactor: CONUS · 0.99
Cites it as background 1 paper
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In fact, practical applications of antineutrino detectors in the nuclear industry have been discussed for a long time, mostly in the context of monitoring power reactors [ref] .
Antineutrino monitoring of spent nuclear fuel · Introduction · 0.87
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