Calibration Methods of Silicon Photomultiplier for JUNO-TAO Central Detector
Pith reviewed 2026-05-16 21:39 UTC · model grok-4.3
The pith
Calibration of Silicon Photomultipliers in JUNO-TAO limits impacts on vertex and energy resolution to under 2% and 3%.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The authors describe channel-level calibration methods for SiPM dark count rate, relative PDE, time offset, gain, and IOCT based on charge and time information, along with a novel method for tile-level EOCT rate and emission angle distribution by switching SiPM groups with an LED. Using one million simulated events, they evaluate expected biases: ~3% for relative PDE, 1.4% for IOCT, 0.4% for DCR, <0.1% for EOCT rate and gain, <0.2 ns for time offset, and <4% for the EOCT emission angle distribution in the main range. These accuracies ensure the overall impacts on vertex precision and energy resolution remain limited to relative degradations below 2% and 3%, respectively, verifying the method
What carries the argument
Charge and time based calibration for SiPM parameters combined with LED group-switching for external optical crosstalk measurement.
Load-bearing premise
The simulation of one million events accurately captures real detector behavior including LED light distribution and sensor response without unmodeled effects that would increase biases in actual operation.
What would settle it
Running the calibration on actual data from the deployed JUNO-TAO detector and comparing the obtained parameter values and resulting resolutions against the simulation predictions would falsify the claim if the observed degradations exceed 2% or 3%.
read the original abstract
The Taishan Antineutrino Observatory (TAO or JUNO-TAO) is a satellite observatory for the Jiangmen Underground Neutrino Observatory (JUNO), located 44 meters away from the No.1 reactor of the Taishan Nuclear Power Plant. TAO can measure the reactor antineutrino energy spectrum with excellent energy resolution (better than 2% at 1 MeV) using state-of-the-art Silicon Photomultipliers (SiPMs) operated at low temperature. To achieve this goal, the SiPMs (together with their readout electronics) must be well calibrated. This paper presents the channel-level calibration methods for the dark count rate (DCR), relative photon detection efficiency (PDE), time offset, gain, and internal optical crosstalk (IOCT) of the SiPMs based on charge and time information of the collected events. For the tile-level calibration of the external optical crosstalk (EOCT), in terms of its rate and emission angle distribution, a novel method is proposed by switching on and off different groups of SiPMs with an LED placed in the detector. Using one million simulated events, the expected calibration biases are evaluated for all the aforementioned parameters: relative PDE (~3%), IOCT (1.4%), DCR (0.4%), EOCT Rate (<0.1%), gain (<0.1%), time offset (<0.2 ns). The emission angle distribution of the EOCT photons could be measured with a bias of less than 4% in the main angular range. With the this calibration accuracy, the overall impacts of SiPM parameter uncertainties and calibration biases on vertex precision and energy resolution are limited, with relative degradation below 2% and 3%, respectively. It verifies the validity of the calibration method for the JUNO-TAO detector.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript presents channel-level calibration methods for SiPM parameters (DCR, relative PDE, time offset, gain, IOCT) extracted from charge and time distributions of collected events, along with a novel tile-level EOCT calibration using LED-driven group switching. Biases for all parameters are quantified from one million simulated events (PDE ~3%, IOCT 1.4%, DCR 0.4%, EOCT rate <0.1%, gain <0.1%, time offset <0.2 ns, EOCT angle distribution <4% bias in main range), and these are propagated to show relative impacts below 2% on vertex precision and 3% on energy resolution.
Significance. If the simulation model holds, the work supplies concrete, numerically explicit calibration procedures and bias estimates that keep SiPM uncertainties from materially degrading the <2% energy resolution target at 1 MeV. The direct extraction of biases from a large simulated sample and the parameter-free character of several reported quantities constitute clear strengths for an instrumentation paper supporting JUNO-TAO.
major comments (2)
- [Abstract and results (bias evaluation)] Abstract and results section on bias propagation: the headline claims of relative degradation below 2% (vertex) and 3% (energy resolution) rest entirely on biases extracted from one million simulated events; any mismatch between the simulated LED light distribution, SiPM response, or unmodeled systematics and actual detector behavior would scale these impact numbers upward, yet no real-data cross-check or sensitivity study to model variations is provided.
- [EOCT calibration subsection] EOCT tile-level method: the novel switching procedure for rate and emission-angle distribution is load-bearing for the <0.1% rate and <4% angle bias claims, but the manuscript does not quantify how uncertainties in the assumed LED spatial distribution or in the on/off switching transients propagate into the extracted EOCT parameters.
minor comments (2)
- [Abstract] Abstract: the phrase 'With the this calibration accuracy' is grammatically incorrect and should read 'With this calibration accuracy'.
- [Simulation and bias evaluation] The manuscript should add a short paragraph discussing the main assumptions of the simulation (LED uniformity, absence of temperature gradients, etc.) and how they might affect the quoted bias values.
Simulated Author's Rebuttal
We thank the referee for the positive assessment of our manuscript and for the constructive comments. We address each major comment below and outline the revisions we will make.
read point-by-point responses
-
Referee: Abstract and results section on bias propagation: the headline claims of relative degradation below 2% (vertex) and 3% (energy resolution) rest entirely on biases extracted from one million simulated events; any mismatch between the simulated LED light distribution, SiPM response, or unmodeled systematics and actual detector behavior would scale these impact numbers upward, yet no real-data cross-check or sensitivity study to model variations is provided.
Authors: We acknowledge that all bias evaluations and propagated impacts are derived from one million simulated events. Real calibration data from the JUNO-TAO detector are not yet available, as the detector is still under construction. To address the concern about model dependence, we will add a dedicated sensitivity study in the revised manuscript. This study will vary key simulation inputs (LED light distribution, SiPM response models, and selected unmodeled systematics) and report the resulting changes to the bias and impact figures, thereby quantifying the robustness of the headline claims. revision: partial
-
Referee: EOCT tile-level method: the novel switching procedure for rate and emission-angle distribution is load-bearing for the <0.1% rate and <4% angle bias claims, but the manuscript does not quantify how uncertainties in the assumed LED spatial distribution or in the on/off switching transients propagate into the extracted EOCT parameters.
Authors: We agree that explicit propagation of these uncertainties would strengthen the EOCT calibration section. In the revised manuscript we will include an additional analysis that quantifies how uncertainties in the assumed LED spatial distribution and in the on/off switching transients affect the extracted EOCT rate and emission-angle distribution. This will be performed via dedicated simulations that vary the relevant parameters within their expected ranges and report the resulting variations in the EOCT observables. revision: yes
Circularity Check
No significant circularity in calibration methods or bias propagation
full rationale
The paper presents channel-level calibration procedures that extract DCR, PDE, time offset, gain, and IOCT directly from measured charge and time distributions of collected events, without any equations that define the target quantities in terms of the fitted outputs. Tile-level EOCT calibration uses a switching method on LED-illuminated groups. Bias estimates for these parameters are obtained by applying the same extraction procedures to one million independent simulated events that encode the assumed light distribution and sensor response; these simulations serve as an external benchmark rather than a self-referential input. The final impact figures (<2% vertex, <3% energy resolution degradation) are obtained by standard propagation of the reported bias values and do not reduce to the calibration inputs by construction. No load-bearing self-citations, uniqueness theorems, or ansatzes are invoked in the provided derivation chain.
Axiom & Free-Parameter Ledger
free parameters (1)
- event selection thresholds
axioms (1)
- standard math Poisson statistics govern dark counts and photon arrivals
Reference graph
Works this paper leans on
-
[1]
M. Fallot et al.,New antineutrino energy spectra predictions from the summation of beta decay branches of the fission products,Phys. Rev. Lett.109(2012) 202504 [1208.3877]
work page internal anchor Pith review Pith/arXiv arXiv 2012
-
[2]
R. Greenwood, R. Helmer, M. Lee, M. Putnam, M. Oates, D. Struttmann et al.,Total absorption gamma-ray spectrometer for measurement of beta-decay intensity distributions for fission product radionuclides,Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment314(1992) 514
work page 1992
-
[3]
A. Algora et al.,Reactor Decay Heat in Pu-239: Solving the gamma Discrepancy in the 4-3000-s Cooling Period, Phys. Rev. Lett.105(2010) 202501. – 24 –
work page 2010
-
[4]
G. Rudstam, P.I. Johansson, O. Tengblad, P. Aagaard and J. Eriksen,Beta and gama spectra of short-lived fission products,Atom. Data Nucl. Data Tabl.45(1990) 239
work page 1990
-
[5]
K. Takahashi and M. Yamada,Gross theory of nuclear beta-decay,Progress of Theoretical Physics41(1969) 1470
work page 1969
-
[6]
On the determination of anti-neutrino spectra from nuclear reactors
P. Huber,On the determination of anti-neutrino spectra from nuclear reactors,Phys. Rev. C84(2011) 024617 [1106.0687]
work page internal anchor Pith review Pith/arXiv arXiv 2011
-
[7]
Improved Predictions of Reactor Antineutrino Spectra
T.A. Mueller et al.,Improved Predictions of Reactor Antineutrino Spectra,Phys. Rev. C83(2011) 054615 [1101.2663]
work page internal anchor Pith review Pith/arXiv arXiv 2011
-
[8]
K. Schreckenbach, H. Faust, F. von Feilitzsch, A. Hahn, K. Hawerkamp and J. Vuilleumier,Absolute measurement of the beta spectrum from 235u fission as a basis for reactor antineutrino experiments,Physics Letters B99(1981) 251
work page 1981
-
[9]
K. Schreckenbach, G. Colvin, W. Gelletly and F. Von Feilitzsch,Determination of the antineutrino spectrum from 235u thermal neutron fission products up to 9.5 mev,Physics Letters B160(1985) 325
work page 1985
-
[10]
A. Hahn, K. Schreckenbach, W. Gelletly, F. von Feilitzsch, G. Colvin and B. Krusche,Antineutrino spectra from 241pu and 239pu thermal neutron fission products,Physics Letters B218(1989) 365
work page 1989
-
[11]
Updated Summation Model: An Improved Agreement with the Daya Bay Antineutrino Fluxes
M. Estienne et al.,Updated Summation Model: An Improved Agreement with the Daya Bay Antineutrino Fluxes, Phys. Rev. Lett.123(2019) 022502 [1904.09358]
work page internal anchor Pith review Pith/arXiv arXiv 2019
- [12]
- [13]
-
[14]
C. Giunti, Y.F. Li, C.A. Ternes and Z. Xin,Reactor antineutrino anomaly in light of recent flux model refinements, Phys. Lett. B829(2022) 137054 [2110.06820]
-
[15]
Spectral Structure of Electron Antineutrinos from Nuclear Reactors
D.A. Dwyer and T.J. Langford,Spectral Structure of Electron Antineutrinos from Nuclear Reactors,Phys. Rev. Lett. 114(2015) 012502 [1407.1281]. [21]JUNOcollaboration,Potential to identify neutrino mass ordering with reactor antineutrinos at JUNO,Chin. Phys. C 49(2025) 033104 [2405.18008]. [22]JUNOcollaboration, A. Abusleme et al.,TAO Conceptual Design Repo...
work page internal anchor Pith review Pith/arXiv arXiv 2015
- [16]
-
[17]
H. Shi, J. Wang, G. Cao, W. Wang and Y. Wei,Vertex reconstruction in the TAO experiment, 8, 2025
work page 2025
- [18]
-
[19]
G. Li et al.,A Novel Measurement Method for SiPM External Crosstalk Probability at Low Temperature,IEEE Trans. Nucl. Sci.71(2024) 1357 [2406.02249]
-
[20]
D. Gallacher et al.,Characterization of external cross-talk from silicon photomultipliers in a liquid xenon detector, Eur. Phys. J. C85(2025) 692 [2502.15991]. – 25 –
-
[21]
Z. Xie, J. Cao, Y. Ding, M. Liu, X. Sun, W. Wang et al.,A liquid scintillator for a neutrino detector working at -50 degree,Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment1009(2021) 165459
work page 2021
-
[22]
Xu et al.,Calibration strategy of the JUNO-TAO experiment,Eur
H. Xu et al.,Calibration strategy of the JUNO-TAO experiment,Eur. Phys. J. C82(2022) 1112 [2204.03256]
-
[23]
G. Luo et al.,Design optimization of plastic scintillators with wavelength-shifting fibers and silicon photomultiplier readouts in the top veto tracker of the JUNO-TAO experiment,Nucl. Sci. Tech.34(2023) 99 [2302.12669]
-
[24]
G. Luo et al.,Performance of plastic scintillator modules for top veto tracker at Taishan Antineutrino Observatory, Nucl. Sci. Tech.36(2025) 91 [2406.15973]. [33]JUNOcollaboration,The Application of SNiPER to the JUNO Simulation,J. Phys. Conf. Ser.898(2017) 042029 [1702.05275]
-
[25]
Lin et al.,Simulation software of the JUNO experiment,Eur
T. Lin et al.,Simulation software of the JUNO experiment,Eur. Phys. J. C83(2023) 382 [2212.10741]. [35]GEANT4collaboration,GEANT4 - A Simulation Toolkit,Nucl. Instrum. Meth. A506(2003) 250
-
[26]
W. Wang,The taishan antineutrino observatory simulation and related experimental studies, Master’s thesis, Nanjing University, Nanjing, China, 2020
work page 2020
-
[27]
Y. Zhang, Z.-Y. Yu, X.-Y. Li, Z.-Y. Deng and L.-J. Wen,A complete optical model for liquid-scintillator detectors, Nucl. Instrum. Meth. A967(2020) 163860 [2003.12212]
-
[28]
Comprehensive sipm mass testing for the juno-tao experiment
H. Wang, “Comprehensive sipm mass testing for the juno-tao experiment.” Neutrino 2024, 2024
work page 2024
- [29]
- [30]
-
[31]
Z. Chen,Tao electronics simulation and data analysis of prototype, Master’s thesis, Nanjing University, Nanjing, China, 2024
work page 2024
- [32]
-
[33]
Z. Xie,Research and development of key detection technologies of the tao experiment, Master’s thesis, Institute of High Energy Physics, Beijing, China, 2022
work page 2022
-
[34]
HaitzandH.Roland,Modelfortheelectricalbehaviorofamicroplasma,JournalofAppliedPhysics35(1964)1370
work page 1964
-
[35]
G. Zappalà, F. Acerbi, A. Ferri, A. Gola, G. Paternoster, V. Regazzoni et al.,Study of the photo-detection efficiency of FBK High-Density silicon photomultipliers,JINST11(2016) P11010. [46]JUNOcollaboration,SiPM and readout electronics for the JUNO-TAO Central Detector,JINST19(2024) C07008
work page 2016
-
[36]
R. Mirzoyan, R. Kosyra and H.-G. Moser,Light emission in si avalanches,Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment610(2009) 98
work page 2009
-
[37]
Modeling crosstalk and afterpulsing in silicon photomultipliers
J. Rosado, V.M. Aranda, F. Blanco and F. Arqueros,Modeling crosstalk and afterpulsing in silicon photomultipliers, Nucl. Instrum. Meth. A787(2015) 153 [1409.4564]
work page internal anchor Pith review Pith/arXiv arXiv 2015
-
[38]
S. Vinogradov,Analytical models of probability distribution and excess noise factor of solid state photomultiplier signals with crosstalk,Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment695(2012) 247. – 26 –
work page 2012
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.