Measurement of the scintillation resolution in liquid xenon and its impact for future segmented calorimeters
Pith reviewed 2026-05-24 11:20 UTC · model grok-4.3
The pith
Liquid xenon scintillation achieves 3.7% energy resolution at 511 keV after saturation correction.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The central claim is that liquid xenon, when read out solely via scintillation light in a light-collection-optimized setup, delivers a saturation-corrected energy resolution of 3.7 ± 0.4% at 511 keV that lies close to the Poissonian expectation of 2.8 ± 0.4%, while the intrinsic resolution component of 2.3 ± 0.8% agrees with the longstanding theoretical estimate of 1.8%.
What carries the argument
The light-collection-optimized detector using VUV-sensitive SiPMs together with saturation-effect corrections applied to the scintillation signals.
If this is right
- Modular liquid-xenon scintillation detectors become competitive building blocks for segmented calorimeters.
- Scintillation-only readout in liquid xenon opens practical designs for positron emission tomography systems.
- Energy resolution near the statistical limit reduces the need for additional charge readout in xenon-based detectors.
Where Pith is reading between the lines
- Similar resolution measurements at higher energies could test whether the intrinsic component remains constant or scales with energy.
- The result invites direct comparison of scintillation-only xenon modules against hybrid charge-plus-light systems in the same calorimeter geometry.
Load-bearing premise
The setup truly maximizes light collection so that the calculated Poissonian limit of 2.8% accurately reflects the number of detected photons.
What would settle it
A repeat measurement at 511 keV that yields a saturation-corrected resolution substantially larger than 3.7% while using the same light-collection geometry and SiPMs would falsify the reported performance.
Figures
read the original abstract
We report on a new measurement of the energy resolution that can be attained in liquid xenon when recording only the scintillation light. Our setup is optimized to maximize light collection, and uses state-of-the-art, high-PDE, VUV-sensitive silicon photomultipliers. We find a value of 3.7 $\pm$ 0.4% at 511 keV, once saturation effects are corrected for, a result close to the Poissonian resolution that we expect in our setup (2.8 $\pm$ 0.4% $\sigma$ at 511 keV). Our results in the intrinsic resolution (2.3 $\pm$ 0.8 %) are compatible, within errors, at 511 keV, with those found by theoretical estimations which have been standing for the last twenty years, 1.8%. Our work opens new possibilities for apparatus based on liquid xenon and using scintillation only. In particular it suggests that modular scintillation detectors using liquid xenon can be very competitive as building blocks in segmented calorimeters, with applications to Positron Emission Tomography technology.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript reports an experimental measurement of the scintillation energy resolution in liquid xenon using an optimized setup with high-PDE VUV-sensitive SiPMs. After applying a saturation correction, the total resolution is found to be 3.7 ± 0.4% at 511 keV, stated to be close to the Poissonian expectation of 2.8 ± 0.4%. An intrinsic resolution of 2.3 ± 0.8% is extracted and reported as compatible within errors with long-standing theoretical estimates of 1.8%. The work concludes that scintillation-only LXe detectors can be competitive building blocks for segmented calorimeters, with potential PET applications.
Significance. If the measurement and its comparison to the Poisson limit hold after verification of the analysis chain, the result would be significant for noble-liquid detector development. It supplies the first direct experimental test in a maximized-light-collection configuration that the resolution can approach the statistical floor, lending support to theoretical intrinsic-resolution predictions that have stood for two decades without experimental confrontation. This strengthens the case for modular LXe scintillation detectors in medical imaging and particle-physics calorimetry.
major comments (2)
- [Abstract / Results (saturation correction)] Abstract and saturation-correction paragraph in Results: Both the reported 3.7 ± 0.4% resolution and the 2.8 ± 0.4% Poisson expectation are obtained only after the same saturation correction is applied to determine the number of detected photons. Because an error in the correction parameters (PDE, cross-talk, recovery time) shifts both quantities in the same direction, the claim that the measured value is “close to the Poissonian resolution” is not independent of the correction model. The functional form of the correction and the numerical values adopted for its parameters must be stated explicitly so that the robustness of the comparison can be assessed.
- [Results (intrinsic resolution extraction)] Section describing extraction of intrinsic resolution: The intrinsic resolution is quoted as 2.3 ± 0.8% and declared compatible with the 1.8% theoretical value, yet the procedure used to isolate the intrinsic component (quadratic subtraction, direct fit, or other) and the propagation of uncertainties that yields the ±0.8% error are not specified. Without this information the compatibility statement cannot be evaluated quantitatively.
minor comments (2)
- [Abstract] The abstract writes “2.8 ± 0.4% σ”; the notation is slightly redundant. Consider “2.8 ± 0.4% (σ)” for clarity.
- [Introduction] The specific references supporting the “theoretical estimations … 1.8%” that have stood for twenty years should be cited explicitly in the introduction or discussion.
Simulated Author's Rebuttal
We thank the referee for the positive assessment of the significance of our work and for the constructive comments. We address each major comment below and will revise the manuscript to incorporate the requested clarifications on the analysis methods.
read point-by-point responses
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Referee: [Abstract / Results (saturation correction)] Abstract and saturation-correction paragraph in Results: Both the reported 3.7 ± 0.4% resolution and the 2.8 ± 0.4% Poisson expectation are obtained only after the same saturation correction is applied to determine the number of detected photons. Because an error in the correction parameters (PDE, cross-talk, recovery time) shifts both quantities in the same direction, the claim that the measured value is “close to the Poissonian resolution” is not independent of the correction model. The functional form of the correction and the numerical values adopted for its parameters must be stated explicitly so that the robustness of the comparison can be assessed.
Authors: We agree that explicit documentation of the saturation correction is necessary to allow independent evaluation of the comparison. In the revised manuscript we will add a dedicated subsection (or expand the existing paragraph) that states the functional form of the correction (a standard model accounting for SiPM saturation, cross-talk, and afterpulsing) together with the numerical values adopted for PDE, cross-talk probability, and recovery time. This will enable readers to test the sensitivity of both the measured resolution and the Poisson expectation to variations in these parameters. revision: yes
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Referee: [Results (intrinsic resolution extraction)] Section describing extraction of intrinsic resolution: The intrinsic resolution is quoted as 2.3 ± 0.8% and declared compatible with the 1.8% theoretical value, yet the procedure used to isolate the intrinsic component (quadratic subtraction, direct fit, or other) and the propagation of uncertainties that yields the ±0.8% error are not specified. Without this information the compatibility statement cannot be evaluated quantitatively.
Authors: We acknowledge that the extraction procedure and uncertainty propagation were not described with sufficient detail. The intrinsic resolution was isolated via quadratic subtraction, σ_intrinsic = √(σ_total² − σ_Poisson²), with the quoted uncertainty obtained by standard Gaussian error propagation that includes the uncertainties on both the total and Poisson terms. In the revised manuscript we will insert a short paragraph (or subsection) in the Results section that explicitly states this method and the propagation formula, allowing quantitative assessment of the compatibility with the 1.8% theoretical value. revision: yes
Circularity Check
No significant circularity in direct experimental measurement
full rationale
This paper reports a direct experimental measurement of scintillation energy resolution in liquid xenon using optimized SiPM light collection. The reported 3.7% resolution (after saturation correction) and the 2.8% Poisson expectation are both derived from the same dataset, but the Poisson limit is the standard statistical floor 1/sqrt(N) computed from the mean photoelectron count; the measured width is the observed distribution width. Subtracting to obtain the 2.3% intrinsic resolution follows the conventional quadrature procedure and does not reduce any claimed result to a self-defined quantity or a fitted parameter renamed as a prediction. No derivation chain, self-citation load-bearing step, or ansatz is present. The work is self-contained against external benchmarks (prior theoretical estimates of 1.8%) and does not invoke any of the enumerated circularity patterns.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption Theoretical intrinsic resolution in liquid xenon is 1.8% at 511 keV
Reference graph
Works this paper leans on
- [1]
-
[2]
S. Vandeberghe, P. Moskal, and J. Karp, State of the art in total body pet, EJNMMI Physics 7, 35 (2020)
work page 2020
-
[3]
V. Westerwoudt, M. Conti, and L. Eriksson, Advantages of improved time resolution for TOF PET at very low statistics, IEEE Trans. Nucl. Sci. 61, 126 (2014)
work page 2014
-
[4]
M. Conti and B. Bendriem, The new opportunities for high time resolution clinical TOF PET, Clinical and Translational Imaging 7, 139 (2019)
work page 2019
-
[5]
S. R. Cherry et al. , Total-body PET: Maximizing sen- sitivity to create new opportunities for clinical research and patient care, J. Nucl. Med. 59, 3 (2018)
work page 2018
-
[6]
R. D. Badawi et al. , First human imaging studies with the EXPLORER total-body PET scanner, J. Nucl. Med. 60, 299 (2019)
work page 2019
-
[8]
K. Fujii et al., High-accuracy measurement of the emis- sion spectrum of liquid xenon in the vacuum ultraviolet region, Nuclear Instruments and Methods in Physics Re- search Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 795, 293 (2015)
work page 2015
-
[9]
Liquid noble gas detectors for low energy particle physics
V. Chepel and H. Araujo, Liquid noble gas detec- tors for low energy particle physics, JINST 8, R04001, arXiv:1207.2292 [physics.ins-det]
work page internal anchor Pith review Pith/arXiv arXiv
-
[10]
Gallucci, The meg liquid xenon calorimeter, Journal of Physics: Conference Series 160, 012011 (2009)
G. Gallucci, The meg liquid xenon calorimeter, Journal of Physics: Conference Series 160, 012011 (2009)
work page 2009
-
[11]
G. Anton et al. (EXO-200 Collaboration), Search for neutrinoless double-β decay with the complete exo-200 dataset, Phys. Rev. Lett. 123, 161802 (2019)
work page 2019
-
[12]
G. Adhikari et al. , Journal of Physics G: Nuclear and Particle Physics 49, 015104 (2021)
work page 2021
-
[13]
J. Aalbers et al. , DARWIN: towards the ultimate dark matter detector, Journal of Cosmology and Astroparticle Physics 2016 (11), 017
work page 2016
-
[14]
G. Anton et al. , Measurement of the scintillation and ionization response of liquid xenon at MeV energies in the EXO-200 experiment, Physical Review C 101, 10.1103/physrevc.101.065501 (2020)
-
[15]
Lavoie, Liquid xenon scintillators for imaging of positron emitters, Med
L. Lavoie, Liquid xenon scintillators for imaging of positron emitters, Med. Phys. 3 (5) , 283 (1976)
work page 1976
-
[16]
V. Chepel et al., The liquid xenon detector for PET: re- cent results, IEEE Transactions on Nuclear Science NS- 46, 1038 (1999)
work page 1999
-
[17]
P. Crespo et al. , Pulse processing for the PET liquid xenon Multiwire Ionisation Chamber, IEEE Transactions on Nuclear Science 47, 2119 (1999)
work page 1999
-
[18]
T. Doke, J. Kikuchi, and F. Nishikido, Time-of-flight positron emission tomography using liquid xenon scin- tillation, Nucl. Instrum. Methods A 569, 863 (2006)
work page 2006
-
[19]
Miceli, Liquid xenon detectors for positron emission tomography, J
A. Miceli, Liquid xenon detectors for positron emission tomography, J. Phys. Conf. Ser. 312, 062006 (2011)
work page 2011
-
[20]
Y. Z. ane others, Studies and optimization of scintillation light measurements for the development of the 3-gamma medical imaging xemis2 liquid xenon compton camera, Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment , 167794 (2022)
work page 2022
-
[21]
Chepel, Liquid xenon detectors for medical imaging, Revista do Detua 4 (2007)
V. Chepel, Liquid xenon detectors for medical imaging, Revista do Detua 4 (2007)
work page 2007
-
[22]
J. J. Gomez-Cadenas et al. , Investigation of the Coin- cidence Resolving Time performance of a PET scanner based on liquid xenon: A Monte Carlo study, JINST 11 (09), P09011, arXiv:1604.04106 [physics.ins-det]
work page internal anchor Pith review Pith/arXiv arXiv
-
[23]
J. J. Gomez-Cadenas, J. M. Benlloch-Rodr´ ıguez, and P. Ferrario, Monte Carlo study of the Coincidence Resolving Time of a liquid xenon PET scanner, us- ing Cherenkov radiation, JINST 12 (08), P08023, arXiv:1706.07629 [physics.ins-det]
work page internal anchor Pith review Pith/arXiv arXiv
-
[24]
V. Herrero-Bosch et al., PETALO read-out: A novel ap- proach for data acquisition systems in PET applications, in 2018 IEEE Nuclear Science Symposium and Medical Imaging Conference (NSS/MIC) (2018)
work page 2018
-
[25]
J. Renner et al. , Processing of Compton events in the PETALO readout system, in 2019 IEEE Nuclear Sci- ence Symposium (NSS) and Medical Imaging Conference 7 (MIC) (2019) pp. 1–7, arXiv:2001.04724 [physics.ins-det]
-
[26]
P. Ferrario et al. , PETALO: Time-of-Flight PET with liquid xenon, in 2018 IEEE Nuclear Science Symposium and Medical Imaging Conference (NSS/MIC) (2018) arXiv:1911.10994 [physics.ins-det]
-
[27]
J. Renner et al. , Monte carlo characterization of PETALO, a full-body liquid xenon-based PET detector, Journal of Instrumentation 17, P05044
-
[28]
T. Doke, R. Sawada, and H. Tawara, Non-proportionality of the scintillation yield in liquid xenon and its effect on the energy resolution for gamma-rays, Technique and Application of Xenon Detectors , 17 (2003)
work page 2003
-
[29]
M. Szydagis et al. , Noble element simulation technique v2.0 (version v2.0.0), Zenodo 10.5281/zenodo.1314669 (2018)
-
[30]
Gamma Ray Spectroscopy with Scintillation Light in Liquid Xenon
K. Ni et al. , Gamma Ray Spectroscopy with Scin- tillation Light in Liquid Xenon, JINST 1, P09004, arXiv:physics/0608034 [physics]
work page internal anchor Pith review Pith/arXiv arXiv
-
[31]
A. Baldini et al., Absorption of scintillation light in a 100 l liquid xenon gamma-ray detector and expected detec- tor performance, Nuclear Instruments and Methods in Physics Research Section A 545, 753 (2005)
work page 2005
-
[32]
D. Akerib et al. , Technical results from the surface run of the lux dark matter experiment, Astroparticle Physics 45, 34 (2013)
work page 2013
-
[33]
M. Yamashita et al. , Scintillation response of liquid xe surrounded by ptfe reflector for gamma rays, Nuclear In- struments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 535, 692 (2004)
work page 2004
-
[34]
A. Di Francesco et al., Tofpet2: a high- performance asic for time and amplitude measurements of sipm signals in time-of-flight applications, JINST 11 (3), C03042
-
[35]
S. Agostinelli et al. , GEANT4 - a simulation toolkit, Nucl. Instrum. Meth. A 506, 250 (2003)
work page 2003
-
[36]
V. Solovov et al. , Measurement of the refractive index and attenuation length of liquid xenon for its scintillation light, Nucl. Instrum. Meth. A 516, 462 (2004)
work page 2004
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