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arxiv: 2604.16245 · v1 · submitted 2026-04-17 · ⚛️ physics.ins-det · hep-ex

Recognition: unknown

Performance Evaluation of Straw Tubes with Muon Beams at CERN

(2) Tufts University, (3) Institute of Nuclear Physics, 4), (4) Joint Institute for Nuclear Research, (5) University of Science, 6), (6) University of Florida, (7) CERN, (8) NRC Kurchatov Institute PNPI), Almaty, Andre Rummler (7), Artem Chukanov (4), Bing Zhou (1), Can Suslu (1), Chihao Li (1), Curtis Weaverdyck (1), Dmitry Sosnov (8), Dubna, Ekaterina Kuznetsova (3, Emmett Salzer (1), Frances Wharton (1), Hui-Chi Lin (1), Jessaly Zhu (1), Jiahao Hu (5), Jiajin Ge (1), Jianming Qian (1), Junjie Zhu (1) ((1) University of Michigan, Liang Guan (1), Linnuo Zhang (1), Ruslan Yakubovych (1), Tatiana Azaryan (2), Technology of China, Temur Enik (3, Tiesheng Dai (1), Vitalii Bautin (4), Yuxiang Guo (1)

Authors on Pith no claims yet

Pith reviewed 2026-05-10 06:44 UTC · model grok-4.3

classification ⚛️ physics.ins-det hep-ex
keywords straw tubesmuon beamsspatial resolutiondetection efficiencytest beamCERNtracking detectorsFCC-ee
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The pith

Straw tubes deliver consistent spatial resolutions and efficiencies in 150 GeV muon tests at CERN

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper reports results from two test beam campaigns that evaluate straw tube detectors as candidates for an FCC-ee straw tracker using 150 GeV muon beams at CERN. Dedicated algorithms were developed to determine single-tube spatial resolution for the primary coordinate in the r-phi plane, spatial resolution for the secondary coordinate along the tube, and detection efficiency as a function of extrapolated hit position. Both datasets produced consistent results for these performance metrics. These benchmarks supply practical data for the design, optimization, and construction of straw chambers intended for high-precision tracking applications.

Core claim

Both datasets showed consistent results for spatial resolutions and efficiency, helping to establish benchmark performance metrics for straw chambers in high-precision tracking applications.

What carries the argument

Dedicated algorithms for hit reconstruction and coordinate determination that extract single-tube spatial resolution in the r-phi plane and along the tube direction, plus efficiency versus hit position, in straw chambers exposed to muon beams.

Load-bearing premise

The custom algorithms developed for hit reconstruction and coordinate determination introduce no significant position-dependent biases or inefficiencies that would invalidate the reported resolutions and efficiencies under the test conditions.

What would settle it

Reprocessing the raw data with independent reconstruction algorithms that reveal large position-dependent variations in resolution or efficiency would show the reported consistency does not hold.

Figures

Figures reproduced from arXiv: 2604.16245 by (2) Tufts University, (3) Institute of Nuclear Physics, 4), (4) Joint Institute for Nuclear Research, (5) University of Science, 6), (6) University of Florida, (7) CERN, (8) NRC Kurchatov Institute PNPI), Almaty, Andre Rummler (7), Artem Chukanov (4), Bing Zhou (1), Can Suslu (1), Chihao Li (1), Curtis Weaverdyck (1), Dmitry Sosnov (8), Dubna, Ekaterina Kuznetsova (3, Emmett Salzer (1), Frances Wharton (1), Hui-Chi Lin (1), Jessaly Zhu (1), Jiahao Hu (5), Jiajin Ge (1), Jianming Qian (1), Junjie Zhu (1) ((1) University of Michigan, Liang Guan (1), Linnuo Zhang (1), Ruslan Yakubovych (1), Tatiana Azaryan (2), Technology of China, Temur Enik (3, Tiesheng Dai (1), Vitalii Bautin (4), Yuxiang Guo (1).

Figure 1
Figure 1. Figure 1: (a) Layout of the straw tubes; (b) Layout of the experimental setup for the 2024 test beam study; and (c) Layout of [PITH_FULL_IMAGE:figures/full_fig_p003_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: (a) Raw ADC distribution for a typical channel and an ADC cut of 100 ns was applied for this channel; and (b) drift [PITH_FULL_IMAGE:figures/full_fig_p004_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: (a) Drift time as a function of the extrapolated [PITH_FULL_IMAGE:figures/full_fig_p005_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: Dependencies of the extracted wire position as a function of the track [PITH_FULL_IMAGE:figures/full_fig_p005_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: (a) Single tube spatial resolution as a function of the drift radius for two typical straw tubes; and (b) The residual [PITH_FULL_IMAGE:figures/full_fig_p006_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: The residual distribution for the secondary coordinate measurement. [PITH_FULL_IMAGE:figures/full_fig_p006_6.png] view at source ↗
Figure 7
Figure 7. Figure 7: Detection efficiency as a function of the extrapolated position from tracks reconstructed by the AZALEA telescope [PITH_FULL_IMAGE:figures/full_fig_p007_7.png] view at source ↗
Figure 8
Figure 8. Figure 8: (a) Distribution of the angular deviation; (b) Distribution of the extrapolated position deviation at the center of the [PITH_FULL_IMAGE:figures/full_fig_p008_8.png] view at source ↗
Figure 9
Figure 9. Figure 9: (a) Display of an event with the muon hits several wires and tube walls leading to only three drift circles found; and [PITH_FULL_IMAGE:figures/full_fig_p009_9.png] view at source ↗
Figure 10
Figure 10. Figure 10: (a) Average width of the unbiased residual as a function of the extrapolated position; and (b) Distribution of the [PITH_FULL_IMAGE:figures/full_fig_p009_10.png] view at source ↗
Figure 11
Figure 11. Figure 11: Detection efficiency as a function of the extrapolated position from tracks reconstructed by the sMDT chambers for [PITH_FULL_IMAGE:figures/full_fig_p010_11.png] view at source ↗
Figure 12
Figure 12. Figure 12: (a) Distribution of the effective diameter of 20 tubes; and (b) Distribution of the tube wire offset from the center [PITH_FULL_IMAGE:figures/full_fig_p010_12.png] view at source ↗
Figure 13
Figure 13. Figure 13: (a) The width of the secondary coordinate residual at different [PITH_FULL_IMAGE:figures/full_fig_p011_13.png] view at source ↗
read the original abstract

We present results from two test beam campaigns that investigate the performance of straw tube detectors as potential candidates for an FCC-ee straw tracker. These studies were carried out at CERN using 150 GeV muon beams. Dedicated algorithms were developed to determine both single tube spatial resolution for the primary coordinate in the $r-\phi$ plane and spatial resolution for the secondary coordinate along the tube direction within a straw chamber. Detection efficiency was also evaluated as a function of the extrapolated hit position for each tube. Both datasets showed consistent results for spatial resolutions and efficiency. Our findings will help establish benchmark performance metrics and provide valuable insight for future design, optimization, and construction of straw chambers for high-precision tracking applications.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

1 major / 2 minor

Summary. The paper reports results from two test beam campaigns at CERN using 150 GeV muon beams to evaluate straw tube detectors as candidates for an FCC-ee straw tracker. Dedicated algorithms are presented for extracting the primary r-φ spatial resolution from drift time and the secondary along-tube coordinate, with detection efficiency measured as a function of extrapolated hit position; both datasets yield consistent resolutions and efficiencies, intended to establish benchmark metrics for future straw chamber design and optimization.

Significance. If the reconstruction algorithms prove unbiased, these direct experimental measurements from controlled beam tests would supply valuable benchmark data for high-precision tracking detectors, with the cross-campaign consistency providing a basic check on reproducibility. The work is grounded in experimental data rather than derivations or fitted parameters.

major comments (1)
  1. [Algorithm description section] The section describing the dedicated algorithms for primary (r-φ drift-time) and secondary (along-tube) coordinate determination: no Monte Carlo closure tests, no comparison to independent methods (e.g., centroid or template fits), and no quantification of position-dependent biases or inefficiencies as a function of drift distance or hit position are provided. These omissions are load-bearing because the reported single-tube resolutions and efficiencies rest directly on the assumption that the algorithms introduce no significant systematics.
minor comments (2)
  1. [Results figures] Efficiency versus position plots would be clearer with statistical error bars or uncertainty bands to allow readers to judge the significance of any observed position dependence.
  2. [Introduction] The manuscript would benefit from citing earlier straw-tube beam-test results to place the achieved resolutions in context.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for the careful and constructive review of our manuscript. The major comment on the algorithm description section raises a valid point about validation, and we address it directly below with a commitment to revisions that strengthen the presentation without altering the core experimental results.

read point-by-point responses
  1. Referee: [Algorithm description section] The section describing the dedicated algorithms for primary (r-φ drift-time) and secondary (along-tube) coordinate determination: no Monte Carlo closure tests, no comparison to independent methods (e.g., centroid or template fits), and no quantification of position-dependent biases or inefficiencies as a function of drift distance or hit position are provided. These omissions are load-bearing because the reported single-tube resolutions and efficiencies rest directly on the assumption that the algorithms introduce no significant systematics.

    Authors: We agree that explicit validation of the reconstruction algorithms is important to confirm the absence of significant systematics. The primary coordinate algorithm converts drift time to radial distance using a data-driven calibration derived from the 150 GeV muon tracks, while the secondary coordinate uses a charge-division method along the straw length; both are standard for this detector type. The manuscript does not contain Monte Carlo closure tests or direct comparisons to centroid or template-fitting approaches, nor does it include explicit plots of residuals versus drift distance. However, the reported consistency of resolutions and efficiencies across two independent beam campaigns already provides an empirical reproducibility check. To address the concern, we will revise the algorithm section to add: (i) quantification of position-dependent effects by showing mean residuals and efficiency as functions of drift distance and extrapolated hit position (building on the existing efficiency-vs-position data), and (ii) a short discussion of why alternative methods were not implemented, noting that the chosen algorithms are optimized for the single-tube geometry and high-rate environment. If a lightweight Monte Carlo can be generated from the existing calibration without new data, we will include a closure test; otherwise we will clearly state the data-driven nature of the validation. These changes will be incorporated in the revised manuscript. revision: yes

Circularity Check

0 steps flagged

No circularity: direct experimental measurements with no derivations or self-referential predictions

full rationale

The paper reports experimental beam-test results for straw-tube spatial resolution and efficiency using muon beams at CERN. No derivation chain, first-principles predictions, fitted parameters renamed as predictions, or self-citations of uniqueness theorems appear in the abstract or described methodology. The central claims rest on measured data consistency between two datasets after applying custom hit-reconstruction algorithms; these algorithms are presented as tools for extracting observables rather than as self-defining or self-predicting constructs. The reported resolutions and efficiencies are therefore independent experimental outputs, not reductions to inputs by construction. This is the expected outcome for a pure performance-evaluation paper.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

This is a pure experimental characterization study. No mathematical derivations, fitted parameters, background axioms, or postulated entities are introduced.

pith-pipeline@v0.9.0 · 5631 in / 965 out tokens · 23688 ms · 2026-05-10T06:44:42.641762+00:00 · methodology

discussion (0)

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Reference graph

Works this paper leans on

16 extracted references · 16 canonical work pages

  1. [1]

    Abada, et al., FCC Physics Opportunities: Future Circular Collider Conceptual Design Report Volume 1, Eur

    A. Abada, et al., FCC Physics Opportunities: Future Circular Collider Conceptual Design Report Volume 1, Eur. Phys. J. C 79 (6) (2019) 474.doi:10.1140/epjc/s10052-019-6904-3

  2. [2]

    doi:10.1140/epjst/e2019-900045-4

    A. Abada, et al., FCC-ee: The Lepton Collider: Future Circular Collider Conceptual Design Report Volume 2, Eur. Phys. J. ST 228 (2) (2019) 261–623.doi:10.1140/epjst/e2019-900045-4

  3. [3]

    Benedikt, et al., Future Circular Collider Feasibility Study Report: Volume 1, Physics, Experiments, Detectors, Eur

    M. Benedikt, et al., Future Circular Collider Feasibility Study Report: Volume 1, Physics, Experiments, Detectors, Eur. Phys. J. C 85 (12) (2025) 1468.arXiv:2505.00272,doi:10.1140/epjc/s10052-025-15077-x

  4. [4]

    Benedikt, et al., Future Circular Collider Feasibility Study Report: Volume 2, Accelerators, Technical Infrastructure and Safety, Eur

    M. Benedikt, et al., Future Circular Collider Feasibility Study Report: Volume 2, Accelerators, Technical Infrastructure and Safety, Eur. Phys. J. ST 234 (19) (2025) 5713–6197.arXiv:2505.00274,doi:10.1140/epjs/s11734-025-01967-4

  5. [5]

    Benedikt, et al., Future Circular Collider Feasibility Study Report: Volume 3 Civil Engineering, Implementation and Sustainability, Eur

    M. Benedikt, et al., Future Circular Collider Feasibility Study Report: Volume 3 Civil Engineering, Implementation and Sustainability, Eur. Phys. J. ST 234 (17) (2025) 5113–5383, [Erratum: Eur. Phys. J. ST 234, 33–44 (2025)].arXiv: 2505.00273,doi:10.1140/epjs/s11734-025-01958-5

  6. [6]

    Dam, Detector requirements, design, and technologies for the FCC-ee Higgs, electroweak, and top factory, Nucl

    M. Dam, Detector requirements, design, and technologies for the FCC-ee Higgs, electroweak, and top factory, Nucl. Instrum. Meth. A 1080 (2025) 170648.arXiv:2505.06781,doi:10.1016/j.nima.2025.170648

  7. [7]

    Jansen, et al., Performance of the EUDET-type beam telescopes, EPJ Tech

    H. Jansen, et al., Performance of the EUDET-type beam telescopes, EPJ Tech. Instrum. 3 (2016) 7.doi:10.1140/epjti/ s40485-016-0033-2

  8. [8]

    Garcia-Sciveres, et al., The FE-I4 pixel readout integrated circuit, Nucl

    M. Garcia-Sciveres, et al., The FE-I4 pixel readout integrated circuit, Nucl. Instrum. Meth. A 636 (2011) S155–S159. doi:10.1016/j.nima.2010.04.101

  9. [9]

    Amidei, et al., Construction of precision sMDT detector for the ATLAS Muon Spectrometer upgrade, JINST 18 (01) (2023) P01041.arXiv:2211.00714,doi:10.1088/1748-0221/18/01/P01041

    D. Amidei, et al., Construction of precision sMDT detector for the ATLAS Muon Spectrometer upgrade, JINST 18 (01) (2023) P01041.arXiv:2211.00714,doi:10.1088/1748-0221/18/01/P01041. 11

  10. [10]

    H. Kroha, et al., Performance of the new amplifier-shaper-discriminator chip for the ATLAS MDT chambers at the HL- LHC, in: 2015 IEEE Nuclear Science Symposium and Medical Imaging Conference, 2016, p. 7581979.arXiv:1603.09093, doi:10.1109/NSSMIC.2015.7581979

  11. [11]

    De Matteis, F

    M. De Matteis, F. Resta, R. Richter, H. Kroha, M. Fras, Y. Zhao, S. Abovyan, A. Baschirotto, An eight-channels 0.13- µm-CMOS front end for ATLAS muon-drift-tubes detectors, IEEE Sensors J. 17 (11) (2017) 3406–3415.doi:10.1109/ JSEN.2017.2694606

  12. [12]

    J. Wang, Y. Liang, X. Xiao, Q. An, J. W. Chapman, T. Dai, B. Zhou, J. Zhu, L. Zhao, Development of a time-to-digital converter ASIC for the upgrade of the ATLAS Monitored Drift Tube detector, Nucl. Instrum. Meth. A 880 (2018) 174–180. arXiv:1708.03692,doi:10.1016/j.nima.2017.10.077

  13. [13]

    Liang, et al., Design and performance of a TDC ASIC for the upgrade of the ATLAS Monitored Drift Tube detector, Nucl

    Y. Liang, et al., Design and performance of a TDC ASIC for the upgrade of the ATLAS Monitored Drift Tube detector, Nucl. Instrum. Meth. A 939 (2019) 10–15.arXiv:1903.06995,doi:10.1016/j.nima.2019.05.050

  14. [14]

    Arai, et al., ATLAS muon drift tube electronics, JINST 3 (2008) P09001.doi:10.1088/1748-0221/3/09/P09001

    Y. Arai, et al., ATLAS muon drift tube electronics, JINST 3 (2008) P09001.doi:10.1088/1748-0221/3/09/P09001

  15. [15]

    Penski, Test result of the new ASD2 chips for Phase-II upgrade of the ATLAS MDT chambers at HL-LHC, JINST 19 (05) (2024) C05008.doi:10.1088/1748-0221/19/05/C05008

    K. Penski, Test result of the new ASD2 chips for Phase-II upgrade of the ATLAS MDT chambers at HL-LHC, JINST 19 (05) (2024) C05008.doi:10.1088/1748-0221/19/05/C05008

  16. [16]

    Y. Guo, X. Hu, T. Schwarz, B. Zhou, J. Zhu, Development and test of a mini-Data Acquisition system for the High- Luminosity LHC upgrade of the ATLAS Monitored Drift Tube detector, Nucl. Instrum. Meth. A 1046 (2023) 167671. arXiv:2205.13475,doi:10.1016/j.nima.2022.167671. 12