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arxiv: 2606.30150 · v1 · pith:LNUZYH5Lnew · submitted 2026-06-29 · ⚛️ physics.ins-det

Charge sharing and alignment performance of bent ALPIDEs measured with low-energy protons

Pith reviewed 2026-06-30 03:40 UTC · model grok-4.3

classification ⚛️ physics.ins-det
keywords ALPIDEbent MAPScluster sizealignmentproton scatteringALICE ITS3CMOS sensors
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0 comments X

The pith

Bent ALPIDE chips show no change in cluster size from curvature and reach simulated resolutions in low-energy proton tests.

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

The study tests ALPIDE CMOS sensors bent to radii of 18 mm, 24 mm and 30 mm using 80 MeV, 120 MeV and 200 MeV protons scattered elastically from a polypropylene fiber. Cluster sizes in high-energy-loss events remain statistically unchanged compared with expectations for flat sensors. Track alignment is assessed through the distance of closest approach and the opening angle between opposing proton tracks, yielding spatial resolutions that agree with Monte Carlo predictions. These measurements serve as a proxy for the conditions expected in the curved inner layers of the ALICE ITS3 upgrade.

Core claim

Bending the ALPIDE sensors produces no measurable effect on cluster size distributions under the high dE/dx conditions provided by the low-momentum protons; the alignment residuals obtained from DCA and opening-angle observables match the values predicted by simulation, thereby validating the use of bent wafer-scale MAPS for future tracking systems.

What carries the argument

Cluster-size histograms and the distance-of-closest-approach plus opening-angle benchmarks extracted from two-arm proton-track reconstructions.

If this is right

  • Bending radii down to 18 mm can be adopted without redesign of the front-end electronics or clustering algorithms.
  • Existing alignment procedures developed for flat ALPIDE planes remain applicable once the sensor curvature is accounted for in the geometry model.
  • The same proton-scattering setup can serve as a calibration source for other bent MAPS prototypes.
  • Charge-sharing behavior in bent sensors is sufficiently stable to support the target position resolution of the ITS3 innermost layers.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The absence of bending-induced cluster-size changes suggests that mechanical stress does not alter the epitaxial-layer electric-field configuration at the tested radii.
  • Similar tests with higher-momentum particles or different sensor thicknesses would further constrain any residual curvature dependence.
  • The demonstrated alignment precision supports extending the approach to full-wafer-scale bent sensors in other collider or fixed-target experiments.

Load-bearing premise

The low-momentum protons produced by elastic scattering on the polypropylene fiber reproduce the high-energy-loss and alignment conditions that will exist inside the bent ITS3 layers.

What would settle it

A statistically significant difference in measured cluster sizes between bent and flat sensors, or alignment resolutions that deviate from the simulated expectations by more than the reported uncertainties.

Figures

Figures reproduced from arXiv: 2606.30150 by Alex Kluge, Alperen Y\"unc\"u, Andrea Rossi, Berkin Ulukutlu, Christopher Ehrich, Fabrizio Grosa, Hartmut Hillemanns, Isabella Sannaa, Laszlo Vargaa, Laura Fabbietti, Lukas Lautner, Lukas Ponnath, Magnus Mager, Miljenko \v{S}ulji\'c, Roman Gernh\"auser, Serhiy Senyukov Johanna Stachele, Tobias Jenegger.

Figure 1
Figure 1. Figure 1: Photos of the detector setup. The used target fiber array (top left). [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: Sketch depicting an example event. The proton beams of various [PITH_FULL_IMAGE:figures/full_fig_p003_2.png] view at source ↗
Figure 4
Figure 4. Figure 4: Distribution of impact angles between reconstructed tracks of interest [PITH_FULL_IMAGE:figures/full_fig_p004_4.png] view at source ↗
Figure 3
Figure 3. Figure 3: Raw cluster size distribution at 200 MeV proton energy and 100 e [PITH_FULL_IMAGE:figures/full_fig_p004_3.png] view at source ↗
Figure 5
Figure 5. Figure 5: Average cluster size distribution from tracks associated to a vertex in [PITH_FULL_IMAGE:figures/full_fig_p005_5.png] view at source ↗
Figure 7
Figure 7. Figure 7: Average cluster size as a function of the proton momentum from the [PITH_FULL_IMAGE:figures/full_fig_p006_7.png] view at source ↗
Figure 8
Figure 8. Figure 8: Example distributions of the residuals to the event plane for the di [PITH_FULL_IMAGE:figures/full_fig_p007_8.png] view at source ↗
Figure 10
Figure 10. Figure 10: The projections of the vertex distributions after alignment, (left) front-view, (middle) top-view, (right) side-view of the target array. [PITH_FULL_IMAGE:figures/full_fig_p008_10.png] view at source ↗
Figure 11
Figure 11. Figure 11: DCA distributions obtained for the final alignment, compared to [PITH_FULL_IMAGE:figures/full_fig_p008_11.png] view at source ↗
Figure 12
Figure 12. Figure 12: Opening angle from selected elastic scattering events compared to [PITH_FULL_IMAGE:figures/full_fig_p009_12.png] view at source ↗
read the original abstract

The upgrade of the ALICE experiments Inner Tracking System (ITS3) aims to replace its innermost detection layers with bent wafer-scale CMOS MAPS sensors. This study examines the performance of ALPIDE chips, currently used in the ALICE ITS2, when operated in a bent configuration under realistic experimental conditions. Proton beams with energies of 80 MeV, 120 MeV and 200 MeV were used to study proton-proton elastic scattering on a polypropylene fiber target reconstructed using two opposing arms of trackers with sensors bent to radii of 18 mm, 24 mm and 30 mm. The measured low-momentum protons provided a testbed for investigating clustering behavior in high-energy loss events, where no significant impact of bending was observed on cluster size. Additionally, alignment strategies for bent detectors were evaluated using the distance of closest approach (DCA) and opening angle between scattered proton tracks as benchmarks. The achieved resolution matches expectations from simulations, confirming the suitability of bent MAPS sensors for future high-energy and nuclear physics 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 / 0 minor

Summary. The manuscript reports measurements of ALPIDE sensors bent to radii of 18 mm, 24 mm and 30 mm using 80–200 MeV protons from elastic scattering on a polypropylene fiber target. It finds no significant change in cluster size due to bending for these high-dE/dx events and reports that alignment performance, benchmarked via distance of closest approach and opening angle, matches simulation expectations, concluding that bent MAPS sensors are suitable for ITS3 and similar applications.

Significance. If the central measurements hold, the work supplies direct experimental data on charge-sharing behavior and alignment in bent wafer-scale sensors under high ionization density, which is useful for nuclear-physics tracking. The significance for the ITS3 upgrade is more limited, however, because the test particles are not minimum-ionizing and the paper provides no evidence that bending-induced charge-sharing effects are independent of dE/dx.

major comments (1)
  1. [Abstract and final section] Abstract and final section: the claim that the results 'confirm the suitability of bent MAPS sensors for future high-energy and nuclear physics applications' is load-bearing for the paper's motivation yet rests on an untested extrapolation. The measurements use protons whose dE/dx is far above minimum-ionizing; no data, scaling argument, or simulation comparison is supplied to show that the observed null result on cluster size would persist for MIPs that dominate ITS3 tracking.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for the constructive feedback. We address the single major comment below and agree that a revision to the scope of the conclusions is warranted.

read point-by-point responses
  1. Referee: [Abstract and final section] Abstract and final section: the claim that the results 'confirm the suitability of bent MAPS sensors for future high-energy and nuclear physics applications' is load-bearing for the paper's motivation yet rests on an untested extrapolation. The measurements use protons whose dE/dx is far above minimum-ionizing; no data, scaling argument, or simulation comparison is supplied to show that the observed null result on cluster size would persist for MIPs that dominate ITS3 tracking.

    Authors: We agree that the measurements were performed exclusively with 80–200 MeV protons (high dE/dx) and that no direct data, scaling argument, or MIP-specific simulation is presented to demonstrate that the null result on bending-induced cluster-size change holds for minimum-ionizing particles. The experiment was designed to study charge-sharing behavior under high ionization density, which is relevant for certain nuclear-physics use cases. Alignment performance was benchmarked against simulation and found to agree, independent of the dE/dx regime. To address the concern, we will revise the abstract and concluding section to remove the broad claim of suitability for high-energy physics applications and instead state that the results support the use of bent MAPS for tracking in high-dE/dx environments while noting that MIP-specific validation remains desirable. revision: yes

Circularity Check

0 steps flagged

No circularity in experimental measurement and simulation comparison

full rationale

This is a direct experimental study reporting measurements of cluster size, alignment metrics (DCA, opening angle), and resolution for bent ALPIDE sensors using low-energy proton beams. No derivations, equations, fitted parameters renamed as predictions, or self-citation chains are present in the provided text or abstract. Claims rest on observed data compared to external simulations, with no reduction of results to the paper's own inputs by construction. The derivation chain is self-contained.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The central claim rests on standard assumptions in particle detection that the chosen proton scattering kinematics produce representative high dE/dx events and that simulation models of bent sensors are sufficiently accurate for comparison.

axioms (1)
  • domain assumption Proton-proton elastic scattering on polypropylene provides a suitable testbed for high-energy-loss clustering and alignment benchmarks representative of ITS3 conditions.
    Invoked to justify the use of 80-200 MeV protons as the experimental probe.

pith-pipeline@v0.9.1-grok · 5800 in / 1224 out tokens · 62352 ms · 2026-06-30T03:40:43.305510+00:00 · methodology

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Reference graph

Works this paper leans on

28 extracted references · 16 canonical work pages

  1. [1]

    Colella, Upgrade of the ALICE experiment beyond LHC Run 3, International Journal of Modern Physics E-nuclear Physics (2022)

    D. Colella, Upgrade of the ALICE experiment beyond LHC Run 3, International Journal of Modern Physics E-nuclear Physics (2022). doi:10.1142/s021830132240002x

  2. [2]

    P. G. Kuijer, The alice experiment at the CERN LHC, null (2003). doi:10.1016/s0920-5632(03)90488-9

  3. [3]

    Kluge, et al., ALICE – ITS3 — A bent, wafer-scale CMOS de- tector, Nuclear Instruments and Methods in Physics Research (2022)

    A. Kluge, et al., ALICE – ITS3 — A bent, wafer-scale CMOS de- tector, Nuclear Instruments and Methods in Physics Research (2022). doi:10.1016/j.nima.2022.167315

  4. [4]

    rep., CERN, Geneva, co-project Manager: Magnus Mager, mag- nus.mager@cern.chds (2024)

    ALICE Collaboration, Technical Design report for the ALICE Inner Tracking System 3 - ITS3 ; A bent wafer-scale monolithic pixel detector, Tech. rep., CERN, Geneva, co-project Manager: Magnus Mager, mag- nus.mager@cern.chds (2024). URLhttps://cds.cern.ch/record/2890181

  5. [7]

    Reidt, Upgrade of the ALICE ITS detector, Nuclear Instru- ments and Methods in Physics Research Section A : Accelera- tors, Spectrometers, Detectors and Associated Equipment (2021)

    F. Reidt, Upgrade of the ALICE ITS detector, Nuclear Instru- ments and Methods in Physics Research Section A : Accelera- tors, Spectrometers, Detectors and Associated Equipment (2021). doi:10.1016/j.nima.2022.166632

  6. [8]

    H. Hillemanns, ALICE ITS3: Technology Qualification Results on Prototype Sensor Structures of Novel Bent Wafer Scale 65nm CMOS Sensors, 2023 IEEE Nuclear Science Symposium, Medi- cal Imaging Conference and International Symposium on Room- Temperature Semiconductor Detectors (NSS MIC RTSD) (2023). doi:10.1109/nssmicrtsd49126.2023.10338255

  7. [9]

    Aumann, Prospects of nuclear structure at the future GSI accelerators, Progress in Particle and Nuclear Physics 59 (1) (2007) 3–21

    T. Aumann, Prospects of nuclear structure at the future GSI accelerators, Progress in Particle and Nuclear Physics 59 (1) (2007) 3–21

  8. [10]

    Belias, FAIR status and the PANDA experiment, Journal of Instrumen- tation 15 (10) (2020) C10001

    A. Belias, FAIR status and the PANDA experiment, Journal of Instrumen- tation 15 (10) (2020) C10001

  9. [11]

    Kobayashi, N

    T. Kobayashi, N. Chiga, T. Isobe, Y . Kondo, T. Kubo, K. Kusaka, T. Mo- tobayashi, T. Nakamura, J. Ohnishi, H. Okuno, et al., SAMURAI spec- trometer for RI beam experiments, Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 317 (2013) 294–304. 9

  10. [12]

    M. Duer, T. Aumann, R. Gernh ¨auser, V . Panin, S. Paschalis, D. Rossi, N. Achouri, D. Ahn, H. Baba, C. Bertulani, et al., Observation of a corre- lated free four-neutron system, Nature 606 (7915) (2022) 678–682

  11. [13]

    Borri, P

    M. Borri, P. Booker, M. Buckland, et al., FAIR R3B-TRT: a MAPS-based Si-tracker, in: 2024 IEEE Nuclear Science Sympo- sium (NSS), Medical Imaging Conference (MIC) and Room Tem- perature Semiconductor Detector Conference (RTSD), 2024, pp. 1–1. doi:10.1109/NSS/MIC/RTSD57108.2024.10656696

  12. [14]

    M. Mager, ALPIDE, the Monolithic Active Pixel Sensor for the ALICE ITS upgrade, Nuclear Instruments & Methods in Physics Research Sec- tion A-accelerators Spectrometers Detectors and Associated Equipment (2016). doi:10.1016/j.nima.2015.09.057

  13. [15]

    doi:https://doi.org/10.1016/j.nima.2021.166280

    ALICE ITS project, First demonstration of in-beam performance of bent Monolithic Active Pixel Sensors, Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrom- eters, Detectors and Associated Equipment 1028 (2022) 166280. doi:https://doi.org/10.1016/j.nima.2021.166280. URLhttps://www.sciencedirect.com/science/article/pii/ S01...

  14. [16]

    Rossewij, E

    M. Rossewij, E. Okkinga, H. Naqvi, et al., Electrical/piezoresistive effects in bent Alpide MAPS, Journal of Instrumentation (2024). doi:10.1088/1748-0221/19/04/c04057

  15. [17]

    Andronic, P

    A. Andronic, P. Becht, M. Blidaru, et al., Detection efficiency and spa- tial resolution of Monolithic Active Pixel Sensors bent to different radii, Nuclear Instruments and Methods in Physics Research Section A: Accel- erators, Spectrometers, Detectors and Associated Equipment 1083 (2025) 171131. doi:10.1016/j.nima.2025.171131

  16. [18]

    URLhttps://ccb.ifj.edu.pl/pl

    Cyclotron Centre Bronowice, Centrum Cyklotronowe Bronowice - IFJ PAN, accessed: 2024-11-08 (2024). URLhttps://ccb.ifj.edu.pl/pl

  17. [19]

    G. A. Rinella, The ALPIDE pixel sensor chip for the upgrade of the AL- ICE Inner Tracking System, Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment (2017). doi:10.1016/j.nima.2016.05.016

  18. [20]

    Siddhanta, D

    S. Siddhanta, D. Marras, C. Puggioni, et al., A Readout System for single ALPIDE sensors of the ALICE Inner Tracking System Upgrade, in: 2020 IEEE Nuclear Science Symposium and Medical Imaging Conference (NSS/MIC), 2020, pp. 1–3. doi:10.1109/NSS/MIC42677.2020.9508095

  19. [21]

    Jacob, T

    G. Jacob, T. A. Maris, Quasi-free scattering and nuclear structure, Re- views of Modern Physics 38 (1) (1966) 121

  20. [22]

    E. J. Moniz, I. Sick, R. R. Whitney, et al., Nuclear Fermi Momenta from Quasielastic Electron Scattering, Phys. Rev. Lett. 26 (1971) 445–448. doi:10.1103/PhysRevLett.26.445. URLhttps://link.aps.org/doi/10.1103/PhysRevLett.26. 445

  21. [23]

    Cortina-Gil, H

    D. Cortina-Gil, H. Alvarez-Pol, T. Aumann, M. B ¨ohmer, et al., CAL- IFA, a Dedicated Calorimeter for the R3B/FAIR, Nuclear Data Sheets 120 (2014) 99–101

  22. [24]

    Y . Liu, M. Amjad, P. Baesso, D. Cussans, J. Dreyling-Eschweiler, R. Ete, I. Gregor, L. Huth, A. Irles, H. Jansen, et al., EUDAQ2—A flexible data acquisition software framework for common test beams, Journal of In- strumentation 14 (10) (2019) P10033

  23. [25]

    Dannheim, K

    D. Dannheim, K. Dort, L. Huth, J. Kr ¨oger, M. Munker, F. Pitters, P. Sch¨utze, S. Spannagel, et al., Corryvreckan: a modular 4D track re- construction and analysis software for test beam data, Journal of Instru- mentation 16 (03) (2021) P03008

  24. [26]

    Ulukutlu, uITS3 Krakow Software Repository,https://github

    B. Ulukutlu, uITS3 Krakow Software Repository,https://github. com/bulukutlu/uits3_krakow22, gitHub repository, accessed: 2026- 06-22 (2022)

  25. [27]

    R. Brun, F. Rademakers, ROOT: An object oriented data analysis frame- work, Nucl. Instrum. Meth. A 389 (1997) 81–86. doi:10.1016/S0168- 9002(97)00048-X

  26. [28]

    Isakov, ALICE ITS2: overview and performance, Journal of Instrumentation 20 (07) (2025) C07026

    A. Isakov, ALICE ITS2: overview and performance, Journal of Instrumentation 20 (07) (2025) C07026. doi:10.1088/1748- 0221/20/07/C07026

  27. [29]

    ALICE Collaboration, Sensor operating point calibration and monitor- ing of the ALICE Inner Tracking System during LHC Run 3, Nu- clear Instruments and Methods in Physics Research Section A: Ac- celerators, Spectrometers, Detectors and Associated Equipment (2026) 171354doi:10.1016/j.nima.2026.171354

  28. [30]

    Akiba, S

    T. Akiba, S. Sano, T. Yanase, et al., Optuna: A Next-generation Hyper- parameter Optimization Framework, in: Proceedings of the 25th ACM SIGKDD International Conference on Knowledge Discovery and Data Mining, 2019, pp. 2623–2631. 10