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arxiv: 1907.02966 · v1 · pith:JBAS34CHnew · submitted 2019-07-05 · ⚛️ physics.ins-det

Prototype of a front-end readout ASIC designed for the Water Cherenkov Detector Array in LHAASO

Pith reviewed 2026-05-25 02:13 UTC · model grok-4.3

classification ⚛️ physics.ins-det
keywords ASICfront-end readoutcharge-to-time conversionWater Cherenkov DetectorLHAASOtime resolutionphotomultiplier tubedynamic range
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The pith

Prototype ASIC for LHAASO water Cherenkov array reaches time resolution better than 0.5 ns over 1 to 4000 photoelectrons.

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

The paper describes the design and initial bench testing of a front-end readout ASIC for photomultiplier tube signals in the Water Cherenkov Detector Array of LHAASO. Signals span a wide dynamic range from single photoelectrons to 4000, and the design uses charge-to-time conversion to encode both charge and timing information into pulse widths that can be digitized together with external TDCs. This approach simplifies the overall readout chain. Bench tests on the 0.35 micrometer CMOS prototype show time resolution better than 0.5 ns across the full range and charge resolution better than 15 percent at the single-photoelectron level, exceeding the stated requirements for the observatory.

Core claim

The prototype ASIC integrates time discrimination and charge-to-time conversion so that both time and charge are digitized simultaneously; bench tests confirm time resolution better than 0.5 ns from 1 to 4000 photoelectrons (0.75 to 3000 pC) and charge resolution better than 1 percent for large amplitudes and better than 15 percent at one photoelectron, with a 0.188 pC threshold.

What carries the argument

Charge-to-time conversion circuit that maps input charge to output pulse width for simultaneous digitization of time and charge information.

If this is right

  • The ASIC meets or exceeds the dynamic-range, timing, and charge-precision needs of the LHAASO water Cherenkov detectors.
  • Charge and time information are captured in a single pulse-width measurement, removing the need for separate analog charge and timing paths.
  • The 0.35 micrometer CMOS implementation is compatible with existing Time-to-Digital Converters for full digitization.
  • Performance holds across the full 1 to 4000 photoelectron range required for air-shower detection.

Where Pith is reading between the lines

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

  • The charge-to-time method could reduce power and complexity in other large-area detector arrays that need wide dynamic range.
  • Further integration of the TDC on the same die might lower overall system latency and jitter.
  • Calibration procedures developed for this ASIC could transfer to similar readout chips in future neutrino or cosmic-ray experiments.

Load-bearing premise

Bench-test conditions with controlled charge injection accurately represent the noise, rate, and signal shape expected from real photomultiplier tubes operating inside the Water Cherenkov Detector Array.

What would settle it

Measure time and charge resolution when the ASIC is driven by actual photomultiplier tube pulses from the Water Cherenkov Detector Array under normal operating rates and backgrounds; deviation beyond the reported resolutions would falsify the performance claim.

Figures

Figures reproduced from arXiv: 1907.02966 by Jiajun Qin, Jianfeng Liu, Lei Zhao, Li Yu, Qi An, Shubin Liu, Weihao Wu, Yu Liang.

Figure 9
Figure 9. Figure 9: figure 9. By adjusting the sizes of the MOSFETs, a delay less than 1 ns is achieved with a step [PITH_FULL_IMAGE:figures/full_fig_p007_9.png] view at source ↗
read the original abstract

The Large High Altitude Air Shower Observatory is in the R&D phase, in which the Water Cherenkov Detector Array is an important part. The signals of Photo-Multiplier Tubes would vary from single photo electron to 4000 photo electrons, and both high precision charge and time measurement is required. To simplify the signal processing chain, the charge-to-time conversion method is employed. A prototype of the front-end readout ASIC is designed and fabricated in Chartered 0.35 {\mu}m CMOS technology, which integrates time disctrimination and converts the input charge information to pulse widths. With Time-to-Digital Converters, both time and charge can be digitized at the same time. We have conducted initial tests on this chip, and the results indicate that a time resolution better than 0.5 ns is achieved over the full dynamic range (1~ 4000 photo electrons, corresponding to 0.75 ~ 3000 pC with the threshold of 0.188 pC); the charge resolution is better than 1% with large input amplitudes (500 ~ 4000 photo electrons), and remains better than 15% with a 1 photo electron input amplitude, which is beyond the application requirement.

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

2 major / 1 minor

Summary. The manuscript presents the design of a prototype front-end readout ASIC fabricated in Chartered 0.35 μm CMOS technology for the Water Cherenkov Detector Array (WCDA) in LHAASO. The ASIC employs charge-to-time conversion to measure PMT signals spanning 1 to 4000 photoelectrons (0.75 to 3000 pC), enabling simultaneous time and charge digitization when paired with TDCs. Initial bench tests with controlled charge injection are reported to achieve time resolution better than 0.5 ns across the full dynamic range and charge resolution better than 1% for 500–4000 PE inputs, remaining better than 15% at 1 PE, exceeding the stated application requirements.

Significance. If the reported resolutions hold under actual WCDA operating conditions, the work provides a practical ASIC solution that simplifies the readout chain for a large-scale water Cherenkov array by integrating time discrimination and charge-to-time conversion in a single chip.

major comments (2)
  1. [Abstract and test-results section] Abstract and test-results section: the headline performance claims (time resolution <0.5 ns; charge resolution <1% at high amplitudes and <15% at 1 PE) are presented without error bars, number of trials, statistical analysis, or raw data, preventing independent assessment of the reliability of the central experimental results.
  2. [Bench-test description] Bench-test description: no quantitative comparison or auxiliary data are supplied to establish that the controlled charge-injection conditions reproduce the noise floor, event rates, and PMT pulse shapes expected inside the WCDA; this equivalence is load-bearing for the assertion that the measured resolutions meet application requirements in the real detector.
minor comments (1)
  1. [Abstract] Typo: 'disctrimination' should read 'discrimination'.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the thorough review and constructive feedback on our manuscript describing the prototype front-end readout ASIC. We address the major comments point by point below and will revise the manuscript to strengthen the presentation of results and test methodology.

read point-by-point responses
  1. Referee: [Abstract and test-results section] Abstract and test-results section: the headline performance claims (time resolution <0.5 ns; charge resolution <1% at high amplitudes and <15% at 1 PE) are presented without error bars, number of trials, statistical analysis, or raw data, preventing independent assessment of the reliability of the central experimental results.

    Authors: We agree that the abstract and results section would benefit from additional statistical details to allow independent assessment. The reported time and charge resolutions are based on repeated bench measurements, but the current manuscript does not include error bars, the number of trials, or explicit statistical analysis. In the revised version we will add error bars to the relevant figures, state the number of measurements performed for each data point, and include a short description of the statistical treatment used to derive the quoted resolutions. revision: yes

  2. Referee: [Bench-test description] Bench-test description: no quantitative comparison or auxiliary data are supplied to establish that the controlled charge-injection conditions reproduce the noise floor, event rates, and PMT pulse shapes expected inside the WCDA; this equivalence is load-bearing for the assertion that the measured resolutions meet application requirements in the real detector.

    Authors: The bench tests employed a standard charge-injection setup calibrated to cover the full 1–4000 PE dynamic range with pulse amplitudes and widths chosen to approximate typical PMT signals. We acknowledge that the manuscript does not supply quantitative comparisons (e.g., measured noise spectra or event-rate simulations) demonstrating exact equivalence to the WCDA environment. As this is a prototype ASIC paper, such system-level validation lies outside the present scope; we will add a dedicated paragraph in the test section explaining the design choices for the injection circuit and noting that full equivalence testing will be addressed in future integrated-detector studies. revision: partial

Circularity Check

0 steps flagged

No circularity; experimental results reported directly from bench tests

full rationale

The manuscript describes ASIC design and reports measured time/charge resolutions from controlled charge-injection bench tests. No equations, derivations, fitted parameters, or predictions are present. Claims rest on direct experimental data rather than any self-referential chain, self-citation load-bearing step, or ansatz. This is the normal non-circular outcome for a pure instrumentation paper.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

This is an experimental hardware design paper; it contains no mathematical derivations, free parameters fitted to data, background axioms, or postulated physical entities.

pith-pipeline@v0.9.0 · 5772 in / 1116 out tokens · 24496 ms · 2026-05-25T02:13:28.343670+00:00 · methodology

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Reference graph

Works this paper leans on

31 extracted references · 31 canonical work pages

  1. [1]

    He, LHAASO Project: detector design and prototype , presented at the 31th Int

    H. He, LHAASO Project: detector design and prototype , presented at the 31th Int. Cosmic Ray Conf., Jul. 2009, Beijing, China

  2. [2]

    M. Chen, Z. Yao, and B. Cao et. al., R&D of LHAASO-WCDA , presented at the 32nd Int. Cosmic Ray Conf., Aug. 2011, Beijing, China. – 12 –

  3. [3]

    L. Zhao, S. Liu, and Q. An, Proposal of the readout electronics for the WCDA in the LHAASO experiment, Chin. Phys. C 38 (2014)016101-1

  4. [4]

    Manfredi, A

    P. Manfredi, A. Leona, and E. Mandelli et al., Noise limits in a front-e nd system based on time- over-threshold signal processing, Nucl. Instrum. Meth. A 439 (2000) 361

  5. [5]

    Delagnes, P

    E. Delagnes, P. Abbon, and Y. Bedfer et. al., SFEl6, a Low Noise Front-End Integrated Circuit Dedicated to the Read-out of Large Micromegas Detectors, IEEE Trans. Nucl. Sci. 47 (2000) 1447

  6. [6]

    Schambach, L

    J. Schambach, L. Bridges, and G. Eppley et al., STAR time of flight readout electronics, DAQ, and cosmic ray test stand, in 2006 IEEE Nucl. Sci. Symp. Conf. Rec. (2006) 485

  7. [7]

    X. Liu, S. Liu, and Q. An, A time-over-threshold technique for PMT signals processing , Nucl. Sci. Tech. 18 (2007)164

  8. [8]

    B. Shi, K. Shimazoe, and T. Fujiwara et al., Application of time-over-threshold readout method to micro strip gas chamber, in Proc. IEEE Nucl. Sci. Symp. Conf. Rec. (2009)419

  9. [9]

    Nishino, K.Awai, and Y.Hayato et

    H. Nishino, K.Awai, and Y.Hayato et. al., High-speed charge-to-time converter ASIC for the Super- Kamiokande detector, Nucl. Instrum. Meth. A 610 (2009)710

  10. [10]

    S. Liu, C. Feng, and Q. An et. al., BES III Time-of-Flight Readout System , IEEE Trans. Nucl. Sci. 57 (2010)419

  11. [11]

    Shi, The 10-ps wave union TDC: Improving FPGA TDC resolution beyond its cell delay, in Proc

    J.Wu and Z. Shi, The 10-ps wave union TDC: Improving FPGA TDC resolution beyond its cell delay, in Proc. IEEE Nucl. Sci. Symp. Conf. (2008)3440

  12. [12]

    J. Wang, S. Liu, Q. Shen, H. Li, and Q. An, A fully fledged TDC implemented in field- programmable gate arrays, IEEE Trans. Nucl. Sci. 57 (2010)446

  13. [13]

    L. Zhao, X. Hu, and S. Liu et. al., The Design of a 16-Channel 15 ps TDC Implemented in a 65 nm FPGA, IEEE Trans. Nucl. Sci. 60 (2013)3532

  14. [14]

    C. Ye, L. Zhao, Z. Zhou, S. Liu, and Q. An, A field-programmable-gate-array based time digitizer for the time-of-flight mass spectrometry, Rev. Sci. Instrum. 85 (2014)045115-1

  15. [15]

    Z. Deng, A. K. Lan, and X. Sun et. al., Development of an Eight-Ch annel Time-Based Readout ASIC for PET Applications, IEEE Trans. Nucl. Sci. 58 (2011)3212

  16. [16]

    X. Zhu, Z. Deng, and K. A. Lan et. al., TIMPIC-II: the Second Versi on Time-Based-Readout ASIC for SSPM Based PET Applications, in Proc. IEEE Nucl. Sci. Symp. Conf. Rec. (2012)1474

  17. [17]

    Behzad Razavi, Design of Analog CMOS Integrated Circuits, McGraw-Hill Co., 2001

  18. [18]

    Anghinolfi, P

    F. Anghinolfi, P. Jarron, and F. Krummenacher et. al., NINO: An Ultrafast Low-Power Front-End Amplifier Discriminator for the Time-of-F light Detector in the ALICE Experiment , IEEE Trans. Nucl. Sci. 51 (2004)1974

  19. [19]

    Harris, CMOS VLSI Design: A Circuits and Systems Perspective, 4th ed

    David M. Harris, CMOS VLSI Design: A Circuits and Systems Perspective, 4th ed. , Addison- Wesley Publishing Co., Neil H.E. Weste, 2010

  20. [20]

    , Springer Science+Business Media, 2007

    Fei Yuan, CMOS Current-Mode Circuits for Data Communications, 1st ed. , Springer Science+Business Media, 2007

  21. [21]

    Fotouhi, All-MOS Voltage-to-Current Converter, IEEE J

    B. Fotouhi, All-MOS Voltage-to-Current Converter, IEEE J. Solid-St. Circ. 36 (2001)147. – 13 –

  22. [22]

    Shukla, J

    R. Shukla, J. Ramírez-Angulo, and A. Lopez-Martin et al., A Low Voltage Rail to Rail V-I Conversion Scheme for Applications in Current Mode A/D Converters , in Proc. Int. Symp. Circuits Syst., 1 (2004) I-916

  23. [23]

    Azcona, B

    C. Azcona, B. Calvo, and S. Celma et al., Low-Voltage Low-Power CMOS Rail-to-Rail V-I Converters, in Proc. ECCTD Conf. (2011)182

  24. [24]

    D. A. Freitas and K. W. Current, CMOS current comparator circuit, Electron. Lett. 19 (1983)695

  25. [25]

    Rodríguez-Vázquez, R

    A. Rodríguez-Vázquez, R. Domínguez-Castro, and F. Medeiro et. al., High Resolution CMOS Current Comparators: Design and Applications to Current-Mode Function Generation , Analog Integr. Circuits Signal Process. 7 (1995)149

  26. [26]

    Ravezzi, D

    L. Ravezzi, D. Stoppa, and G.-F. Dalla Betta, Simple high-speed CMOS current comparator , Electron. Lett. 33 (1997)1829

  27. [27]

    Tang and K.-P

    X. Tang and K.-P. Pun, High-performance CMOS current comparator , Electron. Lett. 45 (2009) 1007

  28. [28]

    Traff, Novel approach to high speed CMOS current comparators, Electron

    H. Traff, Novel approach to high speed CMOS current comparators, Electron. Lett. 28 (1992)310

  29. [29]

    An Overview of LVDS Technology , Texas Instruments, Inc., 1998, http://http://www.ti.com/lit/an/snla165/snla165.pdf

  30. [30]

    2008, http://www.hamamatsu.com/resources/pdf/etd/LARGE_AREA_PMT_TPMH1286E05.pdf

    Large Photocathode Area Photomultiplier Tubes , Hamamatsu Inc., Jan. 2008, http://www.hamamatsu.com/resources/pdf/etd/LARGE_AREA_PMT_TPMH1286E05.pdf

  31. [31]

    Christiansen, High performance time to digital converter , CERN/EP-MIC, Mar

    J. Christiansen, High performance time to digital converter , CERN/EP-MIC, Mar. 2004, http://tdc.web.cern.ch/tdc/hptdc/docs/hptdc_manual_ver2.2.pdf