Temperature Dependence of Gain and Time Resolution in LGAD Detectors
Pith reviewed 2026-05-18 18:08 UTC · model grok-4.3
The pith
LGAD gain-voltage curves at multiple temperatures can be reconstructed from one reference curve via a bias-compensation relation derived from an equivalent rectangular gain layer.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The non-uniform multiplication region in an LGAD is replaced by an equivalent rectangular gain layer. A first-order bias-compensation relation for constant gain is derived from this representation and shown to be temperature-independent. The entire gain-voltage curve family at different temperatures is thereby reconstructed from a main curve measured at a reference temperature. The same equivalent-layer approach is applied to timing by separating total time resolution into jitter and intrinsic parts and assigning each part its own temperature-dependent bias offset, producing a function-level description of multi-temperature LGAD timing curves.
What carries the argument
equivalent rectangular gain layer representation of the multiplication region, supplying a first-order bias-compensation relation for constant gain
If this is right
- Gain at any temperature is obtained by shifting the reference gain curve by the computed bias offset.
- Time-resolution curves at multiple temperatures follow from separate bias offsets applied to the jitter and intrinsic components.
- Characterization effort is reduced because exhaustive multi-temperature sweeps are no longer required.
- The analytical model supplies a practical tool for predicting operating points and performing calibration in temperature-varying environments.
Where Pith is reading between the lines
- Large detector arrays could adopt reduced-density temperature testing protocols based on the compensation relation.
- Real-time temperature correction routines in readout electronics could incorporate the derived bias offsets directly.
- The rectangular-layer approximation could be compared with device simulations to establish its range of validity.
- Extension of the same compensation method to irradiated LGADs would test whether the framework remains predictive after radiation damage.
Load-bearing premise
Replacing the actual non-uniform multiplication region with an equivalent rectangular gain layer still yields a temperature-independent bias-compensation relation accurate enough for the tested devices and the independent dataset.
What would settle it
A direct measurement at a second temperature in which the gain after applying the predicted bias compensation deviates substantially from the value on the reference curve.
read the original abstract
Low-Gain Avalanche Diodes (LGADs) provide moderate internal gain and time resolutions of a few tens of picoseconds, making them a key technology for ultrafast timing in high-energy physics and beyond. However, both their gain and timing characteristics vary strongly with reverse-bias voltage and temperature. This work establishes a compact analytical framework that describes multi-temperature LGAD gain and timing behavior through an equivalent representation of the gain layer. The non-uniform multiplication region is replaced by an equivalent rectangular gain layer, from which a first-order bias-compensation relation for constant gain is derived and validated. Using multi-temperature measurements of LGADs designed by IHEP and fabricated by IME, together with an independent HPK dataset, we show that the gain-voltage curve family can be reconstructed from a reference-temperature main curve, substantially reducing characterization effort. The same idea is then extended to timing by decomposing the total time resolution into jitter and intrinsic components and representing their temperature dependences as component-wise equivalent bias offsets. The resulting framework provides a function-level description of multi-temperature LGAD time-resolution curves and offers a practical tool for calibration, operation, and reduced-density characterization of LGAD-based ultrafast timing systems.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper claims that modeling the LGAD multiplication region as an equivalent rectangular gain layer yields a first-order bias-compensation relation that permits reconstruction of the full family of gain-voltage curves at multiple temperatures from a single reference-temperature curve. The same decomposition into equivalent bias offsets is applied to time resolution after separating jitter and intrinsic contributions. The framework is derived analytically and validated on multi-temperature data from IHEP/IME devices together with an independent HPK dataset.
Significance. If the central approximation holds with the reported accuracy, the work supplies a compact, function-level description that can materially reduce the experimental effort required for temperature-dependent characterization of LGAD timing detectors. The inclusion of an external HPK dataset provides a useful check against device-specific fitting.
major comments (1)
- The derivation of the first-order bias-compensation relation rests on replacing the actual peaked field profile with a uniform rectangular slab (see the section introducing the equivalent rectangular gain layer). Because the ionization coefficient is exponentially sensitive to the local field, any temperature-induced shift in the shape or position of the real peak may introduce higher-order corrections not captured by a fixed rectangular equivalent. The manuscript demonstrates overall agreement with measured curves but does not quantify the residual temperature-dependent error that would remain if the true non-uniform profile were restored; a dedicated residual analysis or comparison against TCAD field profiles across the measured temperature range would directly test whether the first-order relation remains sufficiently accurate at the edges of the operating window.
minor comments (2)
- In the figures that overlay reconstructed and measured gain curves, add a residual panel or tabulated RMS deviation per temperature to make the reconstruction fidelity quantitative rather than visual.
- Clarify in the text whether the equivalent-layer width and height are held strictly fixed across all temperatures or allowed a weak temperature dependence; the current wording leaves this ambiguous.
Simulated Author's Rebuttal
We thank the referee for the careful review and constructive comment on the equivalent rectangular gain layer approximation. We address the point below and outline the planned revision.
read point-by-point responses
-
Referee: The derivation of the first-order bias-compensation relation rests on replacing the actual peaked field profile with a uniform rectangular slab (see the section introducing the equivalent rectangular gain layer). Because the ionization coefficient is exponentially sensitive to the local field, any temperature-induced shift in the shape or position of the real peak may introduce higher-order corrections not captured by a fixed rectangular equivalent. The manuscript demonstrates overall agreement with measured curves but does not quantify the residual temperature-dependent error that would remain if the true non-uniform profile were restored; a dedicated residual analysis or comparison against TCAD field profiles across the measured temperature range would directly test whether the first-order relation remains sufficiently accurate at the edges of the operating window.
Authors: We agree that the exponential sensitivity of the ionization coefficient implies that any temperature-driven change in the actual field peak could produce higher-order corrections beyond the fixed rectangular equivalent. The model is presented as a first-order approximation whose validity is tested by its ability to reconstruct the full family of measured gain curves from a single reference-temperature curve, with comparable performance on both the IHEP/IME and independent HPK datasets. To directly address the request for quantification of residuals, the revised manuscript will include a new subsection that extracts and plots the relative residuals between measured and reconstructed gains as a function of temperature, with particular attention to the high- and low-gain edges of the operating window. This data-driven residual analysis will provide a practical bound on any unaccounted temperature dependence. A device-specific TCAD reconstruction of the evolving field profile lies outside the scope of the present experimental study; we will instead note this limitation and cite existing literature on LGAD field profiles to contextualize the expected size of higher-order effects. revision: partial
Circularity Check
No significant circularity; derivation grounded by independent dataset
full rationale
The paper replaces the non-uniform gain layer with an equivalent rectangular representation, derives a first-order bias-compensation relation from that model, and validates reconstruction of the full gain-voltage family on both its own IHEP/IME multi-temperature data and a separate HPK dataset. Because the central relation is obtained from the rectangular ansatz rather than by fitting the target multi-temperature curves directly, and because external data provide an independent check, the derivation chain does not reduce to its inputs by construction. No load-bearing self-citation or fitted-input-renamed-as-prediction step is present in the supplied text.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption The non-uniform multiplication region can be replaced by an equivalent rectangular gain layer without loss of predictive power for temperature dependence.
invented entities (1)
-
equivalent rectangular gain layer
no independent evidence
Lean theorems connected to this paper
-
IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
The non-uniform multiplication region is replaced by an equivalent rectangular gain layer, from which a first-order bias-compensation relation for constant gain is derived
-
IndisputableMonolith/Foundation/AlphaCoordinateFixation.leancostAlphaLog_high_calibrated_iff unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
M = M0 exp(∫ A √E α(T,E) dE) with Massey α(T,E) = p1 exp(−(p2 + p3 T)/E)
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
Works this paper leans on
-
[1]
Understanding and simu- lating SiPMs,
F. Acerbi and S. Gundacker, “Understanding and simu- lating SiPMs,” vol. 926, pp. 16–35. [Online]. Available: https://linkinghub.elsevier.com/retrieve/pii/S0168900218317704
-
[2]
SPAD Figures of Merit for Photon-Counting, Photon-Timing, and Imaging Applications: A Review,
D. Bronzi, F. Villa, S. Tisa, and etal, “SPAD Figures of Merit for Photon-Counting, Photon-Timing, and Imaging Applications: A Review,” vol. 16, no. 1, pp. 3–12. [Online]. Available: http://ieeexplore.ieee.org/document/7283534/
-
[3]
R. Heller, J. Ellin, M. Backfish, and etal, “Demonstration of LGADs and Cherenkov Gamma Detectors for Prompt Gamma Timing Proton Therapy Range Verification,” vol. 9, no. 4, pp. 508–514. [Online]. Available: https://ieeexplore.ieee.org/document/10748344/
-
[4]
Characterization of thin LGAD sensors designed for beam monitoring in proton therapy,
O. Marti Villarreal, A. Vignati, S. Giordanengo, and etal, “Characterization of thin LGAD sensors designed for beam monitoring in proton therapy,” vol. 1046, p. 167622. [Online]. Available: https://linkinghub.elsevier.com/retrieve/pii/S0168900222009147
-
[5]
Beam test results of 25 and 35 $$\mu$$m thick FBK ultra-fast silicon detectors,
F. Carnesecchi, S. Strazzi, A. Alici, and etal, “Beam test results of 25 and 35 $$\mu$$m thick FBK ultra-fast silicon detectors,” vol. 138, no. 1, p. 99. [Online]. Available: https://link.springer.com/10.1140/epjp/s13360-022-03619-1
-
[6]
The Development of SiPM-Based Fast Time-of-Flight Detector for the AMS-100 Experiment in Space,
C. Chung, T. Backes, C. Dittmar, and etal, “The Development of SiPM-Based Fast Time-of-Flight Detector for the AMS-100 Experiment in Space,” vol. 6, no. 1, p. 14. [Online]. Available: https://www.mdpi.com/2410-390X/6/1/14
-
[7]
S. Schael, A. Atanasyan, J. Berdugo, and etal, “AMS-100: The next generation magnetic spectrometer in space – An international science platform for physics and astrophysics at Lagrange point 2,” vol. 944, p. 162561. [Online]. Available: https://linkinghub.elsevier.com/retrieve/pii/S0168900219310848
-
[8]
Time-resolved synchrotron light source X-ray detection with Low-Gain Avalanche Diodes,
G. Saito, M. Leite, S. Mazza, and etal, “Time-resolved synchrotron light source X-ray detection with Low-Gain Avalanche Diodes,” vol. 1064, p. 169454. [Online]. Available: https://linkinghub.elsevier.com/retrieve/pii/S0168900224003802
-
[9]
A High-Granularity Timing Detector for the ATLAS Phase-II upgrade,
M. Casado, “A High-Granularity Timing Detector for the ATLAS Phase-II upgrade,” vol. 1032, p. 166628. [Online]. Available: https://linkinghub.elsevier.com/retrieve/pii/S0168900222002005
-
[10]
The CMS MTD Endcap Timing Layer: Precision timing with Low Gain Avalanche Diodes,
M. Ferrero, “The CMS MTD Endcap Timing Layer: Precision timing with Low Gain Avalanche Diodes,” vol. 1032, p. 166627. [Online]. Available: https://linkinghub.elsevier.com/retrieve/pii/S0168900222001991
-
[11]
Science Requirements and Detector Concepts for the Electron- Ion Collider,
R. Abdul Khalek, A. Accardi, J. Adam, and etal, “Science Requirements and Detector Concepts for the Electron- Ion Collider,” vol. 1026, p. 122447. [Online]. Available: https://linkinghub.elsevier.com/retrieve/pii/S0375947422000677 AUTHORet al.: PREPARATION OF PAPERS FOR IEEE TRANSACTIONS AND JOURNALS (FEBRUARY 2017) 7
work page 2017
-
[12]
Temperature characteristics of silicon avalanche photodiodes,
I. Wegrzecka, M. Grynglas, M. Wegrzecki, and etal, “Temperature characteristics of silicon avalanche photodiodes,” J. Fraczek, Ed., pp. 194–201. [Online]. Available: http://proceedings.spiedigitallibrary.org/proceeding.aspx?articleid=895659
-
[13]
K. Ogasawara, S. Livi, and D. McComas, “Temperature dependence of the thin dead layer avalanche photodiode for low energy electron measurements,” vol. 611, no. 1, pp. 93–98. [Online]. Available: https://linkinghub.elsevier.com/retrieve/pii/S016890020901794X
-
[14]
Characterization of Ultra-Fast Silicon Detectors (UFSD) for high energy physics applications,
F. Zareef, A. Oblakowska-Mucha, T. Szumlak, and etal, “Characterization of Ultra-Fast Silicon Detectors (UFSD) for high energy physics applications,” vol. 1061, p. 169085. [Online]. Available: https://linkinghub.elsevier.com/retrieve/pii/S0168900224000111
-
[15]
M. Zhao, X. Jia, K. Wu, and etal, “Low Gain Avalanche Detectors with good time resolution developed by IHEP and IME for ATLAS HGTD project,” vol. 1033, p. 166604. [Online]. Available: https://linkinghub.elsevier.com/retrieve/pii/S0168900222001875
-
[16]
Effects of Shallow Carbon and Deep N++ Layer on the Radiation Hardness of IHEP-IME LGAD Sensors,
M. Li, Y . Fan, X. Jia, and etal, “Effects of Shallow Carbon and Deep N++ Layer on the Radiation Hardness of IHEP-IME LGAD Sensors,” vol. 69, no. 5, pp. 1098–1103. [Online]. Available: https://ieeexplore.ieee.org/document/9739028/
-
[17]
Design and testing of LGAD sensor with shallow carbon implantation,
K. Wu, X. Jia, T. Yang, and etal, “Design and testing of LGAD sensor with shallow carbon implantation,” vol. 1046, p. 167697. [Online]. Avail- able: https://linkinghub.elsevier.com/retrieve/pii/S0168900222009895
-
[18]
Statistics of the Recombinations of Holes and Electrons
W. Shockley and J. W. T. Read, “Statistics of the Recombinations of Holes and Electrons,” vol. 87, no. 5, p. 835. [Online]. Available: https://journals.aps.org/pr/abstract/10.1103/PhysRev.87.835
-
[19]
S. M. Sze, K. K. Ng, and Y . Li,Physics of Semiconductor Devices, fourth edition ed. Wiley
-
[20]
Analysis of the performance of low gain avalanche diodes for future particle detectors,
A. Vakili, L. Pancheri, M. Farasat, and etal, “Analysis of the performance of low gain avalanche diodes for future particle detectors,” vol. 18, no. 07, p. P07052. [Online]. Available: https://iopscience.iop.org/article/10.1088/1748-0221/18/07/P07052/meta
-
[21]
M. Ferrero, R. Arcidiacono, M. Mandurrino, and etal,An Introduction to Ultra-Fast Silicon Detectors. Taylor & Francis. [Online]. Available: https://library.oapen.org/handle/20.500.12657/49731
-
[22]
E. M. Conwell,High Field Transport in Semiconductors, 3rd ed., ser. Solid State Physics Supplement. Acad. Pr, no. 9
-
[23]
Temperature Dependence of Impact Ionization in Submicrometer Silicon Devices,
D. Massey, J. David, and G. Rees, “Temperature Dependence of Impact Ionization in Submicrometer Silicon Devices,” vol. 53, no. 9, pp. 2328–2334. [Online]. Available: https://ieeexplore.ieee.org/document/1677871/
-
[25]
Ionization coefficients in semiconductors: A nonlocalized property,
Y . Okuto and C. R. Crowell, “Ionization coefficients in semiconductors: A nonlocalized property,” vol. 10, no. 10, p. 4284. [Online]. Available: https://journals.aps.org/prb/abstract/10.1103/PhysRevB.10.4284
-
[26]
Study of Impact Ionization Coefficients in Silicon With Low Gain Avalanche Diodes,
E. Curr ´as Rivera and M. Moll, “Study of Impact Ionization Coefficients in Silicon With Low Gain Avalanche Diodes,” vol. 70, no. 6, pp. 2919–2926. [Online]. Available: https://ieeexplore.ieee.org/document/10114953/
-
[27]
Design optimization of ultra-fast silicon detectors,
N. Cartiglia, R. Arcidiacono, M. Baselga, and etal, “Design optimization of ultra-fast silicon detectors,” vol. 796, pp. 141–148. [Online]. Avail- able: https://linkinghub.elsevier.com/retrieve/pii/S0168900215004982
-
[28]
M., Bintanja, R., Blackport, R
M. Li, Y . Fan, B. Liu, and etal, “The performance of IHEP-NDL LGAD sensors after neutron irradiation,” vol. 16, no. 08, p. P08053. [Online]. Available: https://iopscience.iop.org/article/10.1088/1748- 0221/16/08/P08053/meta
-
[29]
Carrier mobilities in silicon empirically related to doping and field,
D. Caughey and R. Thomas, “Carrier mobilities in silicon empirically related to doping and field,” vol. 55, no. 12, pp. 2192–2193. [Online]. Available: http://ieeexplore.ieee.org/document/1448053/
-
[30]
A review of some charge transport properties of silicon,
C. Jacoboni, C. Canali, G. Ottaviani, and etal, “A review of some charge transport properties of silicon,” vol. 20, no. 2, pp. 77–89. [Online]. Avail- able: https://linkinghub.elsevier.com/retrieve/pii/0038110177900545
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.