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REVIEW 2 major objections 7 minor 23 references

Pre-study of a Li2MoO4 based bolometer for 100Mo neutrinoless double beta decay experiment in China

T0 review · 2 major / 7 minor · reviewed 2026-08-16 · deepseek-v4-flash

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Pith's one-line read A (2 cm)^3 Li2MoO4 bolometer operated at 28 mK with heat-only readout achieves 24.6 keV resolution at 511 keV, establishing a working prototype for a 100Mo neutrinoless double beta decay experiment in China.

desk verdict Solid pre-study of a Chinese LMO bolometer: credible first demonstration and useful low-temperature data, with an unquantified heat-capacity intercept and an acknowledged 10 K-to-mK scintillation extrapolation as the soft spots to fix. read the letter →

arxiv 2505.01961 v1 pith:6WEDXUNU submitted 2025-05-04 physics.ins-det nucl-ex

Deyong Duan , Mingxuan Xue , Kangkang Zhao , Taiyuan Liu , Haiping Peng , Jiaxuan Cao , Long Ma , Liang Chen
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Hui Yuan Qing Lin Zizong Xua Xiaolian Wang
This is my paper · ORCID
classification physics.ins-detnucl-ex
keywords neutrinolessdoublebetadecaylithiummolybdate(Li2MoO4)cryogenicphononscintillatingbolometerscintillationlightyieldemissionspectrumlow-temperatureheatcapacityNTD-Gereadout100Mo
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The pith

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

The reading

This pre-study seeks to establish that lithium molybdate (Li2MoO4, LMO) bolometers can be fabricated and operated in China as detectors for the neutrinoless double $\beta$ decay of 100Mo. The authors characterise LMO crystals from room temperature down to 10 K, finding the emission spectrum peaks near 510 nm and the light yield rises steeply as temperature drops, and they measure the heat capacity down to 200 mK, obtaining a characteristic temperature $\Theta_D = (330 \pm 3)$ K. They then assemble a (2 cm)^3 LMO bolometer read out by a neutron-transmutation-doped germanium thermometer and operate it at 28 mK, reaching an energy resolution of 24.6 keV at 511 keV and 32.2 keV at 1274 keV. These numbers demonstrate working detector operation, and the material data are meant to support a future light-heat dual-readout detector for a deep-underground 100Mo experiment in China.

What carries the argument

The load-bearing object is the cryogenic phonon scintillating bolometer in its heat-only incarnation: a polished LMO absorber linked to a copper frame through PTFE pieces, with an NTD-Ge resistance thermometer coupled to the crystal and thin gold wire bonds carrying the signal. An energy deposit heats the crystal; the weak thermal link lets it cool back with a decay time of about 30 ms, and a matched optimal filter extracts pulse amplitudes from a triggerless 10 kHz stream. The second mechanism is the $T^{3}$ heat-capacity law with characteristic temperature $\Theta_D = (330 \pm 3)$ K, which turns the measured temperature rise into an energy scale and predicts the sensitivity of larger absorbers. The scintillation data are the third piece: the 510 nm emission peak and the low-temperature light-yield growth are the quantitative inputs for designing the future light detector and for enabling $\alpha$/$\beta$ discrimination.

What would settle it

A direct mK-temperature scintillation measurement would settle it: cool an LMO crystal from the same growth line below 50 mK in a dilution refrigerator and record its emission spectrum and light yield with a photodetector covering 350 to 850 nm. If the emission peak departs from 510 nm or the light yield stops increasing below 10 K, the extrapolated design basis for the light-heat dual-readout upgrade fails.

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Extended reading notes

Core claim

The discovery claimed is that a heat-only LMO bolometer with a cubic (2 cm)^3 absorber can be built and operated at 28 mK on a ground-level cryostat to give clean gamma spectra: the 22Na lines at 511 and 1274 keV are resolved with FWHM 24.6 keV and 32.2 keV, and the Compton edge at 1061 keV plus a 1460 keV 40K line are visible in ten hours of data. On the material side, the paper claims that LMO emission peaks near 510 nm at low temperature and its light yield increases as the temperature falls, especially below 50 K, and that heat capacity follows the $T^{3}$ heat-capacity law with characteristic temperature $\Theta_D = (330 \pm 3)$ K down to 200 mK. The authors take the combination as a foundation for a light-heat dual-readout bolometer: the 510 nm peak sets the design target for a light detector and its anti-reflection coating, while the measured heat capacity lets future crystals be designed from the $T^{3}$ heat-capacity law.

Load-bearing premise

The load-bearing premise is that the scintillation properties measured only down to 10 K—emission peaking near 510 nm and light yield rising steeply at low temperature—remain representative down to the 28 mK bolometer operating temperature, since no direct mK scintillation measurement was made.

Editorial extensions

If this is right

  • The demonstrated 24.6 keV FWHM at 511 keV gives a working domestic LMO bolometer as a starting point for the planned 100Mo search.
  • Using the characteristic temperature $\Theta_D = (330 \pm 3)$ K, future LMO crystal sizes and operating temperatures can be chosen with a quantitative prediction of heat capacity and pulse height.
  • The 510 nm emission peak and the steep light-yield rise below 50 K indicate that a light detector sensitive near 510 nm should provide the light signal needed for alpha/beta discrimination in the dual-readout upgrade.
  • Longer data taking, better shielding, and operation at the proposed 2400 m underground site should reduce the observed environmental background lines and improve the resolution beyond the ground-level values.
  • The presence of the 1061 keV Compton edge and the 1460 keV line in ten hours of data shows the detector already has enough spectral quality for calibration and background studies.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • If the 10 K scintillation trends persist to 28 mK, the dual-readout design should add the alpha/beta discrimination that a single heat channel cannot provide, and the quoted resolutions are then a floor for the full detector.
  • The heat-capacity measurement together with the observed 29.8 ms decay time is enough to estimate the thermal conductance of the PTFE suspension; a future analysis could check whether that conductance matches the design and whether it contributes thermal noise to the resolution.
  • A decisive next step would be to move the same bolometer underground: if the background lines shrink while the gamma-peak widths stay fixed, the ground-level resolution loss is environmental, whereas unchanged widths would point to the crystal or readout chain.
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Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, and a circularity audit.

Referee Report

2 major / 7 minor

Summary. This paper reports a pre-study toward a 100Mo neutrinoless double beta decay experiment in China using Li2MoO4 (LMO) bolometers. The authors characterize the scintillation properties of a SICCAS-grown LMO sample from 300 K down to 10 K, measuring the emission spectrum (peaking at 510 nm at 10 K) and the temperature dependence of the light yield. They measure the specific heat of a 14.3 mg LMO sample over 200 mK–2 K, fit C/T = γ + βT^2, extract a Debye temperature ΘD = (330 ± 3) K, and compare it to an independent literature value. They then design, assemble, and operate a (2 cm)^3 cubic LMO bolometer with NTD-Ge heat readout at 28 mK in a ground-above dilution refrigerator, calibrate it with a 22Na source, and obtain FWHM energy resolutions of 24.6 keV at 511 keV and 32.2 keV at 1274 keV. The paper concludes that these studies lay the foundation for manufacturing bolometers in China and for future double beta decay research at the China Jinping Underground Laboratory.

Significance. If the results hold, the paper provides the first domestic demonstration of an LMO bolometer in China, showing that the full chain—crystal production, assembly, cryogenic operation, and signal processing—works with a measurable energy resolution. The scintillation and heat-capacity data for this specific SICCAS LMO crystal are also useful inputs for the community. The FWHM values are modest compared with CUPID or AMoRE, but the paper explicitly acknowledges this and identifies improvement paths. The main strengths are the reproducible detector construction, the use of a matched-filter analysis (with reference to open software), and the independent cross-check of the Debye temperature against a literature value. However, the heat-capacity analysis leaves an unresolved linear term in C/T that is load-bearing for the mK extrapolation, and the scintillation design is based on a 10 K spectrum extrapolated to mK temperatures; these points currently limit the strength of the conclusions drawn from the characterization studies.

major comments (2)
  1. [Section 3, Eq. (2)] The fit to C/T = γ + βT^2 reports no value for the intercept γ, even though the Debye temperature is derived from β alone and the intercept is rejected as a systematic uncertainty of the testing platform. A real linear term, if present, would scale as T and dominate over the T^3 Debye term at the 28 mK operating point, where the bolometer actually runs. Please report γ with its uncertainty, quantify its contribution relative to βT^2 at 28 mK and at 200 mK, and support the rejection either with a direct measurement (e.g., an addenda-only run or a platform background measurement) or by propagating the resulting systematic uncertainty into the predicted mK heat capacity. The current justification relies on a previous PbWO4 study [19] that involves a different crystal and does not, by itself, establish the platform artifact for LMO.
  2. [Section 2] The scintillation emission spectrum is measured only down to 10 K, and the manuscript explicitly states that mK-level measurements cannot be made directly. Since the light detector design—semiconductor band gap and anti-reflective coating thickness—depends on the emission wavelength at the operating temperature, the planned dual-readout bolometer is being designed on an extrapolated trend. Please either provide lower-temperature data or soften the design implications in Sections 2 and 6 to reflect this extrapolation uncertainty. This is not a fatal flaw for the heat-only demonstration reported here, but it is load-bearing for the stated next step of building a light-heat dual-readout detector.
minor comments (7)
  1. [Abstract/Keywords] The keyword line reads 'Keyworks'; it should be 'Keywords'.
  2. [Section 4 header] The heading 'LMO based bolometer desigh and assembly' contains a typo: 'desigh' should be 'design'.
  3. [Section 5, Figure 10(b)] In the figure label, 'HM=32.2WF keV' appears to be a garbled version of 'FWHM=32.2 keV'; please correct it.
  4. [Section 6] The phrase 'in the near further' near the end of the conclusion should likely read 'in the near future'.
  5. [Section 3, Eq. (1)] To allow the reader to reproduce the Debye temperature from the fitted β, please state explicitly the values of r (number of atoms per unit cell) and the unit-cell count Ncore for the 14.3 mg LMO sample used in Eq. (1).
  6. [Figure 6] The residual panel labeled Q appears to show only non-negative values; if the residuals are centered near zero, the vertical axis should extend to negative values so the reader can see the full deviation pattern.
  7. [Section 5, calibration fit] The energy calibration is based on two gamma lines only; please report the uncertainties of the fitted slope and intercept, and the reduced chi-square or equivalent goodness-of-fit statistic, so the reader can judge the calibration quality.

Circularity Check

0 steps flagged · score 2.0 of 10

No significant circularity: direct measurements and an independent Debye-temperature comparison carry the main claims; only a minor, non-load-bearing self-citation appears in the heat-capacity intercept treatment.

full rationale

The paper's central results are measured, not derived from themselves. Scintillation yields and spectra are direct spectrometer measurements from 300 K down to 10 K, and the mK-level extrapolation is explicitly presented as an assumption rather than as a derived prediction. Heat capacity is measured with a PPMS relaxation technique and fitted to C/T = gamma + beta*T^2; the Debye temperature is extracted from the fitted slope and cross-checked against the independent measurement by Musikhin et al. [20], so the fit is not circular. The bolometer energy resolution (FWHM 24.6 keV at 511 keV and 32.2 keV at 1274 keV) comes from calibrated 22Na spectra processed with a standard matched filter; the calibration lines set the energy scale, and the FWHM is a measured width, not a predicted quantity derived from fitted parameters. The only self-referential element is the rejection of the C/T intercept as a systematic platform effect based on the authors' prior PbWO4 study [19]; however, this choice is presented as a systematic rather than a physical term, does not enter the bolometer demonstration, and is not load-bearing for the paper's main conclusion. The paper also honestly notes that mK-level scintillation properties cannot yet be measured directly and uses the 10-300 K trend as an alternative approach, which is a stated limitation rather than a circular step. Overall, the derivation chain is self-contained against external data and the measured detector performance, so no significant circularity is present.

Assumptions & free parameters 3 free parameters · 4 assumptions · 0 invented entities

No new entities or forces are introduced. The work relies on standard solid-state physics (Debye model) and an extrapolation from 10 K to mK for scintillation behavior. The free parameters are physically motivated material properties or calibration constants.

free parameters (3)
  • Debye temperature Theta_D = 330 ± 3 K
    Extracted from the slope of the C/T versus T^2 fit over 200 mK to 2 K, using the Debye model in Eq. (1).
  • Intercept gamma in C/T fit = not reported
    Fitted in Eq. (2) but rejected as a systematic artifact; the effect of its removal on Theta_D is not quantified.
  • Energy calibration slope = 3.9e-3 MeV/ADC channel
    Linear calibration using the 511 keV and 1274 keV gamma lines from 22Na; used to convert ADC to energy.
assumptions (4)
  • domain assumption The Debye model C(T) = (12/5) r N_core k_B pi^4 (T/Theta_D)^3 holds for the 21.7 g LMO crystal down to 28 mK, though it is only directly measured down to 200 mK.
    The heat capacity is not measured at the bolometer operating temperature; the T^3 law is assumed to extrapolate.
  • domain assumption Scintillation properties measured down to 10 K remain representative at mK operating temperatures.
    The paper states that mK-level scintillation cannot be measured directly and uses the temperature trends as an indirect approach.
  • domain assumption The intercept gamma in the C/T fit is a systematic artifact of the testing platform, as seen in the authors' previous PbWO4 study, and can be discarded.
    The rejection is justified by prior experience rather than by the current data; the effect on the Debye temperature is not quantified.
  • domain assumption The external 22Na calibration source provides an accurate energy scale for internal energy depositions in the crystal.
    The calibration assumes no significant position dependence or non-linearity of the NTD-Ge response within 0.5 to 1.3 MeV.

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Cite this review

Pith. "Pith review of Pre-study of a Li2MoO4 based bolometer for 100Mo neutrinoless double beta decay experiment in China." pith.science (2026). https://pith.science/paper/6WEDXUNU

@misc{pith2026250501961,
  author       = {Pith},
  title        = {Pith review of: Pre-study of a Li2MoO4 based bolometer for 100Mo neutrinoless double beta decay experiment in China},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/6WEDXUNU}},
  note         = {Machine review of arXiv:2505.01961}
}
read the original abstract

The cryogenic phonon scintillating bolometer is a promising and extremely attractive option to search for the nuclide neutrinoless double beta decay. In this paper, a pre-study of bolometer based on Li2MoO4 (LMO) crystal is presented, in which the properties of the LMO crystal at the low temperature, including scintillation characteristics and specific heat, are investigated in detail. The excitation spectrum and light yield are measured from the room temperature down to 10 K, and heat capacity is measured down to temperature of O(200) mK. Furthermore, a (2 cm)3 cubic LMO based bolometer is manufactured and tested at ultra-low mK-level temperature in a ground-above cryostat platform, and a good energy resolution is achieved. The studies laid a foundation to manufacture the bolometer detector in China and conduct neutrinoless double beta decay research at the China Jinping Underground Laborator

Figures

Figures reproduced from arXiv: 2505.01961 by the authors.

Figure 1
Figure 1. Schematic diagram of the cryogenic phonon-scintillating bolometer. There are five main compo [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 2
Figure 2. LMO crystals grown by SICCAS. The slices are 10 mm [PITH_FULL_IMAGE:figures/full_fig_p003_2.png] view at source ↗
Figure 3
Figure 3. The excitation spectrum of LMO at 10 K, peaked at [PITH_FULL_IMAGE:figures/full_fig_p003_3.png] view at source ↗
Figures from the paper (7 more)
Figure 4
Figure 4. Figure 4: (a) A laser-induced emission spectrum of a LMO crystal at different temperatures, peaked at 510 [PITH_FULL_IMAGE:figures/full_fig_p004_4.png]
Figure 5
Figure 5. Figure 5: LMO crystal sample with a mass of 14.3 mg glued on the testing platform. The wires are for [PITH_FULL_IMAGE:figures/full_fig_p004_5.png]
Figure 6
Figure 6. Figure 6: The ratio C/T as a linear function of T 2 . The error bars of heat capacity are determined by PPMS model fitting software. The Q value is defined as the residuals divided by the error of data to represent the deviation between data and the fitting result. transferring …
Figure 7
Figure 7. Figure 7: (a) The (2cm)3 cubic LMO bolometer is assembled inside a thick copper frame. (b) The LMO bolometer is mounted on the spring floating plate in a cryostat at USTC. 5 Detector operation and data analysis The cryostat platform is operated stably with a temperature of 20 mK…
Figure 8
Figure 8. Figure 8: The ground-above cryostat platform used to test the LMO based bolometer located at USTC. [PITH_FULL_IMAGE:figures/full_fig_p006_8.png]
Figure 9
Figure 9. Figure 9: The LMO bolometer heat pulse in a 0.5-second time window. The typical decay time is 29.8 ms [PITH_FULL_IMAGE:figures/full_fig_p006_9.png]
Figure 10
Figure 10. Figure 10: (a) Energy calibration of the LMO based bolometer using [PITH_FULL_IMAGE:figures/full_fig_p007_10.png]

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Works this paper leans on

23 extracted references · 17 canonical work pages

  1. [20]

    The heat capacity of Li 2MoO4 in the temperature range 6–310 K,

    A. Musikhin, V. Naumov, M. Bespyatov, et al. , “The heat capacity of Li 2MoO4 in the temperature range 6–310 K,” Journal of Alloys and Compounds , vol. 639, pp. 145–148, 2015. doi: 10.1016/j. jallcom.2015.03.159

    doi:10.1016/j 2015

  2. [19]

    Study of a coherent elastic neutrino-nucleus scattering experiment at a reactor with a PbWO 4-based bolometer,

    L. Zhang, M. Xue, K. Zhao, et al., “Study of a coherent elastic neutrino-nucleus scattering experiment at a reactor with a PbWO 4-based bolometer,” Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment , vol. 1043, p. 167 469,

    work page

  3. [1]

    Neutrinoless double-beta decay: Status and prospects,

    M. J. Dolinski, A. W. P. Poon, and W. Rodejohann, “Neutrinoless double-beta decay: Status and prospects,” Annual Review of Nuclear and Particle Science , vol. 69, pp. 219–251, 2019. doi: 10.1146/ annurev-nucl-101918-023407

    work page 2019

  4. [2]

    Neutrinoless double beta decay and neutrino mass,

    J. D. Vergados, H. Ejiri, and F. ˇSimkovic, “Neutrinoless double beta decay and neutrino mass,”Interna- tional Journal of Modern Physics E, vol. 25, no. 11, p. 1 630 007, 2016.doi: 10.1142/s0218301316300071

    work page doi:10.1142/s0218301316300071 2016

  5. [3]

    Neutrinoless double beta decay: 2015 review,

    S. Dell’Oro, S. Marcocci, M. Viel, et al., “Neutrinoless double beta decay: 2015 review,” Advances in High Energy Physics , vol. 2016, pp. 1–37, 2016. doi: 10.1155/2016/2162659

    doi:10.1155/2016/2162659 2015

  6. [4]

    Scintillating bolometers for double beta decay search,

    L. Gironi, “Scintillating bolometers for double beta decay search,” Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, vol. 617, no. 1-3, pp. 478–481, 2010

    work page 2010

  7. [5]

    Development of 100Mo-containing scintillating bolometers for a high- sensitivity neutrinoless double-beta decay search,

    E. Armengaud, C. Augier, et al., “Development of 100Mo-containing scintillating bolometers for a high- sensitivity neutrinoless double-beta decay search,” The European Physical Journal C , vol. 77, no. 11, p. 785, 2017

    work page 2017

  8. [6]

    Q values of the 76Ge and 100Mo double-beta decays,

    S. Rahaman, V.-V. Elomaa, T. Eronen, et al., “Q values of the 76Ge and 100Mo double-beta decays,” Physics Letters B , vol. 662, no. 2, pp. 111–116, 2008. doi: 10.1016/j.physletb.2008.02.047

    work page doi:10.1016/j.physletb.2008.02.047 2008

Show all 23 references
  1. [7]

    The experiment for neutrinoless double-beta decay: Performance and prospects,

    E. Armengaud, C. Augier, et al., “The experiment for neutrinoless double-beta decay: Performance and prospects,” The European Physical Journal C , vol. 80, no. 1, p. 44, doi: 10.1140/epjc/s10052- 019-7578-6

    doi

  2. [8]

    Searching for neutrinoless double beta decay with the AMoRE experiments,

    S. C. Kim and AMoRE Collaborat, “Searching for neutrinoless double beta decay with the AMoRE experiments,” Nuovo Cimento C-colloquia And Communications In Physics , vol. 46, no. 1, 2023. doi: 10.1393/ncc/i2023-23008-y

    2023 doi

  3. [9]

    The CROSS experiment: Search for 0 ν2β decay with surface sensitive bolometers,

    A. Zolotarova and CROSS Collaboration, “The CROSS experiment: Search for 0 ν2β decay with surface sensitive bolometers,” ser. Journal of Physics Conference Series, vol. 1468, 2020. doi: 10.1088/1742- 6596/1468/1/012147

    2020 doi

  4. [10]

    First test of a CdMoO 4 scintillating bolometer for neutrinoless double beta decay experiments with 116Cd and 100Mo nuclides,

    M. Xue, D. Poda, Y. Zhang, et al. , “First test of a CdMoO 4 scintillating bolometer for neutrinoless double beta decay experiments with 116Cd and 100Mo nuclides,” Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associa...

    2019

  5. [11]

    Performance of ZnMoO 4 crystal as cryogenic scintil- lating bolometer to search for double beta decay of molybdenum,

    L. Gironi, C. Arnaboldi, J. W. Beeman, et al., “Performance of ZnMoO 4 crystal as cryogenic scintil- lating bolometer to search for double beta decay of molybdenum,” Journal of Instrumentation , vol. 5, no. 11, P11007, 2010. doi: 10.1088/1748-0221/5/11/P11007

    2010 doi

  6. [12]

    PbMoO4 Synthesis from ancient lead and its single crystal growth for neutrinoless double beta decay search,

    A. Khan, P. Aryal, H. Kim, et al., “PbMoO4 Synthesis from ancient lead and its single crystal growth for neutrinoless double beta decay search,” Crystals, vol. 10, no. 3, 2020

    2020

  7. [13]

    In situ observation of rock spalling in the deep tunnels of the China Jinping Underground Laboratory (2400 m depth),

    X.-T. Feng, H. Xu, S.-L. Qiu, et al. , “In situ observation of rock spalling in the deep tunnels of the China Jinping Underground Laboratory (2400 m depth),” Rock Mechanics and Rock Engineering , vol. 51, no. 4, pp. 1193–1213, 2018. doi: 10.1007/s00603-017-1387-8

    2018 doi

  8. [14]

    Various types of Anti-Reflective Coatings (ARCs) based on the layer composition and surface topography: A review,

    M. Moayedfar and M. K. Assadi, “Various types of Anti-Reflective Coatings (ARCs) based on the layer composition and surface topography: A review,” Reviews on Advanced Materials Science, vol. 53, no. 2, pp. 187–205, 2018. doi: doi:10.1515/rams-2018-0013

    2018 doi

  9. [15]

    Fluorolog series modular research fluorometers for lifetime and steady state measurement , HORIBA

  10. [16]

    Physics behind the debye temperature,

    J. Garai, “Physics behind the debye temperature,” 2009. arXiv: physics/0703001 [physics.chem-ph]

    2009 arXiv

  11. [17]

    Physical property measurement system heat capacity option user’s manual , Quantum Design

  12. [18]

    Simultaneous measurement of heat capacity and internal relaxation time,

    M. Nagasawa, “Simultaneous measurement of heat capacity and internal relaxation time,” Review of Scientific Instruments, vol. 87, no. 5, p. 054 904, 2016. doi: 10.1063/1.4948914

    2016 doi

  13. [21]

    Electrical and thermal-properties of neutron-transmutation- doped Ge at 20-mK,

    N. Wang, F. Wellstood, B. Sadoulet, et al., “Electrical and thermal-properties of neutron-transmutation- doped Ge at 20-mK,” Physical Review B, vol. 41, no. 6, pp. 3761–3768, 1990. doi: 10.1103/PhysRevB. 41.3761

    1990 doi

  14. [22]

    Offline data processing software for a Li 2MoO4 bolometer demon- stration experiment at China Jinping Underground Laboratory,

    K. Zhao, M. Xue, H. Peng, et al., “Offline data processing software for a Li 2MoO4 bolometer demon- stration experiment at China Jinping Underground Laboratory,” Journal of Instrumentation , vol. 19, no. 06, P06032, 2024. doi: 10.1088/1748-0221/19/06/P06032. 10

    2024 doi

  15. [2022]

    doi: 10.1016/j.nima.2022.167469. 9

    2022

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