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arxiv: 2604.02538 · v2 · submitted 2026-04-02 · ❄️ cond-mat.mtrl-sci

Recognition: 2 theorem links

· Lean Theorem

Temperature-dependent Raman spectra of 2H-MoS2 from Machine Learning-driven statistical sampling

Authors on Pith no claims yet

Pith reviewed 2026-05-13 20:23 UTC · model grok-4.3

classification ❄️ cond-mat.mtrl-sci
keywords Raman spectroscopy2H-MoS2temperature dependenceanharmonic effectsmachine learning samplingphonon statistics
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The pith

Machine learning sampling produces temperature-dependent Raman spectra for 2H-MoS2 that match measured frequency and linewidth trends.

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

The paper develops a machine-learning approach to generate statistical samples of atomic configurations and compute the Raman spectrum of crystalline 2H-MoS2 while incorporating thermal and anharmonic effects. The resulting peak positions and widths change with temperature in the same way as observed in experiments. This addresses the scatter in experimental Raman data by supplying a consistent first-principles description that includes temperature explicitly. The work also positions the same framework for future calculations on amorphous molybdenum sulfides.

Core claim

A machine-learning model trained on density-functional-theory configurations is used to drive statistical sampling that yields Raman spectra of 2H-MoS2, including thermal shifts and anharmonic broadening; the computed temperature dependence of frequencies and linewidths agrees closely with experimental measurements.

What carries the argument

Machine-learning-driven statistical sampling of atomic configurations to capture anharmonic phonon statistics and compute temperature-dependent Raman intensities.

If this is right

  • Temperature trends in Raman frequencies and linewidths follow directly from the sampled anharmonic statistics.
  • The same sampling procedure supplies a validated route to spectra that include explicit thermal disorder.
  • The framework can be applied to related molybdenum sulfide phases once appropriate training data are generated.

Where Pith is reading between the lines

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

  • The approach could be tested on other layered chalcogenides to check whether the same level of agreement holds when anharmonicity is stronger.
  • Extending the sampling to include explicit defects or doping would test whether the method remains predictive for real-world samples.
  • The computational cost reduction implied by the ML surrogate opens the possibility of mapping Raman response over wide temperature and pressure ranges in a single workflow.

Load-bearing premise

The machine learning model trained on a limited set of DFT configurations accurately reproduces the anharmonic phonon statistics and Raman intensities across the full temperature range without systematic bias in the sampling.

What would settle it

High-temperature Raman measurements that show frequency shifts or linewidths outside the computed trends, beyond the reported experimental uncertainty, would falsify the claimed agreement.

Figures

Figures reproduced from arXiv: 2604.02538 by Alo\"is Castellano, Matthieu J. Verstraete, Samuel Longo.

Figure 1
Figure 1. Figure 1: FIG. 1. 2H-MoS [PITH_FULL_IMAGE:figures/full_fig_p006_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. Phonon bands of MoS [PITH_FULL_IMAGE:figures/full_fig_p006_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. Calculated phonon bands at 300 K with stochastic [PITH_FULL_IMAGE:figures/full_fig_p007_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. Position and FWHM of the peaks in MoS [PITH_FULL_IMAGE:figures/full_fig_p008_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5. R [PITH_FULL_IMAGE:figures/full_fig_p008_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: FIG. 6. Theoretical isotropically averaged Raman spectra of [PITH_FULL_IMAGE:figures/full_fig_p009_6.png] view at source ↗
Figure 7
Figure 7. Figure 7: FIG. 7. Raman intensity ratio between modes E [PITH_FULL_IMAGE:figures/full_fig_p009_7.png] view at source ↗
read the original abstract

Molybdenum sulfides are in the spotlight of materials science thanks to their interesting properties for applications in optoelectronics, nanocomposites, lubricants, and catalysis. The structural characterization of Molybdenum sulfides is a crucial step to understand and tune their properties. Vibrational techniques, such as infrared and Raman spectroscopy, can directly link to structural features, but the experimental literature suffers from large variability. Theoretical calculations are a powerful tool complementing and explaining empirical measurements. The reliability of first-principles calculation depends on the level of approximation made, taking into account disorder, doping, or temperature to yield a good description of the phonon statistics and related measurable quantities, such as the infrared and Raman peaks. In this study we calculate the Raman spectrum of crystalline 2H-MoS2, including broadening and shifts due to thermal and anharmonic effects. Our results demonstrate excellent agreement with experimental measurements; notably, the calculated temperature trends in frequencies and linewidths align with empirical observations. These findings establish a robust computational framework, paving the way for similar studies on amorphous Molybdenum sulfides.

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 / 2 minor

Summary. The manuscript presents a machine-learning-driven statistical sampling approach to compute the temperature-dependent Raman spectra of crystalline 2H-MoS2, incorporating anharmonic phonon effects on frequencies and linewidths. The central claim is that the calculated temperature trends show excellent agreement with experimental measurements, establishing a computational framework extensible to amorphous molybdenum sulfides.

Significance. If the ML sampling is shown to faithfully reproduce anharmonic statistics without extrapolation bias, the work would offer an efficient route to model thermal broadening and shifts in Raman spectra for 2D materials, addressing experimental variability and enabling studies on disordered systems at lower computational cost than direct AIMD.

major comments (2)
  1. [Methods] Methods section: the manuscript provides no quantitative details on the size of the DFT training set for the ML model, the validation procedure (e.g., force or energy errors on held-out configurations), or any direct test of the sampled ensemble against long AIMD trajectories at the highest temperatures studied; this information is required to substantiate that high-T anharmonic configurations are not under-sampled.
  2. [Results] Results section on temperature trends: the reported linewidth increase with temperature is presented as aligning with experiment, yet no error bars on the computed spectra, no mean-absolute deviation from measured values, and no comparison of ML-sampled vs. AIMD phonon density of states at elevated T are given; without these the central claim of accurate anharmonic statistics remains unverifiable.
minor comments (2)
  1. [Abstract] Abstract: the phrase 'excellent agreement' is used without accompanying quantitative metrics; a brief statement of the observed frequency shift rates or linewidth slopes would strengthen the summary.
  2. [Introduction] Introduction: additional citations to recent experimental Raman studies on 2H-MoS2 would better contextualize the noted variability in measured spectra.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the constructive comments, which help clarify the validation requirements for the ML-driven approach. We address each major comment below and will incorporate the requested details and comparisons into the revised manuscript.

read point-by-point responses
  1. Referee: [Methods] Methods section: the manuscript provides no quantitative details on the size of the DFT training set for the ML model, the validation procedure (e.g., force or energy errors on held-out configurations), or any direct test of the sampled ensemble against long AIMD trajectories at the highest temperatures studied; this information is required to substantiate that high-T anharmonic configurations are not under-sampled.

    Authors: We agree that quantitative validation metrics are necessary to substantiate the reliability of the ML model and sampling at high temperatures. In the revised manuscript we will expand the Methods section to report the exact size of the DFT training set, the validation procedure including mean absolute errors on energies and forces for held-out configurations, and a direct comparison of the ML-sampled ensemble against long AIMD trajectories at the highest temperatures studied, using metrics such as the phonon density of states to confirm adequate sampling of anharmonic effects. revision: yes

  2. Referee: [Results] Results section on temperature trends: the reported linewidth increase with temperature is presented as aligning with experiment, yet no error bars on the computed spectra, no mean-absolute deviation from measured values, and no comparison of ML-sampled vs. AIMD phonon density of states at elevated T are given; without these the central claim of accurate anharmonic statistics remains unverifiable.

    Authors: We acknowledge that the absence of error bars, quantitative deviation metrics, and explicit ML-vs-AIMD comparisons limits the verifiability of the temperature trends. We will revise the Results section to include error bars on the computed Raman spectra, report the mean-absolute deviation between calculated and experimental frequency shifts and linewidths, and add a direct comparison of the phonon density of states from ML sampling versus AIMD at elevated temperatures to strengthen the evidence for accurate anharmonic statistics. revision: yes

Circularity Check

0 steps flagged

No significant circularity; central results validated against external experiments

full rationale

The paper computes temperature-dependent Raman spectra of 2H-MoS2 via machine-learning sampling of anharmonic configurations drawn from DFT, then directly compares the resulting frequency shifts and linewidth trends to independent experimental measurements. No derivation step reduces by construction to its own inputs: the ML model is trained on a finite set of DFT snapshots and used to generate statistics, but the reported agreement is with external data rather than with quantities defined or fitted inside the same workflow. No self-citation is invoked as a uniqueness theorem, no ansatz is smuggled via prior work, and no known empirical pattern is merely renamed. The derivation chain therefore remains self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Based on abstract only; no explicit free parameters, axioms, or invented entities are stated. The approach implicitly relies on the transferability of the ML model trained on DFT data, but details are absent.

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Reference graph

Works this paper leans on

79 extracted references · 79 canonical work pages

  1. [1]

    Quantum phonon occupations can be enforced in the definition of the distri- bution function

    Stochastic sampling By making an initial guess of the IFCs, it is possible to determine the harmonic canonical ensemble (NVT) probability distribution function of the positions, which is easily shown to be a Gaussian distribution around the equilibrium geometry of each atom. Quantum phonon occupations can be enforced in the definition of the distri- butio...

  2. [2]

    harmonic canonical ensemble

    Molecular dynamics sampling While the stochastic sampling explores an effective “harmonic canonical ensemble”, molecular dynamics simulations can also be used, to sample the full poten- tial energy surface (PES) and the full (classical) canoni- cal ensemble. Starting from the thermalized equilibrium (super)cell, the system is evolved under the action of t...

  3. [3]

    Materials for the Quan- tum Age

    Considerations on the supercell The choice of odd numbers of repetitions of the unit cell in the supercell along the in-plane and out-of-plane directions (such as 883) may appear unusual at first, but it is the result of a careful convergence study. Given the limited computational resources, we choose to favor the in-plane convergence over the out-of-plan...

  4. [4]

    Light emis- sion properties of 2d transition metal dichalcogenides: Fundamentals and applications.Advanced Optical Mate- rials, 6(21):1800420, 2018

    Weihao Zheng, Ying Jiang, Xuelu Hu, Honglai Li, Zhoux- iaosong Zeng, Xiao Wang, and Anlian Pan. Light emis- sion properties of 2d transition metal dichalcogenides: Fundamentals and applications.Advanced Optical Mate- rials, 6(21):1800420, 2018

  5. [5]

    Exciton physics and device application of two-dimensional transition metal dichalcogenide semiconductors.npj 2D Mater Appl, 2(1):29, 2018

    Thomas Mueller and Ermin Malic. Exciton physics and device application of two-dimensional transition metal dichalcogenide semiconductors.npj 2D Mater Appl, 2(1):29, 2018

  6. [6]

    Jaramillo, Kristina P

    Thomas F. Jaramillo, Kristina P. Jørgensen, Jacob Bonde, Jane H. Nielsen, Sebastian Horch, and Ib Chork- endorff. Identification of active edge sites for electro- chemical H2 evolution from MoS2 nanocatalysts.Sci- ence, 317(5834):100–102, 2007

  7. [7]

    Jørgensen, Jane H

    Berit Hinnemann, Poul Georg Moses, Jacob Bonde, Kristina P. Jørgensen, Jane H. Nielsen, Sebastian Horch, Ib Chorkendorff, and Jens K. Nørskov. Biomimetic hy- drogen evolution: MoS2 nanoparticles as catalyst for hy- drogen evolution.J. Am. Chem. Soc., 127(15):5308–5309, 10 2005

  8. [8]

    Transition metal dichalcogenides-based catalysts for CO2 conversion: An updated review.International Journal of Hydrogen Energy, 68:35–50, 2024

    Dalilah Mohmad Khaidar, Wan Nor Roslam Wan Isa- hak, Zatil Amali Che Ramli, and Khairul Naim Ahmad. Transition metal dichalcogenides-based catalysts for CO2 conversion: An updated review.International Journal of Hydrogen Energy, 68:35–50, 2024

  9. [9]

    2d transition metal dichalcogenides: Design, modulation, and challenges in electrocatalysis.Advanced Materials, 33(6):1907818, 2021

    Qiang Fu, Jiecai Han, Xianjie Wang, Ping Xu, Tai Yao, Jun Zhong, Wenwu Zhong, Shengwei Liu, Tan- gling Gao, Zhihua Zhang, Lingling Xu, and Bo Song. 2d transition metal dichalcogenides: Design, modulation, and challenges in electrocatalysis.Advanced Materials, 33(6):1907818, 2021

  10. [10]

    Vazirisereshk, Ashlie Martini, David A

    Mohammad R. Vazirisereshk, Ashlie Martini, David A. Strubbe, and Mehmet Z. Baykara. Solid lubrication with MoS2: A review.Lubricants, 7(7):57, 2019

  11. [11]

    Shankara, Pradeep L

    A. Shankara, Pradeep L. Menezes, K. R. Y. Simha, and Satish V. Kailas. Study of solid lubrication with MoS2 coating in the presence of additives using reciprocating ball-on-flat scratch tester.Sadhana, 33(3):207–220, 2008

  12. [12]

    Mechanical proper- ties of transition metal dichalcogenides: towards high- performance polymer nanocomposites.2D Mater., 12(1):012002, 2024

    Dimitrios G Papageorgiou, Ming Dong, Han Zhang, Mufeng Liu, and Robert J Young. Mechanical proper- ties of transition metal dichalcogenides: towards high- performance polymer nanocomposites.2D Mater., 12(1):012002, 2024

  13. [13]

    D. Yang, P. Westreich, and R. F. Frindt. Transition metal dichalcogenide/polymer nanocomposites.Nanos- tructured Materials, 12(1):467–470, 1999

  14. [14]

    2d transition metal dichalcogenide nanoma- terials: advances, opportunities, and challenges in multi- functional polymer nanocomposites.J

    Mojtaba Ahmadi, Omid Zabihi, Seokwoo Jeon, Mitra Yoonessi, Aravind Dasari, Seeram Ramakrishna, and Mi- noo Naebe. 2d transition metal dichalcogenide nanoma- terials: advances, opportunities, and challenges in multi- functional polymer nanocomposites.J. Mater. Chem. A, 8(3):845–883, 2020

  15. [15]

    Outstanding mechani- cal properties of monolayer MoS2 and its application in elastic energy storage.Phys

    Qing Peng and Suvranu De. Outstanding mechani- cal properties of monolayer MoS2 and its application in elastic energy storage.Phys. Chem. Chem. Phys., 15(44):19427–19437, 2013

  16. [16]

    Chemi- cally activating MoS2 via spontaneous atomic palladium interfacial doping towards efficient hydrogen evolution

    Zhaoyan Luo, Yixin Ouyang, Hao Zhang, Meiling Xiao, Junjie Ge, Zheng Jiang, Jinlan Wang, Daiming Tang, Xinzhong Cao, Changpeng Liu, and Wei Xing. Chemi- cally activating MoS2 via spontaneous atomic palladium interfacial doping towards efficient hydrogen evolution. Nat Commun, 9(1):2120, 2018

  17. [17]

    Boundary activated hydrogen evolution reaction on monolayer MoS2.Nat Commun, 10(1):1348, 2019

    Jianqi Zhu, Zhi-Chang Wang, Huijia Dai, Qinqin Wang, Rong Yang, Hua Yu, Mengzhou Liao, Jing Zhang, Wei Chen, Zheng Wei, Na Li, Luojun Du, Dongxia Shi, Wenlong Wang, Lixin Zhang, Ying Jiang, and Guangyu Zhang. Boundary activated hydrogen evolution reaction on monolayer MoS2.Nat Commun, 10(1):1348, 2019

  18. [18]

    J. K. Nørskov, T. Bligaard, A. Logadottir, J. R. Kitchin, J. G. Chen, S. Pandelov, and U. Stimming. Trends in the exchange current for hydrogen evolution.J. Electrochem. Soc., 152(3):J23, 2005

  19. [19]

    Botton, and Xueliang Sun

    Niancai Cheng, Samantha Stambula, Da Wang, Moham- mad Norouzi Banis, Jian Liu, Adam Riese, Biwei Xiao, Ruying Li, Tsun-Kong Sham, Li-Min Liu, Gianluigi A. Botton, and Xueliang Sun. Platinum single-atom and cluster catalysis of the hydrogen evolution reaction.Nat Commun, 7(1):13638, 2016

  20. [20]

    Charles C. L. McCrory, Suho Jung, Ivonne M. Ferrer, Shawn M. Chatman, Jonas C. Peters, and Thomas F. Jaramillo. Benchmarking hydrogen evolving reaction and oxygen evolving reaction electrocatalysts for solar water splitting devices.J. Am. Chem. Soc., 137(13):4347–4357, 2015

  21. [21]

    Benck, Thomas R

    Jesse D. Benck, Thomas R. Hellstern, Jakob Kibsgaard, Pongkarn Chakthranont, and Thomas F. Jaramillo. Catalyzing the hydrogen evolution reaction (HER) with molybdenum sulfide nanomaterials.ACS Catal., 4(11):3957–3971, 2014

  22. [22]

    Amorphous molybdenum sulfide films as catalysts for electrochemical hydrogen production in water.Chem

    Daniel Merki, St´ ephane Fierro, Heron Vrubel, and Xile Hu. Amorphous molybdenum sulfide films as catalysts for electrochemical hydrogen production in water.Chem. Sci., 2(7):1262–1267, 2011

  23. [23]

    Parkinson and Neil V

    Joseph D. Parkinson and Neil V. Rees. Hydrogen evolu- tion at MoS2: rationalising the reaction mechanism and outlook for electrocatalyst development.J Solid State Electrochem, 29(6):2075–2088, 2025

  24. [24]

    Tran, Thu V

    Phong D. Tran, Thu V. Tran, Maylis Orio, Stephane Torelli, Quang Duc Truong, Keiichiro Nayuki, Yoshikazu Sasaki, Sing Yang Chiam, Ren Yi, Itaru Honma, James Barber, and Vincent Artero. Coordination polymer structure and revisited hydrogen evolution catalytic mechanism for amorphous molybdenum sulfide.Nature Mater, 15(6):640–646, 2016

  25. [25]

    Phonon and raman scattering of two-dimensional transition metal dichalco- genides from monolayer, multilayer to bulk material

    Xin Zhang, Xiao-Fen Qiao, Wei Shi, Jiang-Bin Wu, De- Sheng Jiang, and Ping-Heng Tan. Phonon and raman scattering of two-dimensional transition metal dichalco- genides from monolayer, multilayer to bulk material. Chemical Society Reviews, 44(9):2757–2785, 2015

  26. [26]

    C. Rice, R. J. Young, R. Zan, U. Bangert, D. Wolver- son, T. Georgiou, R. Jalil, and K. S. Novoselov. Raman- scattering measurements and first-principles calculations of strain-induced phonon shifts in monolayer MoS2. Phys. Rev. B, 87(8):081307, 2013

  27. [27]

    Pollard, Nicola Bonini, Barry Brennan, Ian S

    Sandro Mignuzzi, Andrew J. Pollard, Nicola Bonini, Barry Brennan, Ian S. Gilmore, Marcos A. Pimenta, David Richards, and Debdulal Roy. Effect of disorder on raman scattering of single-layer MoS2.Phys. Rev. B, 91(19):195411, 2015

  28. [28]

    Brus, Tony F

    Changgu Lee, Hugen Yan, Louis E. Brus, Tony F. Heinz, James Hone, and Sunmin Ryu. Anomalous lattice vi- brations of single- and few-layer MoS2.ACS Nano, 4(5):2695–2700, 2010

  29. [29]

    Molina-S´ anchez and L

    A. Molina-S´ anchez and L. Wirtz. Phonons in single- layer and few-layer MoS2 and WS2.Phys. Rev. B, 84(15):155413, 2011

  30. [30]

    R. G. Gordon. Molecular motion in infrared and raman spectra.J. Chem. Phys., 43(4):1307–1312, 1965

  31. [31]

    Philip B. Allen. Theory of thermal expansion: Quasi-harmonic approximation and corrections from quasi-particle renormalization.Mod. Phys. Lett. B, 34(2):2050025, 2020

  32. [32]

    First-principles study of the phonon vibrational spectra and thermal properties of hexagonal MoS2.Solid State Sciences, 40:1–6, 2015

    Jiaonan Yuan, Zhenlong Lv, Qing Lu, Yan Cheng, Xian- grong Chen, and Lingcang Cai. First-principles study of the phonon vibrational spectra and thermal properties of hexagonal MoS2.Solid State Sciences, 40:1–6, 2015

  33. [33]

    A. H. Romero, E. K. U. Gross, M. J. Verstraete, and Olle Hellman. Thermal conductivity in PbTe from first principles.Phys. Rev. B, 91(21):214310, 2015

  34. [34]

    Nina Shulumba, Olle Hellman, and Austin J. Minnich. Lattice thermal conductivity of polyethylene molecular crystals from first-principles including nuclear quantum effects.Phys. Rev. Lett., 119(18):185901, 2017

  35. [35]

    Florian Knoop, Nina Shulumba, Alo¨ ıs Castellano, J. P. Alvarinhas Batista, Roberta Farris, Matthieu J. Ver- straete, Matthew Heine, David Broido, Dennis S. Kim, Johan Klarbring, Igor A. Abrikosov, Sergei I. Simak, and 11 Olle Hellman. TDEP: Temperature dependent effective potentials.Journal of Open Source Software, 9(94):6150, 2024

  36. [36]

    Olle Hellman, Peter Steneteg, I. A. Abrikosov, and S. I. Simak. Temperature dependent effective potential method for accurate free energy calculations of solids. Phys. Rev. B, 87(10):104111, 2013

  37. [37]

    Olle Hellman and I. A. Abrikosov. Temperature- dependent effective third-order interatomic force con- stants from first principles.Phys. Rev. B, 88(14):144301, 2013

  38. [38]

    Abrikosov, and Sergei I

    Johan Klarbring, Olle Hellman, Igor A. Abrikosov, and Sergei I. Simak. Anharmonicity and ultralow thermal conductivity in lead-free halide double perovskites.Phys. Rev. Lett., 125(4):045701, 2020

  39. [39]

    Novikov, Konstantin Gubaev, Evgeny V

    Ivan S. Novikov, Konstantin Gubaev, Evgeny V. Podryabinkin, and Alexander V. Shapeev. The MLIP package: moment tensor potentials with MPI and active learning.Mach. Learn.: Sci. Technol., 2(2):025002, 2020

  40. [40]

    Marmolejo-Tejada and Mart´ ın A

    Juan M. Marmolejo-Tejada and Mart´ ın A. Mosquera. Thermal properties of single-layer MoS2–WS2 alloys en- abled by machine-learned interatomic potentials.Chem. Commun., 58(49):6902–6905, 2022

  41. [41]

    A. K. Nair, C. M. Da Silva, and C. H. Amon. Predict- ing interfacial thermal conductance and thermal conduc- tivity across multilayer TiS2/MoS2 van der waals het- erostructures using moment tensor potentials.J. Phys. Chem. C, 129(31):14145–14153, 2025

  42. [42]

    Chunfeng Cui, Yuwen Zhang, Tao Ouyang, Chao Tang, Chaoyu He, Jin Li, Mingxing Chen, and Jianxing Zhong. Machine learning interatomic potentials as efficient tools for obtaining reasonable phonon dispersions and accu- rate thermal conductivity: A case study of typical two- dimensional materials.Appl. Phys. Lett., 123(15):152201, 2023

  43. [43]

    Machine learning assisted canonical sampling (mlacs).Computer Physics Communications, 316:109730, 2025

    Alo¨ ıs Castellano, Romuald B´ ejaud, Pauline Richard, Olivier Nadeau, Cl´ ement Duval, Gr´ egory Geneste, Gabriel Antonius, Johann Bouchet, Antoine Levitt, Gabriel Stoltz, and Fran¸ cois Bottin. Machine learning assisted canonical sampling (mlacs).Computer Physics Communications, 316:109730, 2025

  44. [44]

    Ab initio canonical sampling based on variational inference.Phys

    Alo¨ ıs Castellano, Fran¸ cois Bottin, Johann Bouchet, An- toine Levitt, and Gabriel Stoltz. Ab initio canonical sampling based on variational inference.Phys. Rev. B, 106(16):L161110, 2022

  45. [45]

    Anubhav Jain, Shyue Ping Ong, Geoffroy Hautier, Wei Chen, William Davidson Richards, Stephen Dacek, Shreyas Cholia, Dan Gunter, David Skinner, Gerbrand Ceder, and Kristin A. Persson. Commentary: The ma- terials project: A materials genome approach to acceler- ating materials innovation.APL Materials, 1(1):011002, 07 2013

  46. [46]

    Verstraete, Joao Abreu, Guillaume E

    Matthieu J. Verstraete, Joao Abreu, Guillaume E. Alle- mand, Bernard Amadon, Gabriel Antonius, Maryam Az- izi, Lucas Baguet, Cl´ ementine Barat, Louis Bastogne, Romuald B´ ejaud, Jean-Michel Beuken, Jordan Bieder, Augustin Blanchet, Francois Bottin, Johann Bouchet, Julien Bouquiaux, Eric Bousquet, James Boust, Fabien Brieuc, V´ eronique Brousseau-Couture,...

  47. [47]

    Romero, Douglas C

    Aldo H. Romero, Douglas C. Allan, Bernard Amadon, Gabriel Antonius, Thomas Applencourt, Lucas Baguet, Jordan Bieder, Fran¸ cois Bottin, Johann Bouchet, Eric Bousquet, Fabien Bruneval, Guillaume Brunin, Damien Caliste, Michel Cˆ ot´ e, Jules Denier, Cyrus Dreyer, Philippe Ghosez, Matteo Giantomassi, Yannick Gillet, Olivier Gingras, Donald R. Hamann, Geoffr...

  48. [48]

    Hamann, Ge- offroy Hautier, Xu He, Nicole Helbig, Natalie Holzwarth, Yongchao Jia, Fran¸ cois Jollet, William Lafargue-Dit- Hauret, Kurt Lejaeghere, Miguel A

    Xavier Gonze, Bernard Amadon, Gabriel Antonius, Fr´ ed´ eric Arnardi, Lucas Baguet, Jean-Michel Beuken, Jordan Bieder, Fran¸ cois Bottin, Johann Bouchet, Eric Bousquet, Nils Brouwer, Fabien Bruneval, Guillaume Brunin, Th´ eo Cavignac, Jean-Baptiste Charraud, Wei Chen, Michel Cˆ ot´ e, Stefaan Cottenier, Jules Denier, Gr´ egory Geneste, Philippe Ghosez, Ma...

  49. [49]

    In- teratomic force constants including the DFT-d dispersion contribution.Phys

    Benoit Van Troeye, Marc Torrent, and Xavier Gonze. In- teratomic force constants including the DFT-d dispersion contribution.Phys. Rev. B, 93(14):144304, 2016

  50. [50]

    Raffaello Bianco, Ion Errea, Lorenzo Paulatto, Mat- teo Calandra, and Francesco Mauri. Second-order structural phase transitions, free energy curvature, and temperature-dependent anharmonic phonons in the self- consistent harmonic approximation: Theory and stochas- tic implementation.Phys. Rev. B, 96:014111, Jul 2017

  51. [51]

    Isotope scattering of dispersive phonons in ge.Phys

    Shin-ichiro Tamura. Isotope scattering of dispersive phonons in ge.Phys. Rev. B, 27:858–866, Jan 1983. 12

  52. [52]

    R. A. Cowley. The lattice dynamics of an anharmonic crystal.Advances in Physics, 12(48):421–480, 1963

  53. [53]

    Light scattering in solids II: Basic concepts and instru- mentation, 1982

  54. [54]

    The atomic simulation environment—a python library for working with atoms.Journal of Physics: Con- densed Matter, 29(27):273002, jun 2017

    Ask Hjorth Larsen, Jens Jørgen Mortensen, Jakob Blomqvist, Ivano E Castelli, Rune Christensen, Marcin Du lak, Jesper Friis, Michael N Groves, Bjørk Hammer, Cory Hargus, Eric D Hermes, Paul C Jennings, Peter Bjerre Jensen, James Kermode, John R Kitchin, Esben Leonhard Kolsbjerg, Joseph Kubal, Kristen Kaasbjerg, Steen Lysgaard, J´ on Bergmann Maronsson, Tri...

  55. [55]

    Phonons and related crystal prop- erties from density-functional perturbation theory.Rev

    Stefano Baroni, Stefano de Gironcoli, Andrea Dal Corso, and Paolo Giannozzi. Phonons and related crystal prop- erties from density-functional perturbation theory.Rev. Mod. Phys., 73:515–562, Jul 2001

  56. [56]

    Dynamical matrices, born effective charges, dielectric permittivity tensors, and interatomic force constants from density-functional per- turbation theory.Phys

    Xavier Gonze and Changyol Lee. Dynamical matrices, born effective charges, dielectric permittivity tensors, and interatomic force constants from density-functional per- turbation theory.Phys. Rev. B, 55:10355–10368, Apr 1997

  57. [57]

    Long.Vibrational Raman Scattering, chapter 5, pages 85–152

    Derek A. Long.Vibrational Raman Scattering, chapter 5, pages 85–152. John Wiley & Sons, Ltd, 2002

  58. [58]

    A. P. Thompson, H. M. Aktulga, R. Berger, D. S. Bolin- tineanu, W. M. Brown, P. S. Crozier, P. J. in ’t Veld, A. Kohlmeyer, S. G. Moore, T. D. Nguyen, R. Shan, M. J. Stevens, J. Tranchida, C. Trott, and S. J. Plimpton. LAMMPS - a flexible simulation tool for particle-based materials modeling at the atomic, meso, and continuum scales.Comp. Phys. Comm., 271...

  59. [59]

    S. H. El-Mahalawy and B. L. Evans. The thermal ex- pansion of 2H-MoS2, 2H-MoSe2 and 2H-WSe2 between 20 and 800°c.J Appl Cryst, 9(5):403–406, 1976

  60. [60]

    Murray and B

    R. Murray and B. Evans. The thermal expansion of 2H- MoS2 and 2H-WSe2 between 10 and 320 k.J Appl Cryst, 12(3):312–315, 1979

  61. [61]

    Electronic prop- erties of bulk and monolayer TMDs: Theoretical study within DFT framework (GVJ-2e method).physica status solidi (a), 214(12):1700218, 2017

    Julia Gusakova, Xingli Wang, Li Lynn Shiau, Anna Krivosheeva, Victor Shaposhnikov, Victor Borisenko, Vasilii Gusakov, and Beng Kang Tay. Electronic prop- erties of bulk and monolayer TMDs: Theoretical study within DFT framework (GVJ-2e method).physica status solidi (a), 214(12):1700218, 2017

  62. [62]

    Espejo, T

    C. Espejo, T. Rangel, A. H. Romero, X. Gonze, and G.- M. Rignanese. Band structure tunability in MoS2 under interlayer compression: A DFT and gw study.Phys. Rev. B, 87(24):245114, 2013

  63. [63]

    Phonon dispersion in MoS2.Phys

    Hans Tornatzky, Roland Gillen, Hiroshi Uchiyama, and Janina Maultzsch. Phonon dispersion in MoS2.Phys. Rev. B, 99(14):144309, 2019

  64. [64]

    Phonon scattering pro- cesses in molybdenum disulfide.Appl

    Zi-Yu Cao and Xiao-Jia Chen. Phonon scattering pro- cesses in molybdenum disulfide.Appl. Phys. Lett., 114(5), 2019

  65. [65]

    T. J. Wieting and J. L. Verble. Infrared and raman studies of long-wavelength optical phonons in hexagonal MoS2.Phys. Rev. B, 3(12):4286–4292, 1971

  66. [66]

    Satyaprakash Sahoo, Anand P. S. Gaur, Majid Ahmadi, Maxime J.-F. Guinel, and Ram S. Katiyar. Temperature- dependent raman studies and thermal conductivity of few-layer MoS2.J. Phys. Chem. C, 117(17):9042–9047, 2013

  67. [67]

    Thripuranthaka, Ranjit V

    M. Thripuranthaka, Ranjit V. Kashid, Chandra Sekhar Rout, and Dattatray J. Late. Temperature de- pendent raman spectroscopy of chemically derived few layer MoS2 and WS2 nanosheets.Applied Physics Let- ters, 104(8):081911, 2014

  68. [68]

    Lanzillo, A

    Nicholas A. Lanzillo, A. Glen Birdwell, Matin Amani, Frank J. Crowne, Pankaj B. Shah, Sina Najmaei, Zheng Liu, Pulickel M. Ajayan, Jun Lou, Madan Dubey, Saroj K. Nayak, and Terrance P. O’Regan. Temperature- dependent phonon shifts in monolayer MoS2.Applied Physics Letters, 103(9):093102, 2013

  69. [69]

    Resonant raman scatter- ing at exciton states tuned by pressure and temperature in 2H-MoS2.Phys

    Tsachi Livneh and Eran Sterer. Resonant raman scatter- ing at exciton states tuned by pressure and temperature in 2H-MoS2.Phys. Rev. B, 81(19):195209, 2010

  70. [70]

    Excitation mechanism of a1g mode and origin of nonlinear temperature dependence of raman shift of CVD-grown mono- and few-layer MoS2 films

    Tianqi Yang, Xiaoting Huang, Hong Zhou, Guangheng Wu, and Tianshu Lai. Excitation mechanism of a1g mode and origin of nonlinear temperature dependence of raman shift of CVD-grown mono- and few-layer MoS2 films. Opt. Express, OE, 24(11):12281–12292, 2016

  71. [71]

    Simpson, Simone Bertolazzi, Ja- copo Brivio, Michael Watson, Xufei Wu, Andras Kis, Tengfei Luo, Angela R

    Rusen Yan, Jeffrey R. Simpson, Simone Bertolazzi, Ja- copo Brivio, Michael Watson, Xufei Wu, Andras Kis, Tengfei Luo, Angela R. Hight Walker, and Huili Grace Xing. Thermal conductivity of monolayer molybdenum disulfide obtained from temperature-dependent raman spectroscopy.ACS Nano, 8(1):986–993, 2014

  72. [72]

    Ultra- fast nonadiabatic phonon renormalization in photoex- cited single-layer MoS2.The Journal of Physical Chem- istry C, 127(33):16515–16524, 2023

    Nina Girotto, Fabio Caruso, and Dino Novko. Ultra- fast nonadiabatic phonon renormalization in photoex- cited single-layer MoS2.The Journal of Physical Chem- istry C, 127(33):16515–16524, 2023

  73. [73]

    Real-time gw- ehrenfest-fan-migdal method for nonequilibrium 2d ma- terials.Nano Letters, 23(15):7029–7036, 2023

    Enrico Perfetto and Gianluca Stefanucci. Real-time gw- ehrenfest-fan-migdal method for nonequilibrium 2d ma- terials.Nano Letters, 23(15):7029–7036, 2023. PMID: 37493350

  74. [74]

    Resonance raman scattering in bulk 2H-MX2 (M=Mo, W; X=S, Se) and monolayer MoS2.J

    Jia-He Fan, Po Gao, An-Min Zhang, Bai-Ren Zhu, Hua- Ling Zeng, Xiao-Dong Cui, Rui He, and Qing-Ming Zhang. Resonance raman scattering in bulk 2H-MX2 (M=Mo, W; X=S, Se) and monolayer MoS2.J. Appl. Phys., 115(5):053527, 2014

  75. [75]

    Najmaei, Z

    S. Najmaei, Z. Liu, P. M. Ajayan, and J. Lou. Thermal effects on the characteristic raman spectrum of molybde- num disulfide (MoS2) of varying thicknesses.Appl. Phys. Lett., 100(1):013106, 2012

  76. [76]

    Ajayan, and J

    Sina Najmaei, Pulickel M. Ajayan, and J. Lou. Quanti- tative analysis of the temperature dependency in raman active vibrational modes of molybdenum disulfide atomic layers.Nanoscale, 5(20):9758–9763, 2013

  77. [77]

    Go lasa, M

    K. Go lasa, M. Grzeszczyk, P. Leszczy´ nski, C. Faugeras, A. A. L. Nicolet, A. Wysmo lek, M. Potemski, and A. Babi´ nski. Multiphonon resonant raman scattering in MoS2.Appl. Phys. Lett., 104(9):092106, 2014

  78. [78]

    A comprehen- sive multiphonon spectral analysis in MoS2.2D Mater., 2(3):035003, 2015

    Tsachi Livneh and Jonathan E Spanier. A comprehen- sive multiphonon spectral analysis in MoS2.2D Mater., 2(3):035003, 2015

  79. [79]

    K. K. Kam and B. A. Parkinson. Detailed photocurrent spectroscopy of the semiconducting group VIB transition metal dichalcogenides.J. Phys. Chem., 86(4):463–467, 1982