REVIEW 3 major objections 5 minor 147 references
Neutron scattering studies of complex lattice dynamics in energy materials
T0 review · 3 major / 5 minor · reviewed 2026-08-15 · deepseek-v4-flash
Pith's one-line read Phonon anharmonicity, not liquid-like phonons, explains ultra-low thermal conductivity in superionic thermoelectrics, a review of neutron scattering evidence concludes.
desk verdict A useful and largely accurate neutron-scattering review, but the central causal claim about anharmonicity in superionic thermoelectrics is stronger than the presented evidence. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The load-bearing observable is the phonon linewidth in the dynamic structure factor $S(\mathbf{Q},\omega)$ measured by inelastic and quasielastic neutron scattering. A phonon peak that broadens faster than its energy shift as temperature rises signals overdamping and giant anharmonic scattering; a peak whose width exceeds its center energy means the vibration mode is overdamped and needs no activation energy to move. In the decisive superionic case, the machinery is the temperature series of the low-frequency (2-4 meV) phonon band together with the tracking of the transverse acoustic phonon across the phase transition: the TA phonon survives, and the rapid linewidth growth of the lower band matches the drop in lattice thermal conductivity. Quasielastic broadening and the elastic incoherent structure factor supply the complementary ingredient, distinguishing long-range diffusion from geometrically confined molecular rotation and tying the dynamics of the mobile sublattice to the rigid framework.
What would settle it
A direct test would compare the measured temperature dependence of the 2-4 meV phonon linewidth in Ag8SnSe6 with a model that includes only ionic hopping, static disorder, and thermal expansion and no phonon-phonon anharmonicity; if that model reproduces the observed broadening, the central attribution fails. Conversely, a single-crystal experiment on another superionic thermoelectric showing that the transverse acoustic phonon vanishes at the phase transition while lattice thermal conductivity remains ultra-low would support the competing liquid-like picture the paper rejects.
Extended reading notes
Core claim
On the paper's own terms, the central discovery is that the mechanism behind ultra-low lattice thermal conductivity in superionic thermoelectrics is extreme phonon anharmonic scattering, and the paper closes the book on the competing liquid-like phonon proposal for the case of Ag8SnSe6. Inelastic neutron scattering on single crystals shows the transverse acoustic phonon still exists at and above the superionic phase transition, contradicting the idea that a diffusing sublattice destroys transverse phonons; in powders, the 2-4 meV low-energy optical phonon band broadens rapidly between 8 K and 100 K, and that linewidth growth tracks the measured drop in lattice thermal conductivity between 20 and 50 K. The same anharmonic, coupled picture is then used to interpret five material classes: the overdamped phonons and weakly bonded selenium atoms that mediate ion diffusion in argyrodite solid electrolytes, the rotation-lattice coupling and configurational entropy in the NH4I barocaloric, the low-energy phonon damping that lengthens hot-carrier lifetimes in CsPbBr3, and the valence-electron transfer between sublattices that drives the magnetostructural transition in MnCoGe. The concluding claim is that lattice dynamics in energy conversion and storage materials always operate through anharmonic evolution of phonons in combination with sublattice, charge, and spin degrees of freedom.
Load-bearing premise
The conclusion that giant phonon anharmonic scattering, not liquid-like phonon behavior, causes the ultra-low lattice thermal conductivity of Ag8SnSe6 rests on the assumption that the rapid broadening of the 2-4 meV optical phonon band between 8 K and 100 K is dominated by phonon-phonon anharmonicity and not by ionic diffusion, disorder-induced scattering, or thermal expansion.
Editorial extensions
If this is right
- If anharmonic scattering is the main heat-flow suppressor in superionic thermoelectrics, then the design target shifts from creating liquid-like sublattices to steepening phonon-phonon scattering, for example through shallow energy surfaces and low-frequency optical phonons.
- The survival of transverse acoustic phonons above the superionic transition in Ag8SnSe6 means the liquid-like phonon picture cannot explain the ultralow lattice thermal conductivity of this compound; the same single-crystal measurement should be extended to other superionics to see whether the conclusion generalizes.
- In argyrodite solid electrolytes, the weakly bonded selenium atoms that change displacement most during the superionic transition are the right chemical sites for tuning ionic conductivity and stability.
- In plastic crystals such as NH4I, strengthening or weakening lattice anharmonicity controls the hydrogen-bond coupling between ammonium ions and the iodide framework, and therefore the pressure scale and configurational entropy of the barocaloric effect.
- In halide perovskites, phonon anharmonicity of the [PbBr6] sublattice governs electron-phonon coupling and hot-carrier lifetime, so phonon engineering is also electronic engineering.
Reading between the lines
- The same linewidth-versus-temperature test used for Ag8SnSe6 could be applied to other superionic thermoelectrics (Cu2Se, AgCrSe2, CuCrSe2) to determine whether anharmonic scattering universally outweighs liquid-like behavior or whether some compounds genuinely lose transverse phonons.
- If anharmonic phonon scattering is the dominant heat-flow suppressor, then doping or strain strategies that increase phonon-phonon scattering without promoting ion migration could decouple low thermal conductivity from high ionic conductivity, a separation the review does not itself propose.
- The review's open question about a two-channel thermal transport model suggests a concrete neutron experiment: measuring phonon linewidths and the quasielastic/diffusive channel in the same crystal and temperature range to look for an off-diagonal contribution; this is an extension implied by but not performed in the paper.
- Machine-learning molecular dynamics already reproduces the sublattice dynamics in the argyrodite example, so it could in principle be used to predict which chemical substitutions steepen the shallow energy landscape, turning the anharmonicity claim into a search rule for new low-conductivity materials.
Signed reviews
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. This review paper surveys neutron scattering techniques for studying lattice dynamics in energy materials, covering neutron diffraction, total scattering, quasi-elastic and inelastic neutron scattering, and their principles, spectrometers, and data-analysis methods. It then presents five case studies: superionic thermoelectric Ag8SnSe6, solid electrolyte Ag8SnSe6, plastic-crystal barocaloric NH4I, photovoltaic CsPbBr3, and magnetocaloric MnCoGe. The paper's central scientific message, stated in Sections 3 and 7, is that in superionic thermoelectric materials the suppression of lattice thermal conductivity by giant phonon anharmonic scattering is more important than that by the superionic phase transition or the liquid-like phonon model, and more broadly that lattice dynamics in energy materials always act through anharmonic phonon evolution coupled with sublattice, charge, and spin degrees of freedom.
Significance. If the central claim were fully supported, the review would provide a useful synthesis of neutron-scattering contributions to energy materials research, and it does have several strengths: it accurately reproduces the main claims of the cited primary literature, it clearly explains the operation and capabilities of different neutron spectrometers, it explicitly identifies open problems (e.g., the two-channel thermal transport model, multi-ion concerted diffusion, and the need for polarized inelastic scattering), and it includes a candid discussion of limitations. However, the review's strongest claim about the causal priority of phonon anharmonicity is not adequately supported by the evidence presented, and the heavy reliance on the authors' own measurements for four of the five case studies makes the synthesis more self-referential than independent. These issues are addressable by revising the framing and adding critical discussion of alternative explanations, so major revision is appropriate.
major comments (3)
- [Section 3] The central claim that in Ag8SnSe6 'the suppression of lattice thermal conductivity by giant phonon anharmonic scattering is more important than that by superionic phase transition and liquid-like phonon model' is under-supported by the evidence shown in Fig. 7. The survival of TA phonons at 450 K (Fig. 7(a),(b)) rules out only the specific liquid-like mechanism in which TA modes vanish; it does not by itself demonstrate that anharmonic scattering dominates. The rapid broadening of the 2–4 meV optical-phonon band in powder S(Q,E) between 8 K and 100 K (Fig. 7(c)–(f)) is attributed to 'extremely large phonon anharmonic behavior,' but the review does not exclude temperature-dependent disorder on the Ag sublattice, quasi-harmonic thermal-expansion shifts, or powder-average dispersion effects as contributors to the observed broadening. Without a quantitative comparison (e.g., energy- and momentum-resolved linewidth analysis against anharmonic DFT or molecular-dynamics predictions, or single-crystal measurements), the priority statement in Section 7 is not established.
- [Section 3] The argument that the linewidth broadening 'is highly consistent with the trend of rapid decrease of lattice thermal conductivity' is correlational. Agreement between a microscopic observable and the macroscopic transport curve cannot assign causal priority to phonon-phonon anharmonicity over other temperature-dependent scattering processes unless those processes are separately quantified. The review should either present such a quantitative decomposition or soften the causal ranking.
- [Sections 3–6] Four of the five case studies are drawn from the authors' own publications (Refs. 31, 68, 138, and 139). The review therefore reads largely as a self-referential summary of the authors' results rather than an independent synthesis. This does not invalidate the scientific content, but for a review article the balance should be improved by adding independent corroborating or conflicting works, and by explicitly mentioning the self-citation-heavy basis in the text.
minor comments (5)
- [Section 1] The phrase 'crystal many alone fail' appears to be a typo for 'crystal structure alone fails'.
- [Section 5] The abbreviation 'ESIF' on page 26 should be 'EISF' to match the correct usage elsewhere in the paper; the text also contains '(ompressibility)' which should be 'compressibility'.
- [Section 7] The sentence 'one is the ... of random diffusion between different phonon branches' is missing a word; it should likely read 'the emergence/effect of random diffusion'.
- [Sections 4 and 6] The same reference [31] is used for both the superionic thermoelectric study and the solid-electrolyte study; the text should distinguish the two datasets more clearly when citing it in different contexts.
- [Abstract] The header abstract and the translated abstract in the full text differ in length and wording; they should be harmonized in the final version.
Circularity Check
No circular derivation: the review synthesizes published experimental results without reducing predictions to fitted inputs or self-citation chains.
full rationale
This paper is a review of neutron scattering studies of lattice dynamics in energy materials; it does not present a new derivation, fitting procedure, or predictive model. The strongest claim, that giant phonon anharmonic scattering is 'more important' than liquid-like phonon behavior in superionic thermoelectrics, is supported by previously published single-crystal inelastic neutron scattering data on Ag8SnSe6 (survival of TA phonons across the superionic transition) and powder S(Q,E) measurements (rapid temperature broadening of low-energy optical phonons). These are externally falsifiable experimental observations, not quantities defined in terms of the review's conclusion. Although the paper frequently cites work by the same authors (e.g., Ref. [31]), those citations point to concrete measurements and machine-learning molecular dynamics results that stand independently of the present review; they are not invoked as a 'uniqueness theorem' or as an unverified premise that forces the conclusion. The interpretive step from linewidth broadening to anharmonicity is a scientific judgment that could be challenged by competing explanations such as disorder or thermal expansion, but that is a question of evidential support and mechanistic inference, not circularity. No equation in the paper reduces a predicted output to an input, no fitted parameter is renamed as a prediction, and no result is imported solely through a self-citation chain. The review is therefore not circular.
Assumptions & free parameters
assumptions (4)
- standard math The double differential scattering cross section follows Fermi's golden rule with the dynamical structure factor S(Q, omega) as given in Eqs. (1)-(4).
- domain assumption Lattice thermal conductivity can be described by the phonon free gas model kappa_lat = (1/3) c v l.
- domain assumption The temperature dependence of phonon linewidth broadening in Ag8SnSe6 is dominated by anharmonic phonon-phonon scattering rather than by ionic diffusion or disorder.
- domain assumption EISF analysis and QENS can determine the orientational degrees of freedom of [NH4]+ tetrahedra in NH4I.
Cite this review
Pith. "Pith review of Neutron scattering studies of complex lattice dynamics in energy materials." pith.science (2026). https://pith.science/paper/O4PR67DE
@misc{pith2026250506076,
author = {Pith},
title = {Pith review of: Neutron scattering studies of complex lattice dynamics in energy materials},
year = {2026},
howpublished = {\url{https://pith.science/paper/O4PR67DE}},
note = {Machine review of arXiv:2505.06076}
}
read the original abstract
Lattice dynamics play a crucial role in understanding the physical mechanisms of cutting-edge energy materials. Many excellent energy materials have complex multiple-sublattice structures, with intricate lattice dynamics, and the underlying mechanisms are difficult to understand. Neutron scattering technologies, which are known for their high energy and momentum resolution, are powerful tools for simultaneously characterizing material structure and complex lattice dynamics. In recent years, neutron scattering techniques have made significant contributions to the study of energy materials, shedding light on their physical mechanisms. This review article details several neutron scattering techniques commonly used in energy material research, including neutron diffraction, total neutron scattering, quasi-elastic and inelastic neutron scattering. Then, some important research progress made in the field of energy materials in recent years using neutron scattering as the main characterization method is reviewed, including ultra-low lattice thermal conductivity in superionic thermoelectric materials, ion diffusion mechanism of solid-state electrolytes, plastic-crystalline phase transition and configuration entropy changes in barocaloric materials, lattice anharmonicity and charge transport in photovoltaic materials, and first-order magnetic-structural phase transition in magnetocaloric materials. In these complex energy conversion and storage materials, lattice dynamics do not work independently, and their functioning in macroscopic physical properties is always achieved through correlation or mutual coupling with other degrees of freedom, such as sublattices, charge, spin, etc. Through these typical examples, this review paper can provide a reference for further exploring and understanding the energy materials and lattice dynamics.
Reference graph
Works this paper leans on
-
[1]
Huang K, Han R Q 1988 Solid State Physics (Beijing: Higher Education Press)
1988
-
[2]
Ashcroft N W, Mermin N D 1976 Solid State Physics (Holt, Rinehart and Winston)
1976
-
[3]
Leguy A M, Frost J M, McMahon A P, Sakai V G, Kochelmann W, Law C, Li X, Foglia F, Walsh A, O'Regan B C, Nelson J, Cabral J T, Barnes P R 2015 Nat. Commun. 6 7124
2015
-
[4]
Wang K, Ren Q Y , Gu Z Q, Duan C M, Wang J Z, Zhu F, Fu Y Y , Hao J P, Zhu J F, He L H, Wang C W, Lu Y Y , Ma J, Ma C 2021 Nat. Commun. 12 4410
2021
-
[5]
Kortshagen Group Thermoelectrics https://kortshagen.umn.edu/research/thermoelectrics
-
[6]
Pressure Makes Best Cooling https://j-parc.jp/en/topics/2019/190329.html [2019-3-29]
2019
-
[7]
He J, Tritt T M 2017 Science 357 1369
2017
-
[8]
Ye L X 2007 Semiconductor Physics (Beijing: Higher Education Press)
2007
Show all 147 references
-
[9]
Chen Z W, Zhang X Y , Pei Y Z 2018 Adv. Mater. 30 1705617
2018
-
[10]
Qiu W, Xi L, Wei P, Ke X, Yang J, Zhang W 2014 Proc. Natl. Acad. Sci. U. S. A. 111 15031
2014
-
[11]
Fu C G, Wu H J, Liu Y T, He J Q, Zhao X B, Zhu T J 2016 Adv. Sci. 3 1600035
2016
-
[12]
Qian X, Zhou J W, Chen G 2021 Nat. Mater. 20 1188
2021
-
[13]
China Phys
Wei B, Sun Q Y , Li C, Hong J W 2021 Sci. China Phys. Mech. Astron. 64 117001
2021
-
[14]
Akkerman Q A, Manna L 2020 ACS Energy Lett. 5 604
2020
-
[15]
Muy S, Bachman J C, Giordano L, Chang H H, Abernathy D L, Bansal D, Delaire O, Hori S, Kanno R, Maglia F, Lupart S, Lamp P, Shao-Horn Y 2018 Energy Environ. Sci. 11 850
2018
-
[16]
Cazorla C 2019 Nature 567 470
2019
-
[17]
Shen J J, Fang T, Fu T Z, Xin J Z, Zhao X B, Zhu T J 2019 J. Inorg. Mater. 34 260
2019
-
[18]
Lin S Q, Li W, Li S S, Zhang X Y , Chen Z W, Xu Y D, Chen Y , Pei Y Z 2017 Joule 1 816
2017
-
[19]
Energy Mater
Li W, Lin S Q, Weiss M, Chen Z W, Li J, Xu Y D, Zeier W G, Pei Y Z 2018 Adv. Energy Mater. 8 1800030
2018
-
[20]
Xia K Y , Hu C L, Fu C G, Zhao X B, Zhu T J 2021 Appl. Phys. Lett. 118 140503
2021
-
[21]
Zhu J F, Ren Q Y , Chen C, Wang C, Shu M F, He M, Zhang C P, Le M D, Torri S, Wang C W, Wang J L, Cheng Z X, Li L S, Wang G H, Jiang Y X, Wu M Z, Qu Z, Tong X, Chen Y , Zhang Q, Ma J 2024 Nat. Commun. 15 2618
2024
-
[22]
Li X Y , Liu P F, Zhao E Y , Zhang Z G, Guidi T, Le M D, Avdeev M, Ikeda K, Otomo T, Kofu M, Nakajima K, Chen J, He L H, Ren Y , Wang X L, Wang B T, Ren Z F, Zhao H Z, Wang F W 2020 Nat. Commun. 11 942
2020
-
[23]
Liu H L, Shi X, Xu F F, Zhang L L, Zhang W Q, Chen L D, Li Q, Uher C, Day T, Snyder G J 2012 Nat. Mater. 11 422
2012
-
[24]
Li L, Liu Y , Dai J Y , Hong A J, Zeng M, Yan Z B, Xu J, Zhang D, Shan D, Liu S L, Ren Z F, Liu J M 2016 J. Mater. Chem. C 4 5806
2016
-
[25]
Christensen M, Abrahamsen A B, Christensen N B, Juranyi F, Andersen N H, Lefmann K, Andreasson J, Bahl C R, Iversen B B 2008 Nat. Mater. 7 811
2008
-
[26]
Koza M M, Johnson M R, Viennois R, Mutka H, Girard L, Ravot D 2008 Nat. Mater. 7 805
2008
-
[27]
Lee S, Esfarjani K, Luo T F, Zhou J W, Tian Z T, Chen G 2014 Nat. Commun. 5 3525
2014
-
[28]
Delaire O, Ma J, Marty K, May A F, McGuire M A, Du M H, Singh D J, Podlesnyak A, Ehlers G, Lumsden M D, Sales B C 2011 Nat. Mater. 10 614
2011
-
[29]
V oneshen D J, Walker H C, Refson K, Goff J P 2017 Phys. Rev. Lett. 118 145901
2017
-
[30]
Li C W, Hong J, May A F, Bansal D, Chi S, Hong T, Ehlers G, Delaire O 2015 Nat. Phys. 11 1063
2015
-
[31]
Ren Q Y , Gupta M K, Jin M, Ding J, Wu J, Chen Z W, Lin S Q, Fabelo O, Rodríguez-Velamazán J A, Kofu M, Nakajima K, Wolf M, Zhu F, Wang J L, Cheng Z, Wang G, Tong X, Pei Y Z, Delaire O, Ma J 2023 Nat. Mater. 22 999
2023
-
[32]
Delaire O, Marty K, Stone M B, Kent P R C, Lucas M S, Abernathy D L, Mandrus D, Sales B C 2011 Proc. Natl. Acad. Sci. U. S. A. 108 4725
2011
-
[33]
Li C W, Hellman O, Ma J, May A F, Cao H B, Chen X, Christianson A D, Ehlers G, Singh D J, Sales B C, Delaire O 2014 Phys. Rev. Lett. 112 175501
2014
-
[34]
Han S, Dai S N, Ma J, Ren Q Y , Hu C L, Gao Z H, Duc Le M, Sheptyakov D, Miao P, Torii S, Kamiyama T, Felser C, Yang J, Fu C G, Zhu T J 2023 Nat. Phys. 19 1649
2023
-
[35]
Bachman J C, Muy S, Grimaud A, Chang H H, Pour N, Lux S F, Paschos O, Maglia F, Lupart S, Lamp P, Giordano L, Shao-Horn Y 2015 Chem. Rev. 116 140
2015
-
[36]
Gao Y R, Nolan A M, Du P, Wu Y F, Yang C, Chen Q L, Mo Y F, Bo S H 2020 Chem. Rev. 120 5954
2020
-
[37]
Famprikis T, Canepa P, Dawson J A, Islam M S, Masquelier C 2019 Nat. Mater. 18 1278
2019
-
[38]
Kamaya N, Homma K, Yamakawa Y , Hirayama M, Kanno R, Yonemura M, Kamiyama T, Kato Y , Hama S, Kawamoto K, Mitsui A 2011 Nat. Mater. 10 682
2011
-
[39]
Energy 1 16030
Kato Y , Hori S, Saito T, Suzuki K, Hirayama M, Mitsui A, Yonemura M, Iba H, Kanno R 2016 Nat. Energy 1 16030
2016
-
[40]
Lanigan-Atkins T, He X, Krogstad M J, Pajerowski D M, Abernathy D L, Xu G, Xu Z, Chung D Y , Kanatzidis M G, Rosenkranz S, Osborn R, Delaire O 2021 Nat. Mater. 20 977
2021
-
[41]
Li B, Kawakita Y , Liu Y , Wang M, Matsuura M, Shibata K, Ohira-Kawamura S, Yamada T, Lin S Q, Nakajima K, Liu S F 2017 Nat. Commun. 8 16086
2017
-
[42]
Li B, Kawakita Y , Ohira-Kawamura S, Sugahara T, Wang H, Wang J L, Chen Y , Kawaguchi S I, Kawaguchi S, Ohara K, Li K, Yu D, Mole R, Hattori T, Kikuchi T, Yano S I, Zhang Z, Zhang Z, Ren W, Lin S Q, Sakata O, Nakajima K, Zhang Z 2019 Nature 567 506
2019
-
[43]
Xie M X, Ren J 2022 Wuli 51 855
2022
-
[44]
Ren Q Y , Chen M N, Geng Y S, Ma J, Tong X 2021 Sci. Sin. : Phys. Mech. Astron. 51 087332
2021
-
[45]
Northwestern Uni
Ma J, Ren Q Y 2017 J. Northwestern Uni. (Nat. Sci. Ed.) 47 783
2017
-
[46]
Squires G L 1978 Introduction to the Theory of Thermal Neutron Scattering (Cambridge: Cambridge University Press
1978
-
[47]
4) (Singapore: World Scientific)
Furrer A, Mesot J, Strässle T 2009 Neutron Scattering in Condensed Matter Physics (V ol. 4) (Singapore: World Scientific)
2009
-
[48]
Sears V F 1992 Neutron News 3 26
1992
-
[49]
188 05001
Berrod Q, Lagrené K, Ollivier J, Zanotti J M 2018 EPJ Web Conf. 188 05001
2018
-
[50]
Wang Y X, Gong W, Su Y H, Li B 2024 Acta Metall. Sin. 60 1001
2024
-
[51]
Delaire O A, Stassis C 2012 Phonon Studies (John Wiley & Sons)
2012
-
[52]
Li B, Wang H, Kawakita Y , Zhang Q, Feygenson M, Yu H L, Wu D, Ohara K, Kikuchi T, Shibata K, Yamada T, Ning X K, Chen Y , He J Q, Vaknin D, Wu R Q, Nakajima K, Kanatzidis M G 2018 Nat. Mater. 17 226
2018
-
[53]
Božin E S, Malliakas C D, Souvatzis P, Proffen T, Spaldin N A, Kanatzidis M G, Billinge S J L 2010 Science 330 1660
2010
-
[54]
Sakata M, Sato M 1990 Acta Crystallogr. Sec. A 46 263
1990
-
[55]
Keen D A, Goodwin A L 2015 Nature 521 303
2015
-
[56]
11) (OUP Oxford)
Neder R B, Proffen T 2008 Diffuse Scattering and Defect Structure Simulations: A Cook Book Using the Program DISCUS (V ol. 11) (OUP Oxford)
2008
-
[57]
Weber T, Simonov A 2012 Zeitschrift für Kristallographie 227 238
2012
-
[58]
Cai G L, Li Y H, Fu Y , Yang H, Mei L, Nie Z Y , Li T F, Liu H, Ke Y B, Wang X L, Brédas J L, Tang M C, Chen X K, Zhan X W, Lu X H 2024 Nat. Commun. 15 2784
2024
-
[59]
Jeffries C M, Ilavsky J, Martel A, Hinrichs S, Meyer A, Pedersen J S, Sokolova A V , Svergun D I 2021 Nature Reviews Methods Primers 1 70
2021
-
[60]
Skoda M W A 2019 Current Opinion in Colloid & Interface Science 42 41
2019
-
[61]
236 04001
Combet S, Cousin F, Fadda G, Schirò G 2020 EPJ Web Conf. 236 04001
2020
-
[62]
Aswal D K, Sarkar P S, Kashyap Y S 2022 Neutron Imaging: Basics, Techniques and Applications (Springer)
2022
-
[63]
Strobl M, Manke I, Kardjilov N, Hilger A, Dawson M, Banhart J 2009 J. Phys. D: Appl. Phys. 42 243001
2009
-
[64]
Today 14 248
Kardjilov N, Manke I, Hilger A, Strobl M, Banhart J 2011 Mater. Today 14 248
2011
-
[65]
Luo W, Feng Y , Liu X Z, Wang M, Zhu D H, Gao W, Geng Y S, Ren Q Y , Shen J Y , Sun Y , Zhang X Y , Xia Y G, Zuo T S, Zheng Y , Tong X 2023 Nucl. Instrum. Methods Phys. Res., Sect. A 1046 167676
2023
-
[66]
Embs J P, Juranyi F, Hempelmann R 2010 Z. Phys. Chem. 224 5
2010
-
[67]
Bee M 1988 Quasielastic Neutron Scattering : Principles and Applications in Solid State Chemistry, Biology, and Materials Science (Bristol, England; Philadelphia: Adam Hilger)
1988
-
[68]
Ren Q Y , Qi J, Yu D H, Zhang Z, Song R Q, Song W L, Yuan B, Wang T H, Ren W J, Zhang Z D, Tong X, Li B 2022 Nat. Commun. 13 2293
2022
-
[69]
Jobic H, Theodorou D N 2007 Microporous Mesoporous Mater. 102 21
2007
-
[70]
Alloys Compd
Verdal N, Udovic T J, Rush J J, Skripov A V 2015 J. Alloys Compd. 645 S513
2015
-
[71]
Merklein M, Kabakova I V , Zarifi A, Eggleton B J 2022 Appl. Phys. Rev. 9 041306
2022
-
[72]
Wolff C, Smith M J A, Stiller B, Poulton C G 2021 J. Opt. Soc. Am. B 38 1243
2021
-
[73]
Baron A Q 2015 arXiv: 1504.01098 [cond-mat.mtrl-sci]
2015 arXiv
-
[74]
Synchrotron
Ishikawa D, Ellis D S, Uchiyama H, Baron A Q 2015 J. Synchrotron. Radiat. 22 3
2015
-
[75]
Wu M, Shi R C, Qi R S, Li Y H, Du J L, Gao P 2023 Ultramicroscopy 253 113818
2023
-
[76]
Delaire O, May A F, McGuire M A, Porter W D, Lucas M S, Stone M B, Abernathy D L, Ravi V A, Firdosy S A, Snyder G J 2009 Phys. Rev. B 80 184302
2009
-
[77]
Shi X, He J 2021 Science 371 343
2021
-
[78]
Mao J, Chen G, Ren Z F 2021 Nat. Mater. 20 454
2021
-
[79]
Toberer E S, Zevalkink A, Snyder G J 2011 J. Mater. Chem. 21 15843
2011
-
[80]
Wei P C, Liao C N, Wu H J, Yang D, He J, Biesold-McGee G V , Liang S, Yen W T, Tang X, Yeh J W, Lin Z, He J H 2020 Adv. Mater. 32 e1906457
2020
-
[81]
Hanus R, Agne M T, Rettie A J E, Chen Z W, Tan G, Chung D Y , Kanatzidis M G, Pei Y Z, V oorhees P W, Snyder G J 2019 Adv. Mater. 31 1900108
2019
-
[82]
Wu Y X, Chen Z W, Nan P F, Xiong F, Lin S Q, Zhang X Y , Chen Y , Chen L D, Ge B H, Pei Y Z 2019 Joule 3 1276
2019
-
[83]
Jiang B B, Yu Y , Cui J, Liu X X, Xie L, Liao J C, Zhang Q H, Huang Y , Ning S C, Jia B H, Zhu B, Bai S Q, Chen L D, Pennycook S J, He J Q 2021 Science 371 830
2021
-
[84]
Zhang Z X, Zhao K P, Wei T R, Qiu P F, Chen L D, Shi X 2020 Energy Environ. Sci. 13 3307
2020
-
[85]
Zhao K P, Qiu P F, Shi X, Chen L D 2019 Adv. Funct. Mater. 30 1903867
2019
-
[86]
Niedziela J L, Bansal D, May A F, Ding J, Lanigan-Atkins T, Ehlers G, Abernathy D L, Said A, Delaire O 2019 Nat. Phys. 15 73
2019
-
[87]
Jiang B B, Qiu P F, Eikeland E, Chen H Y , Song Q F, Ren D D, Zhang T S, Yang J, Iversen B B, Shi X, Chen L D 2017 J. Mater. Chem. C 5 943
2017
-
[88]
Ding J, Niedziela J L, Bansal D, Wang J L, He X, May A F, Ehlers G, Abernathy D L, Said A, Alatas A, Ren Y , Arya G, Delaire O 2020 Proc. Natl. Acad. Sci. U. S. A. 117 3930
2020
-
[89]
Xie L, Feng J H, Li R, He J Q 2020 Phys. Rev. Lett. 125 245901
2020
-
[90]
Trachenko K 2008 Phys. Rev. B 78 104201
2008
-
[91]
Xie L, Wu D, Yang H L, Yu Y , Wang Y F, He J Q 2019 J. Mater. Chem. C 7 9263
2019
-
[92]
Li W, Lin S Q, Ge B H, Yang J, Zhang W Q, Pei Y Z 2016 Adv. Sci. 3 1600196
2016
-
[93]
de Boissieu M 2023 Nat. Mater. 22 931
2023
-
[94]
Energy 1 16141
Janek J, Zeier W G 2016 Nat. Energy 1 16141
2016
-
[95]
Zhao Q, Stalin S, Zhao C Z, Archer L A 2020 Nat. Rev. Mater. 5 229
2020
-
[96]
He X F, Zhu Y Z, Mo Y F 2017 Nat. Commun. 8 15893
2017
-
[97]
Zou Z Y , Li Y J, Lu Z H, Wang D, Cui Y H, Guo B K, Li Y J, Liang X M, Feng J W, Li H, Nan C W, Armand M, Chen L Q, Xu K, Shi S Q 2020 Chem. Rev. 120 4169
2020
-
[98]
Zhu L, Wang Y W, Chen J C, Li W L, Wang T T, Wu J, Han S Y , Xia Y H, Wu Y M, Wu M Q, Wang F W, Zheng Y , Peng L M, Liu J J, Chen L Q, Tang W P 2022 Sci. Adv. 8 eabj7698
2022
-
[99]
Wang Y , Richards W D, Ong S P, Miara L J, Kim J C, Mo Y , Ceder G 2015 Nat. Mater. 14 1026
2015
-
[100]
Kraft M A, Culver S P, Calderon M, Böcher F, Krauskopf T, Senyshyn A, Dietrich C, Zevalkink A, Janek J, Zeier W G 2017 J. Am. Chem. Soc. 139 10909
2017
-
[101]
Zhang Z, Nazar L F 2022 Nat. Rev. Mater. 7 389
2022
-
[102]
Energy Mater
Muy S, Schlem R, Shao-Horn Y , Zeier W G 2021 Adv. Energy Mater. 11 2002787
2021
-
[103]
The Royal Society 2021 https://royalsociety.org/topics
2021
-
[104]
United Nations Environmental Programme https://ozone.unep.org/ites/default/files/2019 [2018-5]
2019
-
[105]
https://www.birmingham.ac.uk/Documents/college
Peters T 2018 Technical Report. https://www.birmingham.ac.uk/Documents/college
2018
-
[106]
Hou H, Qian S, Takeuchi I 2022 Nat. Rev. Mater. 7 633
2022
-
[107]
Chen Y L, Wang Y , Sun W, Qian S X, Liu J 2022 The Innovation 3 100205
2022
-
[108]
Aprea C, Greco A, Maiorino A, Masselli C 2019 Climate 7 115
2019
-
[109]
Maier L M, Corhan P, Barcza A, Vieyra H A, V ogel C, Koenig J D, Schäfer-Welsen O, Wöllenstein J, Bartholomé K 2020 Commun. Phys. 3 186
2020
-
[110]
Aprea C, Greco A, Maiorino A, Masselli C 2020 Energy 190 116404
2020
-
[111]
Lloveras P, Zhang Z, Zeng M, Barrio M, Kawakita Y , Yu D, Lin S Q, Li K, Moya X, Tamarit J L, Li B 2023 Colossal Barocaloric Plastic Crystals (IOP Publishing) p7-1-7-30
2023
-
[112]
Zhang K, Zhang Z, Pan H L, Wang H Y , Zhao X T, Qi J, Zhang Z, Song R Q, Yu C Y , Huang B H, Li X J, Chen H C, Yin W, Tan C L, Hu W J, Wübbenhorst M, Luo J S, Yu D H, Zhang Z D, Li B 2024 The Innovation 5 100577
2024
-
[113]
Li B, Zhang Z D 2021 Sci. Sin. Phys. Mech. Astron. 51 067505
2021
-
[114]
Qian X, Han D, Zheng L, Chen J, Tyagi M, Li Q, Du F, Zheng S, Huang X, Zhang S, Shi J, Huang H, Shi X, Chen J, Qin H, Bernholc J, Chen X, Chen L Q, Hong L, Zhang Q M 2021 Nature 600 664
2021
-
[115]
Sin.: Phys
Hao J Z, Hu F X, Wei Z B, Shen F R, Zhou H B, Gao Y H, Qiao K M, Liang W H, Zhang C, Wang J, Sun J R, Shen B G 2021 Sci. Sin.: Phys. Mech. Astron. 51 067520
2021
-
[116]
Aznar A, Lloveras P, Barrio M, Negrier P, Planes A, Manosa L, Mathur N D, Moya X, Tamarit J L 2020 J. Mater. Chem. A 8 639
2020
-
[117]
Li J, Dunstan D, Lou X, Planes A, Manosa L, Barrio M, Tamarit J L, Lloveras P 2020 J. Mater. Chem. A 8 20354
2020
-
[118]
Li F B, Li M, Xu X, Yang Z C, Xu H, Jia C K, Li K, He J, Li B, Wang H 2020 Nat. Commun. 11 4190
2020
-
[119]
Lloveras P, Aznar A, Barrio M, Negrier P, Popescu C, Planes A, Manosa L, Stern-Taulats E, Avramenko A, Mathur N D, Moya X, Tamarit J L 2019 Nat. Commun. 10 1803
2019
-
[120]
Zhang Z, Li K, Lin S Q, Song R, Yu D, Wang Y , Wang J L, Kawaguchi S, Zhang Z, Yu C, Li X, Chen J, He L, Mole R, Yuan B, Ren Q Y , Qian K, Cai Z, Yu J, Wang M, Zhao C, Tong X, Zhang Z, Li B 2023 Sci. Adv. 9 eadd0374
2023
-
[121]
Staveley L A K 1962 Annu. Rev. Phys. Chem. 13 351
1962
-
[122]
Seo J, Ukani R, Zheng J, Braun J D, Wang S, Chen F E, Kim H K, Zhang S, Thai C, McGillicuddy R D, Yan H, Vlassak J J, Mason J A 2024 J. Am. Chem. Soc. 146 2736
2024
-
[123]
Yu Z B, Zhou H B, Hu F X, Liu C, Yuan S K, Wang D H, Hao J Z, Gao Y H, Wang Y X, Wang B J, Tian Z Y , Lin Y , Zhang C, Yin Z, Wang J, Chen Y Z, Li Y L, Sun J R, Zhao T Y , Shen B G 2022 NPG Asia Mater. 14 96
2022
-
[124]
Sakata M, Harada J, Cooper M J, Rouse K D 1980 Acta Crystallogr. Sec. A 36 7
1980
-
[125]
Songvilay M, Giles-Donovan N, Bari M, Ye Z G, Minns J L, Green M A, Xu G, Gehring P M, Schmalzl K, Ratcliff W D, Brown C M, Chernyshov D, van Beek W, Cochran S, Stock C 2019 Phys. Rev. Mater. 3 093602
2019
-
[126]
Lee W, Li H, Wong A B, Zhang D, Lai M, Yu Y , Kong Q, Lin E, Urban J J, Grossman J C, Yang P 2017 Proc. Natl. Acad. Sci. U. S. A. 114 8693
2017
-
[127]
Li W, Vasenko A S, Tang J, Prezhdo O V 2019 J. Phys. Chem. Lett. 10 6219
2019
-
[128]
Ren Q Y , Fu C G, Qiu Q Y , Dai S N, Liu Z Y , Masuda T, Asai S, Hagihala M, Lee S, Torri S, Kamiyama T, He L H, Tong X, Felser C, Singh D J, Zhu T J, Yang J, Ma J 2020 Nat. Commun. 11 3142
2020
-
[129]
de Campos A, Rocco D L, Carvalho A M, Caron L, Coelho A A, Gama S, da Silva L M, Gandra F C, dos Santos A O, Cardoso L P, von Ranke P J, de Oliveira N A 2006 Nat. Mater. 5 802
2006
-
[130]
Krenke T, Duman E, Acet M, Wassermann E F, Moya X, Manosa L, Planes A 2005 Nat. Mater. 4 450
2005
-
[131]
Liu J, Gottschall T, Skokov K P, Moore J D, Gutfleisch O 2012 Nat. Mater. 11 620
2012
-
[132]
Choe W, Pecharsky V K, Pecharsky A O, Gschneidner Jr K A, Young Jr V G, Miller G J 2000 Phys. Rev. Lett. 84 4617
2000
-
[133]
Ren Q Y , Hutchison W D, Wang J L, Cobas R, Cadogan J M, Campbell S J 2015 Hyperfine Interactions 231 75
2015
-
[134]
Alloys Compd
Ren Q Y , Hutchison W D, Wang J L, Studer A J, Campbell S J 2017 J. Alloys Compd. 693 32
2017
-
[135]
Ren Q Y , Hutchison W D, Wang J L, Studer A J, Din M F M, Pérez S M, Cadogan J M, Campbell S J 2016 J. Phys. D: Appl. Phys. 49 175003
2016
-
[136]
Status Solidi A 211 1101
Ren Q Y , Hutchison W D, Wang J L, Muñoz Pérez S, Cadogan J M, Campbell S J 2014 Phys. Status Solidi A 211 1101
2014
-
[137]
Liu E K, Wang W H, Feng L, Zhu W, Li G J, Chen J L, Zhang H W, Wu G H, Jiang C B, Xu H B, de Boer F 2012 Nat. Commun. 3 873
2012
-
[138]
Ren Q Y , Hutchison W, Wang J L, Studer A, Wang G, Zhou H B, Ma J, Campbell S J 2019 ACS Appl. Mater. Interfaces 11 17531
2019
-
[139]
Ren Q Y , Hutchison W D, Wang J L, Studer A J, Campbell S J 2018 Chem. Mater. 30 1324
2018
-
[140]
Landrum G A, Hoffmann R, Evers J, Boysen H 1998 Inorg. Chem. 37 5754
1998
-
[141]
Zhu Y F, Xia Y , Wang Y C, Sheng Y , Yang J, Fu C G, Li A R, Zhu T J, Luo J, Wolverton C, Snyder G J, Liu J J, Zhang W Q 2020 Research 2020 4589786
2020
-
[142]
Today 48 198
Lin S Q, Li W, Pei Y Z 2021 Mater. Today 48 198
2021
-
[143]
Wang Y X, Lin R X, Zhu P C, Zheng Q H, Wang Q J, Li D Y , Zhu J 2018 Nano Lett. 18 2772
2018
-
[144]
Energy Mater
Bernges T, Hanus R, Wankmiller B, Imasato K, Lin S Q, Ghidiu M, Gerlitz M, Peterlechner M, Graham S, Hautier G, Pei Y Z, Hansen M R, Wilde G, Snyder G J, George J, Agne M T, Zeier W G 2022 Adv. Energy Mater. 12 2200717
2022
-
[145]
Luo Y X, Yang X L, Feng T L, Wang J Y , Ruan X L 2020 Nat. Commun. 11 2554
2020
-
[146]
Simoncelli M, Marzari N, Mauri F 2019 Nat. Phys. 15 809
2019
-
[147]
Mukhopadhyay S, Parker D S, Sales B C, Puretzky A A, McGuire M A, Lindsay L 2018 Science 360 1455
2018
Reviewed August 15, 2026 · model on record in the stance chip above.
Discussion (0). Continue with ORCID to comment.