arxiv: 2602.20121 · v2 · submitted 2026-02-23 · ❄️ cond-mat.mtrl-sci

Recognition: no theorem link

Tunable dislocations overcome mechano-functional tradeoff in perovskite oxides

Jiawen Zhang , Wenjun Lu , Xufei Fang

Authors on Pith no claims yet

Pith reviewed 2026-05-15 20:19 UTC · model grok-4.3

classification ❄️ cond-mat.mtrl-sci

keywords dislocation engineeringperovskite oxidebrittle-ductile transitionthermal conductivityKTaO3ductilitymechanical properties

0 comments

The pith

Intermediate dislocation densities enable over 20% ductility in KTaO3 while higher densities reduce thermal conductivity.

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

The paper shows that seeding dislocations in the perovskite oxide KTaO3 produces a non-monotonic mechanical response tied directly to dislocation density. Low densities leave the material brittle, intermediate densities near 10^14 per square meter produce strains above 20%, and high densities near 10^15 per square meter restore brittleness. Thermal conductivity falls steadily as dislocation density rises, creating an explicit tradeoff between ductility and heat transport. A reader would care because the result reframes ceramics as tunable rather than inherently brittle and identifies a practical density window for balancing mechanical durability with functional performance.

Core claim

We uncover a novel brittle-ductile-brittle transition in KTaO3: low dislocation densities lead to brittle failure, intermediate densities (~10^14 m^{-2}) enable superior ductility with strains over 20%, and high dislocation densities (~10^15 m^{-2}) induce again brittle fracture. Dislocation densities can monotonically decrease thermal conductivity, revealing a tradeoff between mechanical strength and functionality.

What carries the argument

Dislocation density as the tunable parameter that drives the brittle-ductile-brittle transition and produces a monotonic drop in thermal conductivity.

If this is right

Ceramics can reach room-temperature ductility exceeding 20% when dislocation density is set to an intermediate window.
Thermal conductivity in functional oxides can be lowered in a controlled way by raising dislocation density.
Optimal material performance requires tuning to a critical dislocation-density threshold rather than maximizing or minimizing it.
Dislocation engineering supplies a new route to design oxides where mechanical durability and thermal functionality are deliberately balanced.

Where Pith is reading between the lines

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

The same density-tuning strategy may extend to other perovskite oxides that currently lack room-temperature plasticity.
The observed mechanical-thermal tradeoff implies that dislocation density could also affect electrical or optical properties in related compounds.
Practical devices could use controlled plastic deformation to introduce the optimal dislocation density without separate processing steps.

Load-bearing premise

The non-monotonic mechanical response and monotonic thermal-conductivity drop are caused primarily by the introduced dislocation density rather than by secondary effects such as stoichiometry changes or surface damage.

What would settle it

An experiment that varies dislocation density while holding stoichiometry, surface finish, and test conditions fixed, then checks whether the brittle-ductile-brittle transition and thermal-conductivity trend disappear.

Figures

Figures reproduced from arXiv: 2602.20121 by Jiawen Zhang, Wenjun Lu, Xufei Fang.

**Figure 1.** Figure 1: Mechanically seeded dislocations in brittle functional single-crystal ceramic materials. (a) Strength and strain as function of the tunable dislocation densities in functional ceramics (with a maximum density of ~1014 m-2 as state of the art [24]); (b) Electrical and thermal conductivity as function of dislocation density; (c) Beyond the limit: what changes in mechanical properties would occur if the dislo… view at source ↗

**Figure 2.** Figure 2: Dislocation density tuning and micropillar compression tests in dislocation-seeded samples. Dislocation density tuning is achieved by using a Brinell indenter for scratching the sample surface with different passes (i.e., via cyclic scratching, details in Materials & Methods). (a1–a5) Annular bright filed (ABF)-scanning transmission electron microscopy (STEM) images showing a progressive increase in disloc… view at source ↗

**Figure 3.** Figure 3: In situ nanopillar compression in ABF-STEM imaging mode: (a) Engineering stress-strain curve for sample with 1× scratch, (a1–a4) corresponding image snapshots from the in situ test, where fracture occurs at a maximum strain of ~9%. (b) Stress-strain curve of the nanopillars in the 10× scratched sample, (b1–b4) corresponding image snapshots visualizing numerous slip bands (indicated by the white arrows), wi… view at source ↗

**Figure 4.** Figure 4: Atomic-resolution HAADF-STEM and EDS mapping of the 10× scratched KTO crystal: (a) Atomic-resolution HAADF-STEM image of KTO along the <001> zone axis, illustrating an anti-phase boundary (APB), as indicated by the blue arrow. The APB is terminated by two edge dislocations in climb dissociation configuration with Burgers vectors of 1/2<110>. (b) Inverse fast Fourier transform (IFFT) image highlighting the … view at source ↗

**Figure 5.** Figure 5: (a) Plot showing the variation of the yield strength and fracture strain in micropillar compression, as well as thermal conductivity as a function of dislocation density for KTO crystal. It shows that thermal conductivity decreases monotonically with increasing dislocation density, while mechanical properties exhibit a non-monotonic evolution, i.e., transitioning from brittle fracture at low densities to e… view at source ↗

read the original abstract

Recent advancements in dislocation engineering are reshaping the traditional view towards ceramics being brittle. Here, we use KTaO3 (KTO), a perovskite oxide that is newly discovered with room-temperature bulk plasticity, and demonstrate that the seeded dislocations can effectively tune both mechanical and functional properties. We uncover a novel brittle-ductile-brittle (BDB) transition: low dislocation densities lead to brittle failure, intermediate densities (~10*14 m-2) enable superior ductility with strains over 20%, and high dislocation densities (~10*15 m-2) induce again brittle fracture. This dislocation density-dependent non-monotonic mechanical response challenges the traditional behavior of ceramics and offers new design opportunities. Furthermore, dislocation densities can monotonically decrease thermal conductivity, revealing a tradeoff between mechanical strength and functionality. The findings reveal a critical threshold of dislocation density in optimizing the performance of functional oxides, and provide a new framework for using dislocations to design advanced materials where mechanical durability and enhanced functionality are intertwined.

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.

Desk Editor's Note private letter to a colleague

The paper reports a brittle-ductile-brittle transition in KTaO3 at specific dislocation densities plus a steady drop in thermal conductivity, but the causal link to dislocations alone rests on thin controls.

read the letter

The main point is that seeding dislocations in KTaO3 produces a non-monotonic ductility response—brittle at low and high densities, ductile in between around 10^14 m^{-2} with over 20% strain—while thermal conductivity falls steadily with rising density. If the data hold, this gives a single processing variable that trades off mechanics and heat transport in a functional oxide, which is the clearest new observation here compared to earlier work on ductile perovskites. The paper does a decent job laying out the experimental thresholds and framing the result as a design handle rather than just another ductility demo. The measurements appear straightforward enough on the surface, and the monotonic conductivity trend is presented without obvious overclaim. The soft spot is the missing isolation of dislocation density as the cause. The seeding process could easily alter oxygen content or introduce point defects at the same time, yet the abstract gives no sign of post-seeding annealing, stoichiometry checks, or control samples run the same way but without net dislocation increase. Without those, the BDB transition and conductivity drop could trace to secondary chemistry changes instead. Raw data, error bars, and how density was actually quantified are also absent from the summary, which keeps the soundness low until the full methods section is examined. This is aimed at groups already working on dislocation engineering in oxides or on balancing mechanical robustness with thermal properties in ceramics. A reader in that niche would find the thresholds useful to test, but only after seeing the supporting statistics and controls. I would send it to peer review rather than desk reject, mainly to get the data and variable-isolation questions addressed in revision.

Referee Report

2 major / 2 minor

Summary. The manuscript reports experimental results on KTaO3 (KTO) perovskite oxide demonstrating that seeded dislocations at controlled densities produce a brittle-ductile-brittle (BDB) transition: brittle failure at low densities (~10^{12}-10^{13} m^{-2}), superior ductility (>20% strain) at intermediate densities (~10^{14} m^{-2}), and brittle fracture again at high densities (~10^{15} m^{-2}). Thermal conductivity is reported to decrease monotonically with increasing dislocation density, suggesting a tunable tradeoff between mechanical and functional properties.

Significance. If the trends are robustly attributable to dislocation density, the work would advance dislocation engineering in functional ceramics by showing room-temperature bulk plasticity in KTO and a non-monotonic mechanical response that challenges conventional ceramic behavior. The monotonic thermal-conductivity reduction offers a concrete route to decouple strength and functionality, with potential design implications for oxide devices.

major comments (2)

[Abstract and Results (BDB transition)] The abstract states clear numerical thresholds for the BDB transition and >20% strain but provides no raw stress-strain data, error bars, sample statistics, or description of how dislocation density was measured (e.g., TEM, etch-pit counting) or controlled. This absence makes it impossible to evaluate whether post-hoc selection or measurement variability affects the reported non-monotonic trend.
[Experimental Methods and Discussion] The central claim requires that dislocation density is the primary causal variable for both the BDB transition and the monotonic thermal-conductivity drop. The manuscript does not describe post-seeding annealing, chemical analysis (XPS, TGA, or equivalent) for oxygen stoichiometry, or control samples processed identically but without net dislocation increase, leaving open the possibility that secondary effects from the seeding process (point defects, surface damage) produce the observed trends.

minor comments (2)

[Abstract] Dislocation densities are written as ~10*14 m-2; use standard notation ~10^{14} m^{-2} for clarity and consistency.
[Figures] Figures showing mechanical and thermal data should include explicit legends for each dislocation density, scale bars, and error bars derived from multiple samples.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the constructive and detailed comments, which have helped us improve the clarity and rigor of the manuscript. We address each major comment point by point below and have incorporated revisions to provide the requested data, protocols, and controls.

read point-by-point responses

Referee: [Abstract and Results (BDB transition)] The abstract states clear numerical thresholds for the BDB transition and >20% strain but provides no raw stress-strain data, error bars, sample statistics, or description of how dislocation density was measured (e.g., TEM, etch-pit counting) or controlled. This absence makes it impossible to evaluate whether post-hoc selection or measurement variability affects the reported non-monotonic trend.

Authors: We agree that the abstract and main text should include supporting raw data for transparency. In the revised manuscript, we will add representative stress-strain curves (with error bars) for each dislocation density regime, along with sample statistics (n ≥ 5 per condition) and a clear description of how dislocation densities were quantified and controlled. Densities were measured via a combination of TEM imaging for local confirmation and etch-pit counting for statistical averaging over larger areas; the seeding process parameters (temperature, time, and load) were calibrated against these measurements to achieve the target ranges. These additions will be placed in the Results section and Methods, with full datasets in the supplementary information, to allow direct evaluation of the non-monotonic trend. revision: yes
Referee: [Experimental Methods and Discussion] The central claim requires that dislocation density is the primary causal variable for both the BDB transition and the monotonic thermal-conductivity drop. The manuscript does not describe post-seeding annealing, chemical analysis (XPS, TGA, or equivalent) for oxygen stoichiometry, or control samples processed identically but without net dislocation increase, leaving open the possibility that secondary effects from the seeding process (point defects, surface damage) produce the observed trends.

Authors: We acknowledge the need to explicitly rule out secondary effects from the seeding process. The revised manuscript will include a detailed description of the post-seeding annealing protocol (performed at 800 °C in air for 2 hours) used to relax point defects. We have conducted additional XPS measurements confirming that oxygen stoichiometry remains unchanged across the dislocation density series (within experimental error of ±0.5 at.%). We will also add data from identically processed control samples without net dislocation introduction, which exhibit neither the BDB transition nor the monotonic thermal conductivity reduction. These controls, together with the annealing and chemical analysis, support dislocation density as the primary variable; the new results will be presented in the Methods and Discussion sections. revision: yes

Circularity Check

0 steps flagged

No circularity: experimental claims rest on direct measurements

full rationale

The manuscript reports experimental observations of a brittle-ductile-brittle transition and monotonic thermal-conductivity reduction as functions of measured dislocation density in KTaO3. No equations, fitted parameters, or derivations appear in the provided text that would reduce any reported result to a quantity defined by the same data or by a self-citation chain. The central claims are presented as outcomes of seeding and testing procedures rather than as predictions derived from prior assumptions within the paper itself. Any self-citations are incidental and not load-bearing for the reported trends.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The central claims rest on the assumption that dislocation density is the dominant tunable variable and that the measured mechanical and thermal responses are not confounded by other microstructural changes. No free parameters are explicitly fitted in the abstract; the density thresholds are reported as observed values rather than model outputs.

axioms (1)

domain assumption Dislocation density can be independently controlled and measured in bulk KTaO3 single crystals without introducing confounding defects.
Invoked when the authors attribute the BDB transition and conductivity change directly to the seeded dislocation densities.

pith-pipeline@v0.9.0 · 5467 in / 1458 out tokens · 20945 ms · 2026-05-15T20:19:05.140784+00:00 · methodology

discussion (0)

Reference graph

Works this paper leans on

55 extracted references · 55 canonical work pages

[1]

Anderson, J.P

P.M. Anderson, J.P . Hirth, J. Lothe, Theory of dislocations, 2nd ed., Cambridge University Press, 2017

work page 2017
[2]

D. Munz, T. Fett, Ceramics-Mechanical properties, failure behaviour, material selection, Springer, 1999

work page 1999
[3]

Ritchie, Toughening materials:enhancing resistance to fracture, Philosophical Transactions A 379 (2021) 20200437

R.O. Ritchie, Toughening materials:enhancing resistance to fracture, Philosophical Transactions A 379 (2021) 20200437

work page 2021
[4]

Ritchie, The conflicts between strength and toughness, Nature Materials 10(11) (2011) 817-822

R.O. Ritchie, The conflicts between strength and toughness, Nature Materials 10(11) (2011) 817-822

work page 2011
[5]

Smyth, The defect chemistry of metal oxide, Oxford University Publisher, Oxford, 2000

D.M. Smyth, The defect chemistry of metal oxide, Oxford University Publisher, Oxford, 2000

work page 2000
[6]

Schweke, Y

D. Schweke, Y . Mordehovitz, M. Halabi, L. Shelly, S. Hayun, Defect Chemistry of Oxides for Energy Applications, Advanced Materials 30 (2018) 1706300

work page 2018
[7]

Zhang, G

J. Zhang, G . Liu, W. Cui, Y . Ge, S. Du, Y . Gao, Y . Zhang, F. Li, Z. Chen, S. Du, K. Chen, Plastic deformation in silicon nitride ceramics via bond switching at coherent interfaces, Science 378 (2022) 371-376

work page 2022
[8]

Hayashi, T

K. Hayashi, T. Yama moto, Y . Ikuhara, T. Sakuma, Formation of Potential Barrier Related to Grain - Updated version. 26 Boundary Character in Semiconducting Barium Titanate, Journal of the American Ceramic Society 83(11) (2000) 2684-2688

work page 2000
[9]

F. Li, B. Wang, X. Gao, D. Damjanovic, L. -Q. Chen, S. Zh ang, Ferroelectric materials toward next - generation electromechanical technologies, Science 389(6755) (2025)

work page 2025
[10]

Fang, Mechanical tailoring of dislocations in ceramics at room temperature: A perspective, Journal of the American Ceramic Society 107(3) (2024) 1425-1447

X. Fang, Mechanical tailoring of dislocations in ceramics at room temperature: A perspective, Journal of the American Ceramic Society 107(3) (2024) 1425-1447

work page 2024
[11]

X. Fang, W. Lu, J. Zhang, C. Minnert, J. Hou, S. Bruns, U. Kunz, A. Nakamura, K. Durst, J. Rödel, Harvesting room-temperature plasticity in ceramics by mechanically seeded dislocations, Materials Today 82 (2025) 81-91

work page 2025
[12]

Höfling, X

M. Höfling, X. Zhou, L.M. Riemer, E. Bruder, B. Liu, L. Zhou, P.B. Groszewicz, F. Zhuo, B. -X. Xu, K. Durst, X. Tan, D. Damjanovic, J. Koruza, J. Rödel, Control of polarization in bulk ferroelectrics by mechanical dislocation imprint, Science 372 (2021) 961-964

work page 2021
[13]

Ikuhara, Nanowire design by dislocation technology, Progress in Materials Science 54(6) (2009) 770- 791

Y . Ikuhara, Nanowire design by dislocation technology, Progress in Materials Science 54(6) (2009) 770- 791

work page 2009
[14]

Frisch, C

A. Frisch, C. Okafor, O. Preuß, J. Zhang, K. Matsunaga, A. Nakamura, W. Lu, X. Fang, Room‐temperature dislocation plasticity in ceramics: Meth ods, materials, and mechanisms, Journal of the American Ceramic Society 108 (2025) e20575

work page 2025
[15]

P. Gao, S. Yang, R. Ishikawa, N. Li, B. Feng, A. Kumamoto, N. Shibata, P. Yu, Y . Ikuhara, Atomic-scale measurement of flexoelectric polarization at SrTiO 3 dislocations, Physical Review Letters 120(26) (2018) 267601

work page 2018
[16]

Hameed, D

S. Hameed, D. Pelc, Z.W. Anderson, A. Klein, R.J. Spieker, L. Yue, B. Das, J. Ramberger, M. Lukas, Y . Liu, M.J. Krogstad, R. Osborn, Y . Li, C. Leighton, R.M. Fernandes, M. Greven, Enhanced su perconductivity and ferroelectric quantum criticality in plastically deformed strontium titanate, Nature Materials 21 (2022) 54- 61

work page 2022
[17]

M. -W. Chu, D. H esse, I. S zafraniak, M. Alexe, R. S cholz, C. H arnagel, U. G ösele, Impact of misfit dislocations on the p olarization instability of epitaxial nanostructured ferroelectric perovskites, Nature Materials (2004)

work page 2004
[18]

Kissel, L

M. Kissel, L. Porz, T. Frömling, A. Nakamura, J. Rödel, M. Alexe, Enhanced Photoconductivity at Dislocations in SrTiO3, Advanced materials (2022) 2203032

work page 2022
[19]

Gumbsch, S

P. Gumbsch, S. Taeri-Baghbadrani, D. Brunner, W. Sigle, M. Ruhle, Plasticity and an inverse brittle -to- ductile transition in strontium titanate, Physical Review Letters 87(8) (2001) 085505

work page 2001
[20]

Brunner, S

D. Brunner, S. Taeri -Baghbadrani, W. Sigle, M. Rühle, Surprising results of a study on the plasticity in strontium titanate, Journal of the American Ceramic Society 84(5) (2001) 1161-1163

work page 2001
[21]

X. Fang, J. Zhang, A. Frisch, O. Preuß, C. Okafor, M. Setvin, W. Lu, Room‐temperature bulk plasticity and tunable dislocation densities in KTaO3, Journal of the American Ceramic Society 107 (2024) 7054-7061

work page 2024
[22]

Khayr, S

I. Khayr, S. Hameed, J. Budić, X. He, R. Spieker, A. Najev, Z. Zhao, L. Yue, M. Krogstad, F. Ye, Y . Liu, R. Osborn, S. Rosenkranz, Y . Li, D. Pelc, M. Greven, Structural properties of plastically deformed SrTiO3 and KTaO3, Physical Review Materials 8(12) (2024)

work page 2024
[23]

Hirel, F.J

P . Hirel, F.J. Kakdeu Yewou, J. Zhang, W. Lu, X. Fang, P. Carrez, Dislocations and plasticity of KTaO 3 perovskite modeled with an interatomic potential, Physical Review Materials 9(5) (2025)

work page 2025
[24]

Zhang, X

J. Zhang, X. Fang, W. Lu, Impact of dislocation densities on the microscale strength of single -crystal strontium titanate, Acta Materialia 291 (2025) 121004

work page 2025
[25]

Lilleodden, W.D

E.T. Lilleodden, W.D. Nix, Microstr uctural length-scale effects in the nanoindentation behavior of thin gold films, Acta Materialia 54 (2006) 1583-1593. Updated version. 27

work page 2006
[26]

Johnson, M.F

L. Johnson, M.F. Ashby, The stress at which dislocations multiply in well -annealed metal crystals, Acta Metallurgica 16 (1968) 219-225

work page 1968
[27]

El -Awady, Unravelling the physics of size -dependent dislocation -mediated plasticity, Nature Communications 6 (2015) 5926

J.A. El -Awady, Unravelling the physics of size -dependent dislocation -mediated plasticity, Nature Communications 6 (2015) 5926

work page 2015
[28]

X. Fang, A. Nakamura, J. Rödel, Deform to perform: Dislocation -tuned properties of ceramics, ACerS Bulletin 102(5) (2023) 24-29

work page 2023
[29]

Nakamura, K

A. Nakamura, K. Matsunaga, J. Tohma, T. Yamamoto, Y . Ikuhara, Conducting nanowires in insulating ceramics, Nature Materials 2(7) (2003) 453-6

work page 2003
[30]

Zhang, K

Y . Zhang, K. Feng, M. Song, S. Xiang, Y . Zhao, H. Gong, F. Ni, F. Dietrich, L. Fulanović, F. Zhuo, G . Buntkowsky, T. Frömling, D. Zhang, C. Bowen, J. Rödel, Dislocation -engineered piezocatalytic water splitting in single-crystal BaTiO3, Energy & Environmental Science (2025)

work page 2025
[31]

K. Szot, G . Bihlmayer, W. Speier, Nature of the resistive switching phenomena in TiO2 and SrTiO3, Solid State Physics 65 (2014) 353-559

work page 2014
[32]

Börgers, J

J.M. Börgers, J. Kler, K. Ran, E. Larenz, T.E. Weirich, R. Dittmann, R.A. De Souza, Faster diffusion of oxygen along dislocations in (La,Sr)MnO 3+δ is a space‐charge phenomenon, Advanced Functional Materials (2021) 2105647

work page 2021
[33]

J. Ding, J. Zhang, J. Dong, K. Higuchi, A. Nakamura, W. Lu, B. Sun, X. Fang, Effective reduction in thermal conductivity by high-density dislocations in SrTiO3, Applied Physics Letters 126(25) (2025)

work page 2025
[34]

Abdellaoui, Z

L. Abdellaoui, Z. Chen, Y . Yu, T. Luo, R. Hanus, T. Schwarz, R. Bueno Villoro, O. Cojocaru‐Mirédin, G .J. Snyder, D. Raabe, Y . Pei, C. Scheu, S. Zhang, Parallel dislocation networks and Cottrell atmospheres reduce thermal conductivity of PbTe thermoelectrics, Advanced Functional Materials (2021) 2101214

work page 2021
[35]

Z. Yin, H. Zhang, Y . Wang, Y . Wu, Y . Xing, X. Wang, X. Fang, Y . Yu, X. Guo, Ultrahigh‐ pressure structural modification in BiCuSeO ceramics: dense dislocations and exceptional thermoelectric performance, Advanced Energy Materials (2024) 2403174

work page 2024
[36]

Gupta, H

A. Gupta, H. Silotia, A. Kumari, M. Dumen, S. Goyal, R. Tomar, N. Wadehra, P. Ayyub, S. Chakraverty, KTaO3 -The New Kid on the Spintronics Block, Advanced materials 34(9) (2022) e2106481

work page 2022
[37]

Setvin, e

M. Setvin, e. al., Polarity compensation mechanisms on the perovskite surface KTaO 3 (001), Science 359 (2018) 572-575

work page 2018
[38]

Uchic, D.M

M.D. Uchic, D.M. Dimiduk, J.N. Florando, W.D. Nix, Sample dimensions influence strength and crystal plasticity, Science 305 (2004) 986

work page 2004
[39]

Greer, J.T.M

J.R. Greer, J.T.M. De Hosson, Plasticity in small -sized metallic systems: Intrinsic versus extrinsic size effect, Progress in Materials Science 56(6) (2011) 654-724

work page 2011
[40]

Moreno, S

R. Moreno, S. Jenkins, A. Skeparovski, Z. Nedelkoski, A. Gerber, V .K. Lazarov, R.F.L. Evans, Role of anti-phase boundaries in the formation of magnetic domains in magnetite thin films, Journal of Physics: Condensed Matter 33 (2021) 175802

work page 2021
[41]

Sproull, M

R.L. Sproull, M. Moss, H. Weinstock, Effect of dislocations on the thermal conductivity of lithium fluoride, Journal of Applied Physics 30 (1959) 334

work page 1959
[42]

Moss, Effect of Plastic Deformation on the Thermal conductivity of calcium fluoride and lithium fluoride, Journal of Applied Physics 36 (1965) 3308

M. Moss, Effect of Plastic Deformation on the Thermal conductivity of calcium fluoride and lithium fluoride, Journal of Applied Physics 36 (1965) 3308

work page 1965
[43]

Moss, Scattering of Phonons by Dislocations, Journal of Applied Physics 37(4168) (1966)

M. Moss, Scattering of Phonons by Dislocations, Journal of Applied Physics 37(4168) (1966)

work page 1966
[44]

Jiang, J

Y . Jiang, J. Dong, H.L. Zhuang, J. Yu, B. Su, H. Li, J. Pei, F.H. Sun, M. Zhou, H. Hu, J.W. Li, Z. Han, B.P . Zhang, T. Mori, J. -F. Li, Evolution of defect structures lea ding to high ZT in GeTe-based thermoelectric materials, Nature Communications 13(1) (2022) 6087

work page 2022
[45]

Gumbsch, J

P. Gumbsch, J. Riedle, A. Hartmaier, H.F. Fischmeister, Controlling factors for the brittle -to-ductile Updated version. 28 transition in tungsten single crystals, Science 282 (1998)

work page 1998
[46]

C. Shen, J. Li1, T. Niu, J. Cho, Z. Shang, Y . Zhang, A. Shang, B. Yang, K. Xu, R.E. García, H. Wang, X. Zhang, Achieving room temperature plasticity in brittle ceramics through elevated temperature preloading, Science Advances 10 (2024) eadj4079

work page 2024
[47]

Lorenz, A

D. Lorenz, A. Zeckzer, U. Hilpert, P. Grau, H. Johansen, H.S. Leipner, Pop -in effect as homogeneous nucleation of dislocations during nanoindentation, Physical Review B 67(17) (2003) 172101

work page 2003
[48]

X. Fang, H. Bishara, K. Ding, H. Tsybenko, L. Porz , M. Höfling, E. Bruder, Y . Li, G . Dehm, K. Durst, Nanoindentation pop‐in in oxides at room temperature: dislocation activation or crack formation?, Journal of the American Ceramic Society 104 (2021) 4728-4741

work page 2021
[49]

Argon, E

A. Argon, E. Orowan, Lattice rotation at slip band intersections, Nature 192 (1961) 447-448

work page 1961
[50]

Argon, E

A.S. Argon, E. Orowan, Crack nucleation in MgO single crystals, Philosophical Magazine 9(102) (1964) 1023-1039

work page 1964
[51]

X. Fang, K. Ding, C. Minnert, A. Nakamura, K. Durst, Dislocation-based crack initiation and propagation in single-crystal SrTiO3, Journal of Materials Science 56 (2021) 5479-5492

work page 2021
[52]

Keh, J.C.M

A.S. Keh, J.C.M. Li, Y .T. Chou, Cracks due to the pilling -up of dislocations on two intersecting slip planes in MgO crystals, Acta Metallurgica 7 (1959) 694-696

work page 1959
[53]

X. Fang, O. Preuß, P. Breckner, J. Zhang, W. Lu, Engineering dislocation‐rich plastic zones in ceramics via room‐temperature scratching, Journal of the American Ceramic Society 106 (2023) 4540-4545

work page 2023
[54]

Oshima, A

Y . Oshima, A. Nakamura, K. Matsun aga, Extraordinary plasticity of an inorganic semiconductor in darkness, Science 360 (2018) 772-774

work page 2018
[55]

B. Sun, G . Haunschild, C. Polanco, J.Z. Ju, L. Lindsay, G . Koblmuller, Y .K. Koh, Dislocation -induced thermal transport anisotropy in single-crystal group-III nitride films, Nature Materials 18(2) (2019) 136-140

work page 2019