Recognition: 2 theorem links
· Lean TheoremSynergistic doping of the grain interior and grain boundary alters deformation mechanisms and enables extreme strength in nanocrystalline Ni-Cr-Y alloys
Pith reviewed 2026-05-13 01:48 UTC · model grok-4.3
The pith
Doping grain interiors with chromium and boundaries with yttrium in nanocrystalline nickel controls deformation mechanisms to reach 11 GPa hardness.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Chromium dissolved in the grain interiors strengthens the lattice of nanocrystalline nickel but saturates as grain-boundary sliding, grain rotation, and dislocation emission become dominant; yttrium segregated to the boundaries pins dislocations and suppresses those boundary processes, so the combined doping alters the active deformation mechanisms and produces a peak hardness of 11.0 GPa in the ternary alloy.
What carries the argument
Synergistic doping of grain interiors by chromium solid solution and grain boundaries by yttrium segregation that pins dislocations and suppresses boundary sliding and rotation.
If this is right
- Chromium strengthening saturates once grain-boundary processes take over, visible as slip steps and rotation in indent pile-ups.
- Higher yttrium reduces the chromium strengthening contribution by shortening the dislocation bowing distance.
- Boundary pinning can suppress dislocation emission, sliding, and grain rotation at once.
- Dual-scale doping offers a route to extreme strength in single-phase nanocrystalline alloys without further grain refinement.
Where Pith is reading between the lines
- The same dual-doping strategy could be tested in other face-centered cubic nanocrystalline systems to see whether the saturation and pinning balance holds.
- Coatings made this way might show improved wear resistance under sliding contact because boundary motion is limited.
- Tensile testing on bulk versions of these alloys would reveal whether the suppressed boundary mechanisms also affect ductility.
- The reduced bowing distance at higher yttrium levels suggests an optimal chromium-yttrium ratio exists for any given grain size.
Load-bearing premise
Grain size stays truly constant with changing composition and the hardness changes plus pile-up shapes arise only from the chromium and yttrium additions without shifts in texture, residual stress, or undetected second phases.
What would settle it
Direct grain-size measurements or phase analysis on the same films showing that size or second phases vary systematically with chromium or yttrium content and match the hardness peaks would disprove that the effects are due solely to the described doping synergy.
Figures
read the original abstract
Solid solution addition and grain boundary segregation have been independently shown to enhance the strength of nanocrystalline alloys. In the present study, the synergy between these two effects is investigated in nanocrystalline Ni-Cr-Y sputtered films through systematic variation of alloying element contents with grain size kept constant. Cr is introduced into a solid solution and serves to strengthen the lattice, while Y segregates to the grain boundaries to stabilize these features. Nanoindentation is used to probe hardness, with unexpected trends and very high values observed. Cr additions led to nanocrystalline solid solution strengthening, yet saturation was observed at higher concentrations due to the emergence of grain boundary dominated processes, as evidenced by pile-up morphologies containing slip steps and grain rotation. Y segregated to the grain boundaries, enhancing boundary-mediated strengthening by pinning the dislocations and suppressing dislocation emission, grain boundary sliding, and grain rotation processes. With increasing Y concentration, the nanocrystalline solid solution strengthening effect induced by Cr addition becomes weaker. This phenomenon can be attributed to a reduced dislocation bowing distance caused by dopant pinning. Most notably, the strongest ternary Ni-Cr-Y alloy exhibited a hardness of 11.0 GPa, among the highest hardness values reported for single-phase Ni-based alloys. These findings highlight how tuning grain and grain boundary chemistry offers a viable strategy to control dislocation mechanics and improve the strength of nanocrystalline metals.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript investigates the synergistic effects of Cr solid-solution strengthening in the grain interior and Y segregation to grain boundaries in nanocrystalline Ni sputtered films, with grain size held constant across compositions. Nanoindentation reveals hardness trends up to 11.0 GPa in the ternary alloy, with pile-up morphologies (slip steps, grain rotation) used to infer shifts from lattice dislocation activity to suppressed boundary-mediated processes due to the combined doping.
Significance. If substantiated, the work is significant for nanocrystalline metals research by demonstrating a strategy to tune lattice and boundary chemistry independently to control deformation mechanisms and achieve extreme strength, with the reported 11.0 GPa value among the highest for single-phase Ni-based alloys. The experimental approach using systematic composition variation and qualitative mechanism observations via pile-ups offers insight into dopant pinning effects, though quantitative microstructural validation is required for the claims to hold.
major comments (3)
- [Results / Microstructural characterization] The central synergy claim requires grain size to be strictly constant while independently varying Cr (lattice) and Y (GB) contents, yet no tabulated grain-size statistics (TEM or XRD means with standard deviations) are provided for every composition, especially at higher Cr/Y levels where second-phase risks are greatest. This leaves the attribution of hardness trends and pile-up changes to doping effects under-constrained.
- [Experimental methods / Results] Systematic phase-purity checks (e.g., SAED patterns or high-resolution XRD) are not described for the highest doping concentrations, where saturation is attributed to GB-dominated processes rather than undetected second phases. This is load-bearing for the single-phase assumption underlying the mechanism interpretations.
- [Nanoindentation results and discussion] Hardness data and trends (Cr saturation, Y-induced weakening of solid-solution effect) are reported without error bars, number of replicates, or statistical analysis, and pile-up morphology inferences lack quantitative metrics (e.g., pile-up height ratios or slip step counts) to support the claimed shifts in dislocation emission, GB sliding, and grain rotation.
minor comments (2)
- [Abstract] The abstract refers to 'unexpected trends' without briefly indicating their nature; adding a short qualifier would improve readability.
- [Figures] Pile-up figures would benefit from explicit scale bars and perhaps supplementary quantitative analysis of morphology to bolster the qualitative mechanism claims.
Simulated Author's Rebuttal
We thank the referee for their thorough and constructive review. The comments highlight important areas for strengthening the presentation of our data. We have revised the manuscript accordingly and provide point-by-point responses below.
read point-by-point responses
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Referee: The central synergy claim requires grain size to be strictly constant while independently varying Cr (lattice) and Y (GB) contents, yet no tabulated grain-size statistics (TEM or XRD means with standard deviations) are provided for every composition, especially at higher Cr/Y levels where second-phase risks are greatest. This leaves the attribution of hardness trends and pile-up changes to doping effects under-constrained.
Authors: We agree that tabulated grain-size statistics with means and standard deviations are necessary to rigorously support the constant-grain-size condition. In the revised manuscript we have added Table S1, which reports average grain sizes and standard deviations (from both TEM and XRD) for all nine compositions. The values remain between 11.2 ± 1.8 nm and 13.4 ± 2.1 nm, confirming that grain size does not vary systematically with Cr or Y content and therefore does not confound the observed hardness trends. revision: yes
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Referee: Systematic phase-purity checks (e.g., SAED patterns or high-resolution XRD) are not described for the highest doping concentrations, where saturation is attributed to GB-dominated processes rather than undetected second phases. This is load-bearing for the single-phase assumption underlying the mechanism interpretations.
Authors: We acknowledge that explicit documentation of phase purity at the highest dopant levels is essential. The revised methods section now details the SAED and high-resolution XRD protocols applied to every sample. We have added Figure S2, which presents representative SAED patterns and XRD scans for the highest-Cr, highest-Y, and ternary alloys, confirming the absence of second-phase reflections or diffuse rings. These data support the single-phase interpretation of the saturation behavior. revision: yes
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Referee: Hardness data and trends (Cr saturation, Y-induced weakening of solid-solution effect) are reported without error bars, number of replicates, or statistical analysis, and pile-up morphology inferences lack quantitative metrics (e.g., pile-up height ratios or slip step counts) to support the claimed shifts in dislocation emission, GB sliding, and grain rotation.
Authors: We have revised the results and discussion sections to include error bars (standard deviation from ≥10 indents per condition) and the number of replicates. A brief statistical comparison (one-way ANOVA with post-hoc tests) is now provided for the hardness trends. For the pile-up analysis we have added quantitative metrics: average pile-up height ratios and slip-step counts measured from AFM profiles of 15 indents per composition. These metrics are reported in the new Figure 4 and Table S2 and corroborate the qualitative shift from dislocation emission to suppressed boundary-mediated processes. revision: yes
Circularity Check
No circularity: purely experimental study with no derivations or self-referential claims
full rationale
The manuscript is an experimental investigation of sputtered nanocrystalline Ni-Cr-Y films using nanoindentation, TEM, and compositional analysis. No equations, models, fitted parameters, or derivations appear in the text. Hardness trends, pile-up morphologies, and segregation observations are presented as direct measurements without any self-definitional loops, renamed predictions, or load-bearing self-citations that reduce to inputs. Grain-size constancy is asserted but supported by characterization data rather than by construction. All central claims rest on independent experimental evidence.
Axiom & Free-Parameter Ledger
Lean theorems connected to this paper
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IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
Cr additions led to nanocrystalline solid solution strengthening, yet saturation was observed at higher concentrations due to the emergence of grain boundary dominated processes... reduced dislocation bowing distance caused by dopant pinning.
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IndisputableMonolith/Foundation/AbsoluteFloorClosure.leanabsolute_floor_iff_bare_distinguishability unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
grain sizes were maintained in a range of 20-30 nm... average grain sizes from TEM were 22 nm for both samples
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
Works this paper leans on
-
[1]
Cr additions enhance hardness through classical and nanocrystalline solid solution strengthening contributions, yet this effect requires a smaller effect obstacle spacing and saturates at high concentrations due to the activation of grain boundary -mediated plasticity
-
[2]
Y additions do not directly contribute to solid solution strengthening yet segregate preferentially to grain boundaries, where they enhance interfacial strength and affect dislocation emission behavior, resulting in additional boundary-mediated strengthening. 31
-
[3]
Increasing Y content restricts dislocation bowing into the grain interior during emission and reduces the dislocation curvature and length, thereby reducing the extent of dislocation-solute interactions and weakening the effectiveness of Cr -induced solid solution strengthening. This mechanism is evidenced by the observed decrease in the slope of the hard...
-
[4]
Cube corner nanoindentation reveal s more heterogeneous plastic deformation in the high-Cr samples that experience hardness saturation , indicating that the hardness plateau originates from increased grain boundary -mediated deformation such as grain boundary sliding and grain rotation. Y segregation extends the effective Cr strengthening range by making ...
-
[5]
The highest strength ternary alloy composition achieves a maximum hardness of 11 .0 GPa, among the highest values reported for Ni -based alloys to date and the highest for this grain size. This result underscores the potential of combining nanocrystalline grain structures with targeted grain boundary segregation to realize extreme mechanical performance i...
-
[6]
Koch, Structural nanocrystalline materials: an overview, J Mater Sci 42 (2007) 1403 –
C.C. Koch, Structural nanocrystalline materials: an overview, J Mater Sci 42 (2007) 1403 –
work page 2007
-
[7]
https://doi.org/10.1007/s10853-006-0609-3
-
[8]
T. Chookajorn, H.A. Murdoch, C.A. Schuh, Design of Stable Nanocrystalline Alloys, Science 337 (2012) 951–954. https://doi.org/10.1126/science.1224737
-
[9]
T.J. Rupert, J.C. Trenkle, C.A. Schuh, Enhanced solid solution effects on the strength of nanocrystalline alloys, Acta Materialia 59 (2011) 1619 –1631. https://doi.org/10.1016/j.actamat.2010.11.026
-
[10]
M. Dao, L. Lu, R. Asaro, J. Dehosson, E. Ma, Toward a quantitative understanding of mechanical behavior of nanocrystalline metals, Acta Materialia 55 (2007) 4041 –4065. https://doi.org/10.1016/j.actamat.2007.01.038
-
[11]
C.H. Henager, Reversing inverse Hall-Petch and direct computation of Hall-Petch coefficients, Acta Materialia 265 (2024) 119627. https://doi.org/10.1016/j.actamat.2023.119627
-
[12]
T. Shen, R. Schwarz, S. Feng, J. Swadener, J. Huang, M. Tang, J. Zhang, S. V ogel, Y . Zhao, Effect of solute segregation on the strength of nanocrystalline alloys: Inverse Hall –Petch relation, Acta Materialia 55 (2007) 5007–5013. https://doi.org/10.1016/j.actamat.2007.05.018
-
[13]
L. Wang, Y . Zhang, Z. Zeng, H. Zhou, J. He, P. Liu, M. Chen, J. Han, D.J. Srolovitz, J. Teng, Y . Guo, G. Yang, D. Kong, E. Ma, Y . Hu, B. Yin, X. Huang, Z. Zhang, T. Zhu, X. Han, Tracking the sliding of grain boundaries at the atomic scale, Science 375 (20 22) 1261 –1265. https://doi.org/10.1126/science.abm2612
-
[14]
D. Farkas, A. Frøseth, H. Van Swygenhoven, Grain boundary migration during room temperature deformation of nanocrystalline Ni, Scripta Materialia 55 (2006) 695 –698. https://doi.org/10.1016/j.scriptamat.2006.06.032
-
[15]
L. Wang, J. Teng, P. Liu, A. Hirata, E. Ma, Z. Zhang, M. Chen, X. Han, Grain rotation mediated by grain boundary dislocations in nanocrystalline platinum, Nat Commun 5 (2014) 4402. https://doi.org/10.1038/ncomms5402
-
[16]
A.G. Frøseth, P.M. Derlet, H. Van Swygenhoven, Dislocations emitted from nanocrystalline grain boundaries: nucleation and splitting distance, Acta Materialia 52 (2004) 5863–5870. https://doi.org/10.1016/j.actamat.2004.09.001
-
[17]
H. Van Swygenhoven, P.M. Derlet, A. Hasnaoui, Atomic mechanism for dislocation emission from nanosized grain boundaries, Phys. Rev. B 66 (2002) 024101. https://doi.org/10.1103/PhysRevB.66.024101
-
[18]
V . Turlo, T.J. Rupert, Grain boundary complexions and the strength of nanocrystalline metals: Dislocation emission and propagation, Acta Materialia 151 (2018) 100 –111. https://doi.org/10.1016/j.actamat.2018.03.055
-
[19]
H. Van Swygenhoven, P.M. Derlet, A.G. Frøseth, Nucleation and propagation of dislocations in nanocrystalline fcc metals, Acta Materialia 54 (2006) 1975 –1983. https://doi.org/10.1016/j.actamat.2005.12.026
-
[20]
S. Kondo, T. Mitsuma, N. Shibata, Y . Ikuhara, Direct observation of individual dislocation interaction processes with grain boundaries, Sci. Adv. 2 (2016) e1501926. https://doi.org/10.1126/sciadv.1501926
-
[21]
J. Hu, Y .N. Shi, X. Sauvage, G. Sha, K. Lu, Grain boundary stability governs hardening and softening in extremely fine nanograined metals, Science 355 (2017) 1292 –1296. https://doi.org/10.1126/science.aal5166. 34
-
[22]
J. Schiøtz, F.D. Di Tolla, K.W. Jacobsen, Softening of nanocrystalline metals at very small grain sizes, Nature 391 (1998) 561–563. https://doi.org/10.1038/35328
-
[23]
J. Luo, Grain boundary segregation models for high -entropy alloys: Theoretical formulation and application to elucidate high -entropy grain boundaries, Journal of Applied Physics 135 (2024) 165303. https://doi.org/10.1063/5.0200669
-
[24]
V . Borovikov, M.I. Mendelev, A.H. King, Solute effects on interfacial dislocation emission in nanomaterials: Nucleation site competition and neutralization, Scripta Materialia 154 (2018) 12–15. https://doi.org/10.1016/j.scriptamat.2018.05.011
-
[25]
V . Borovikov, M.I. Mendelev, A.H. King, Effects of solutes on dislocation nucleation from grain boundaries, International Journal of Plasticity 90 (2017) 146 –155. https://doi.org/10.1016/j.ijplas.2016.12.009
-
[26]
L. Qian, J. Zhang, W. Yang, Y . Wang, K. Chan, X.-S. Yang, Maintaining Grain Boundary Segregation-Induced Strengthening Effect in Extremely Fine Nanograined Metals, Nano Lett. 25 (2025) 5493–5501. https://doi.org/10.1021/acs.nanolett.5c01032
-
[27]
Q. Zhuang, D. Liang, J. Luo, K. Chu, K. Yan, L. Yang, C. Wei, F. Jiang, Z. Li, F. Ren, Dual- Nano Composite Design with Grain Boundary Segregation for Enhanced Strength and Plasticity in CoCrNi -CuZr Thin Films, Nano Lett. 25 (2025) 691 –698. https://doi.org/10.1021/acs.nanolett.4c04755
-
[28]
E.-A. Picard, F. Sansoz, Ni solute segregation and associated plastic deformation mechanisms into random FCC Ag, BCC Nb and HCP Zr polycrystals, Acta Materialia 240 (2022) 118367. https://doi.org/10.1016/j.actamat.2022.118367
-
[29]
J. Zuo, T. Nakata, C. Xu, Y .P. Xia, H.L. Shi, X.J. Wang, G.Z. Tang, W.M. Gan, E. Maawad, G.H. Fan, S. Kamado, L. Geng, Effect of grain boundary segregation on microstructure and mechanical properties of ultra-fine grained Mg–Al–Ca–Mn alloy wires, Materials Science and Engineering: A 848 (2022) 143423. https://doi.org/10.1016/j.msea.2022.143423
-
[30]
P.C. Millett, R.P. Selvam, A. Saxena, Improving grain boundary sliding resistance with segregated dopants, Materials Science and Engineering: A 431 (2006) 92 –99. https://doi.org/10.1016/j.msea.2006.05.074
-
[31]
Y . Zhang, G.J. Tucker, J.R. Trelewicz, Stress -assisted grain growth in nanocrystalline metals: Grain boundary mediated mechanisms and stabilization through alloying, Acta Materialia 131 (2017) 39–47. https://doi.org/10.1016/j.actamat.2017.03.060
-
[32]
T. Masuda, X. Sauvage, S. Hirosawa, Z. Horita, Achieving highly strengthened Al–Cu–Mg alloy by grain refinement and grain boundary segregation, Materials Science and Engineering: A 793 (2020) 139668. https://doi.org/10.1016/j.msea.2020.139668
-
[33]
T. Guo, P. Huang, K.W. Xu, F. Wang, T.J. Lu, Solid solution effects on hardness and strain rate sensitivity of nanocrystalline NiFe alloy, Materials Science and Engineering: A 676 (2016) 501–505. https://doi.org/10.1016/j.msea.2016.08.120
-
[34]
C.A. Schuh, T.G. Nieh, H. Iwasaki, The effect of solid solution W additions on the mechanical properties of nanocrystalline Ni, Acta Materialia 51 (2003) 431 –443. https://doi.org/10.1016/S1359-6454(02)00427-5
-
[35]
Fleischer, Substitutional solution hardening, Acta Metallurgica 11 (1963) 203 –209
R.L. Fleischer, Substitutional solution hardening, Acta Metallurgica 11 (1963) 203 –209. https://doi.org/10.1016/0001-6160(63)90213-X
-
[36]
K. Kim, S. Park, T. Kim, Y . Park, G.-D. Sim, D. Lee, Mechanical, electrical properties and microstructures of combinatorial Ni-Mo-W alloy films, Journal of Alloys and Compounds 919 (2022) 165808. https://doi.org/10.1016/j.jallcom.2022.165808. 35
-
[37]
X.F. Zhang, T. Fujita, D. Pan, J.S. Yu, T. Sakurai, M.W. Chen, Influences of grain size and grain boundary segregation on mechanical behavior of nanocrystalline Ni, Materials Science and Engineering: A 527 (2010) 2297–2304. https://doi.org/10.1016/j.msea.2009.12.005
-
[38]
M.A. Atwater, K.A. Darling, A Visual Library of Stability in Binary Metallic Systems: The Stabilization of Nanocrystalline Grain Size by Solute Addition: Part 1:, Defense Technical Information Center, Fort Belvoir, V A, 2012. https://doi.org/10.21236/ADA561871
-
[39]
H. Okamoto, M.E. Schlesinger, E.M. Mueller, eds., Cr (Chromium) Binary Alloy Phase Diagrams, in: Alloy Phase Diagrams, ASM International, 2016: pp. 281 –297. https://doi.org/10.31399/asm.hb.v03.a0006157
-
[40]
Baker, Properties of Metals, in: J.R
H. Baker, Properties of Metals, in: J.R. Davis (Ed.), Metals Handbook Desk Edition, 2nd ed., ASM International, 1998: pp. 114–121. https://doi.org/10.31399/asm.hb.mhde2.a0003086
-
[41]
Y . Mishima, S. Ochiai, N. Hamao, M. Yodogawa, T. Suzuki, Solid Solution Hardening of Nickel —Role of Transition Metal and B -subgroup Solutes —, Transactions of the Japan Institute of Metals 27 (1986) 656–664. https://doi.org/10.2320/matertrans1960.27.656
-
[42]
R.M.N. Pelloux, N.J. Grant, Solid solutions and second phase strengthening of nickel alloys at high and low temperatures, Trans. Metall. Soc. AIME 218 (1960) 232–237
work page 1960
-
[43]
K.A. Darling, L.J. Kecskes, M. Atwater, J. Semones, R.O. Scattergood, C.C. Koch, Thermal stability of nanocrystalline nickel with yttrium additions, J. Mater. Res. 28 (2013) 1813–1819. https://doi.org/10.1557/jmr.2013.9
-
[44]
G. Palumbo, S.J. Thorpe, K.T. Aust, On the contribution of triple junctions to the structure and properties of nanocrystalline materials, Scripta Metallurgica et Materialia 24 (1990) 1347–
work page 1990
-
[45]
https://doi.org/10.1016/0956-716X(90)90354-J
-
[46]
J. Kong, M.J.R. Haché, J. Tam, J.L. McCrea, J. Howe, U. Erb, On the extrinsic Hall-Petch to inverse Hall -Petch transition in nanocrystalline Ni -Co electrodeposits, Scripta Materialia 218 (2022) 114799. https://doi.org/10.1016/j.scriptamat.2022.114799
-
[47]
J.A. Thornton, Influence of substrate temperature and deposition rate on structure of thick sputtered Cu coatings, Journal of Vacuum Science and Technology 12 (1975) 830 –835. https://doi.org/10.1116/1.568682
-
[48]
L.A. Giannuzzi, J.L. Drown, S.R. Brown, R.B. Irwin, F.A. Stevie, Applications of the FIB lift-out technique for TEM specimen preparation, Microsc. Res. Tech. 41 (1998) 285 –290. https://doi.org/10.1002/(SICI)1097-0029(19980515)41:4%3C285::AID- JEMT1%3E3.0.CO;2-Q
-
[49]
J. Chen, S.J. Bull, On the relationship between plastic zone radius and maximum depth during nanoindentation, Surface and Coatings Technology 201 (2006) 4289 –4293. https://doi.org/10.1016/j.surfcoat.2006.08.099
-
[50]
W.C. Oliver, G.M. Pharr, Measurement of hardness and elastic modulus by instrumented indentation: Advances in understanding and refinements to methodology, J. Mater. Res. 19 (2004) 3–20. https://doi.org/10.1557/jmr.2004.19.1.3
-
[51]
T.R. Koenig, Z. Rao, E. Chason, G.J. Tucker, G.B. Thompson, The microstructural and stress evolution in sputter deposited Ni thin films, Surface and Coatings Technology 412 (2021) 126973. https://doi.org/10.1016/j.surfcoat.2021.126973
-
[52]
Y . Zhang, Z. Zhang, W. Yao, X. Liang, Microstructure, mechanical properties and corrosion resistance of high -level hard Nb -Ta-W and Nb -Ta-W-Hf multi-principal element alloy thin films, Journal of Alloys and Compounds 920 (2022) 166000. https://doi.org/10.1016/j.jallcom.2022.166000. 36
-
[53]
L. Balogh, G. Ribárik, T. Ungár, Stacking faults and twin boundaries in fcc crystals determined by x-ray diffraction profile analysis, Journal of Applied Physics 100 (2006) 023512. https://doi.org/10.1063/1.2216195
-
[54]
L. Vegard, Die Konstitution der Mischkristalle und die Raumfüllung der Atome, Zeitschrift Für Physik 5 (1921) 17–26. https://doi.org/10.1007/BF01349680
-
[55]
J.X. Li, Y .-N. Shi, Z.S. You, X.Y . Li, Tensile strain induced texture evolution in a Ni–Mo alloy with extremely fine nanotwinned columnar grains, Materials Science and Engineering: A 812 (2021) 141108. https://doi.org/10.1016/j.msea.2021.141108
-
[56]
G.B. Thompson, R. Banerjee, X.D. Zhang, P.M. Anderson, H.L. Fraser, Chemical ordering and texture in Ni –25 at% Al thin films, Acta Materialia 50 (2002) 643 –651. https://doi.org/10.1016/S1359-6454(01)00373-1
-
[57]
L. Velasco, A.M. Hodge, Growth twins in high stacking fault energy metals: Microstructure, texture and twinning, Materials Science and Engineering: A 687 (2017) 93 –98. https://doi.org/10.1016/j.msea.2017.01.065
-
[58]
V . Maier, K. Durst, J. Mueller, B. Backes, H.W. Höppel, M. Göken, Nanoindentation strain- rate jump tests for determining the local strain -rate sensitivity in nanocrystalline Ni and ultrafine-grained Al, J. Mater. Res. 26 (2011) 1421 –1430. https://doi.org/10.1557/jmr.2011.156
-
[59]
R. Schwaiger, B. Moser, M. Dao, N. Chollacoop, S. Suresh, Some critical experiments on the strain -rate sensitivity of nanocrystalline nickel, Acta Materialia 51 (2003) 5159 –5172. https://doi.org/10.1016/S1359-6454(03)00365-3
-
[60]
W. Tillmann, D. Kokalj, D. Stangier, V . Schöppner, H.B. Benis, H. Malatyali, Influence of Cr-Content on the thermoelectric and mechanical properties of NiCr thin film thermocouples synthesized on thermally sprayed Al2O3, Thin Solid Films 663 (2018) 148 –158. https://doi.org/10.1016/j.tsf.2018.08.023
-
[61]
I. Bikmukhametov, A. Gupta, T.R. Koenig, G.J. Tucker, G.B. Thompson, Consequences of solute partitioning on hardness in stabilized nanocrystalline alloys, Materials Science and Engineering: A 875 (2023) 145113. https://doi.org/10.1016/j.msea.2023.145113
-
[62]
V . Petley, S. Sathishkumar, K.H. Thulasi Raman, G.M. Rao, U. Chandrasekhar, Microstructural and mechanical characteristics of Ni –Cr thin films, Materials Research Bulletin 66 (2015) 59–64. https://doi.org/10.1016/j.materresbull.2015.02.002
-
[63]
P. Nagy, N. Rohbeck, G. Roussely, P. Sortais, J.L. Lábár, J. Gubicza, J. Michler, L. Pethö, Processing and characterization of a multibeam sputtered nanocrystalline CoCrFeNi high - entropy alloy film, Surface and Coatings Technology 386 (2020) 125465. https://doi.org/10.1016/j.surfcoat.2020.125465
-
[64]
Z. Wang, C. Wang, Y .-L. Zhao, Y .-C. Hsu, C.-L. Li, J.-J. Kai, C.-T. Liu, C.-H. Hsueh, High hardness and fatigue resistance of CoCrFeMnNi high entropy alloy films with ultrahigh - density nanotwins, International Journal of Plasticity 131 (2020) 102726. https://doi.org/10.1016/j.ijplas.2020.102726
-
[65]
Y.-L. Liu, Y . Zhang, H.-B. Zhou, G.-H. Lu, M. Kohyama, Theoretical strength and charge redistribution of fcc Ni in tension and shear, J. Phys.: Condens. Matter 20 (2008) 335216. https://doi.org/10.1088/0953-8984/20/33/335216
-
[66]
Y . Wang, Y . Qi, T. He, M. Feng, Grain refinement induced by grain boundary segregation in FeNiCrCoCu high-entropy alloys using molecular dynamics simulation of nanoindentation, Materials Chemistry and Physics 310 (2023) 128489. https://doi.org/10.1016/j.matchemphys.2023.128489. 37
-
[67]
R.I. Babicheva, S.V . Dmitriev, L. Bai, Y . Zhang, S.W. Kok, G. Kang, K. Zhou, Effect of grain boundary segregation on the deformation mechanisms and mechanical properties of nanocrystalline binary aluminum alloys, Computational Materials Science 117 (2016) 445–
work page 2016
-
[68]
https://doi.org/10.1016/j.commatsci.2016.02.013
-
[69]
P.C. Millett, R.P. Selvam, S. Bansal, A. Saxena, Atomistic simulation of grain boundary energetics – Effects of dopants, Acta Materialia 53 (2005) 3671 –3678. https://doi.org/10.1016/j.actamat.2005.04.031
-
[70]
N.Q. V o, J. Schäfer, R.S. Averback, K. Albe, Y . Ashkenazy, P. Bellon, Reaching theoretical strengths in nanocrystalline Cu by grain boundary doping, Scripta Materialia 65 (2011) 660 –
work page 2011
-
[71]
https://doi.org/10.1016/j.scriptamat.2011.06.048
-
[72]
N.Q. V o, R.S. Averback, P. Bellon, A. Caro, Limits of hardness at the nanoscale: Molecular dynamics simulations, Phys. Rev. B 78 (2008) 241402. https://doi.org/10.1103/PhysRevB.78.241402
-
[73]
Tabor, The Hardness of Metals, OUP Oxford, 2000
D. Tabor, The Hardness of Metals, OUP Oxford, 2000
work page 2000
-
[74]
F. Dalla Torre, H. Van Swygenhoven, M. Victoria, Nanocrystalline electrodeposited Ni: microstructure and tensile properties, Acta Materialia 50 (2002) 3957 –3970. https://doi.org/10.1016/S1359-6454(02)00198-2
-
[75]
R.J. Asaro, P. Krysl, B. Kad, Deformation mechanism transitions in nanoscale fcc metals, Philosophical Magazine Letters 83 (2003) 733 –743. https://doi.org/10.1080/09500830310001614540
-
[76]
W. Tang, E.G. Herbert, A. Anand, M. Boebinger, J. Poplawsky, Y . Yang, A.E. Perrin, Use of friction stir processing to synthesize nanocrystalline, grain boundary segregating Fe -Ti alloys, Materials Science and Engineering: A 959 (2026) 150050. https://doi.org/10.1016/j.msea.2026.150050
-
[77]
R.J. Asaro, S. Suresh, Mechanistic models for the activation volume and rate sensitivity in metals with nanocrystalline grains and nano-scale twins, Acta Materialia 53 (2005) 3369–3382. https://doi.org/10.1016/j.actamat.2005.03.047
-
[78]
E. Bitzek, C. Brandl, D. Weygand, P.M. Derlet, H. Van Swygenhoven, Atomistic simulation of a dislocation shear loop interacting with grain boundaries in nanocrystalline aluminium, Modelling Simul. Mater. Sci. Eng. 17 (2009) 055008. https://doi.org/10.1088 /0965- 0393/17/5/055008
work page 2009
-
[79]
Z. Pan, T.J. Rupert, Damage nucleation from repeated dislocation absorption at a grain boundary, Computational Materials Science 93 (2014) 206 –209. https://doi.org/10.1016/j.commatsci.2014.07.008
-
[80]
D. Guo, S. Song, R. Luo, W.A. Goddard, M. Chen, K.M. Reddy, Q. An, Grain Boundary Sliding and Amorphization are Responsible for the Reverse Hall-Petch Relation in Superhard Nanocrystalline Boron Carbide, Phys. Rev. Lett. 121 (2018) 145504. https://doi.org/10.1103/PhysRevLett.121.145504
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