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	<title>dynamic recovery &#8211; Science</title>
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	<title>dynamic recovery &#8211; Science</title>
	<link>https://scienmag.com</link>
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		<title>Microstructure evolution and dynamic recrystallization of spray-formed Al–Zn–Mg–Cu alloy under hot deformation</title>
		<link>https://scienmag.com/microstructure-evolution-and-dynamic-recrystallization-of-spray-formed-al-zn-mg-cu-alloy-under-hot-deformation/</link>
		
		<dc:creator><![CDATA[Neil Sanderson]]></dc:creator>
		<pubDate>Tue, 20 Oct 2026 20:51:50 +0000</pubDate>
				<category><![CDATA[Technology and Engineering]]></category>
		<category><![CDATA[Al–Zn–Mg–Cu alloy]]></category>
		<category><![CDATA[Al–Zn–Mg–Cu alloy hot deformation]]></category>
		<category><![CDATA[anisotropic grain orientation during hot deformation]]></category>
		<category><![CDATA[continuous dynamic recrystallization mechanisms]]></category>
		<category><![CDATA[continuous recrystallization]]></category>
		<category><![CDATA[dynamic recovery]]></category>
		<category><![CDATA[effects of loading history on microstructure]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[flow stress behavior under dynamic recrystallization]]></category>
		<category><![CDATA[grain boundaries]]></category>
		<category><![CDATA[hot deformation]]></category>
		<category><![CDATA[hot deformation behavior of Al–Zn–Mg–Cu alloys]]></category>
		<category><![CDATA[influence of deformation temperature and strain rate]]></category>
		<category><![CDATA[low-angle grain boundary evolution]]></category>
		<category><![CDATA[microstructure]]></category>
		<category><![CDATA[microstructure evolution]]></category>
		<category><![CDATA[microstructure evolution under varying deformation conditions]]></category>
		<category><![CDATA[spray-formed alloy]]></category>
		<category><![CDATA[spray-formed aluminum alloy microstructure]]></category>
		<category><![CDATA[strain-rate history]]></category>
		<category><![CDATA[strain-rate-jump compression testing]]></category>
		<category><![CDATA[subgrain rotation in aluminum alloys]]></category>
		<category><![CDATA[texture intensity]]></category>
		<category><![CDATA[uniaxial compression]]></category>
		<guid isPermaLink="false">https://scienmag.com/?p=323037</guid>

					<description><![CDATA[An experimental compression study reports how temperature, strain rate and loading history affected flow stress, texture and continuous dynamic recrystallization in spray-formed Al–Zn–Mg–Cu alloy.]]></description>
										<content:encoded><![CDATA[<p>An experimental study of spray-formed Al–Zn–Mg–Cu alloy found that continuous dynamic recrystallization, expressed through a subgrain structure, was associated with changes in flow stress and texture during hot deformation. The reported behavior varied with deformation temperature and strain rate, with higher temperatures and lower strain rates promoting further continuous recrystallization development and reducing texture intensity.</p>
<p>The researchers investigated the alloy using hot uniaxial compression tests at 350–450 °C and strain rates of 0.01–1 s<sup>−1</sup>. They also conducted strain-rate-jump compression tests to examine the influence of loading-rate history. These were laboratory deformation experiments on one spray-formed alloy; the available abstract does not describe replication, uncertainty estimates or the number of specimens tested.</p>
<p>According to the abstract, subgrain rotation driven by dynamic recovery and deformation was identified as the principal mechanism of continuous dynamic recrystallization. Three forms of low-angle grain boundaries were observed: equiaxed subgrain structures, and low-angle boundaries with preferred orientations either parallel to the compression direction or perpendicular to it. The reported orientations were also associated with grain orientation.</p>
<p>The strain-rate-jump tests showed an asymmetric response in flow stress and microstructure evolution to loading history, which the abstract describes as observed for the first time in hot deformation of Al–Zn–Mg–Cu alloy. The authors suggest that dislocation accumulation and the time available for rearrangement through dynamic recovery may contribute to differences from constant-strain-rate uniaxial compression. The available summary does not provide the magnitude of the flow-stress changes, quantitative texture data, detailed boundary statistics or full methodological information, so the scope of these findings is limited to the reported abstract rather than an assessment of the complete article.</p>
<p><strong>Subject of Research:</strong> Hot-deformation microstructure and continuous dynamic recrystallization in spray-formed Al–Zn–Mg–Cu alloy</p>
<p><strong>Article Title:</strong> Microstructure evolution and dynamic recrystallization of spray-formed Al–Zn–Mg–Cu alloy under hot deformation</p>
<p><strong>Article References:</strong> Tao, L., Zhang, Z., Jia, W., Sun, C., Li, D., Jia, Z., &amp; Zhou, G. (2026). Microstructure evolution and dynamic recrystallization of spray-formed Al–Zn–Mg–Cu alloy under hot deformation. <em>Journal of Materials Science, 61</em>(43), 33974-33994. <a href="https://doi.org/10.1007/s10853-026-13710-y" rel="noopener noreferrer">https://doi.org/10.1007/s10853-026-13710-y</a></p>
<p><strong>Image Credits:</strong> AI Generated</p>
<p><strong>DOI:</strong> <a href="https://doi.org/10.1007/s10853-026-13710-y" rel="noopener noreferrer">10.1007/s10853-026-13710-y</a></p>
<p><strong>Keywords:</strong> Al–Zn–Mg–Cu alloy, spray-formed alloy, hot deformation, continuous recrystallization, dynamic recovery, uniaxial compression, strain-rate history, microstructure evolution, texture intensity, grain boundaries, Microstructure, evolution</p>
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		<post-id xmlns="com-wordpress:feed-additions:1">323037</post-id>	</item>
		<item>
		<title>Nitrogen-Containing High-Entropy Alloy Reveals Temperature-Shaped Microstructural Recovery</title>
		<link>https://scienmag.com/nitrogen-containing-high-entropy-alloy-reveals-temperature-shaped-microstructural-recovery/</link>
		
		<dc:creator><![CDATA[Neil Sanderson]]></dc:creator>
		<pubDate>Tue, 20 Oct 2026 08:25:40 +0000</pubDate>
				<category><![CDATA[Technology and Engineering]]></category>
		<category><![CDATA[annealing twins]]></category>
		<category><![CDATA[continuous dynamic recrystallization]]></category>
		<category><![CDATA[dislocation storage and recovery mechanisms]]></category>
		<category><![CDATA[dynamic recovery]]></category>
		<category><![CDATA[dynamic recrystallization in high-entropy alloys]]></category>
		<category><![CDATA[effect of temperature on flow stress and strain]]></category>
		<category><![CDATA[flow stress]]></category>
		<category><![CDATA[grain refinement]]></category>
		<category><![CDATA[high entropy alloys]]></category>
		<category><![CDATA[High-entropy alloy microstructural recovery]]></category>
		<category><![CDATA[high-entropy alloy thermomechanical properties]]></category>
		<category><![CDATA[hot deformation]]></category>
		<category><![CDATA[isothermal compression testing of FeMnCoCrN alloys]]></category>
		<category><![CDATA[Microstructural]]></category>
		<category><![CDATA[microstructural softening and hardening phenomena]]></category>
		<category><![CDATA[microstructural stability]]></category>
		<category><![CDATA[microstructure evolution during hot deformation]]></category>
		<category><![CDATA[nitrogen-containing alloys]]></category>
		<category><![CDATA[stability]]></category>
		<category><![CDATA[strain rate effects on alloy deformation]]></category>
		<category><![CDATA[Temperature-dependent]]></category>
		<category><![CDATA[temperature-dependent deformation behavior]]></category>
		<guid isPermaLink="false">https://scienmag.com/?p=317103</guid>

					<description><![CDATA[Compression tests of an as-cast nitrogen-containing Fe–Mn–Co–Cr high-entropy alloy reveal that dynamic recovery, continuous recrystallization and grain refinement shift substantially between 700 and 900 °C.]]></description>
										<content:encoded><![CDATA[<p>A laboratory study of an as-cast nitrogen-containing high-entropy alloy shows that its microstructural response during hot deformation changes sharply with temperature, even though the alloy’s flow stress does not fall in a simple, step-by-step manner. Researchers investigated Fe46Mn35.5Co9Cr9N0.5 at.% alloy through isothermal compression tests conducted from 700 to 1000 °C at a strain rate of 0.001 s−1. The material displayed a pronounced decrease in peak flow stress as temperature increased, together with a relatively high peak strain of approximately 0.4 and limited post-peak softening.</p>
<p>The central finding is that dynamic recrystallization could begin well below the stress and strain levels associated with the peak of the deformation curve. Poliak–Jonas analysis indicated that the restoration process started at stresses and strains far below the measured peak values, while the final microstructure contained a significant fraction of recrystallized grains. This distinction matters because the onset of recrystallization did not automatically produce a dominant macroscopic softening response. Instead, the alloy’s behavior reflected a sustained competition between the storage of dislocations and mechanisms that restore, or reorganize, the deformed structure.</p>
<p>At 700 °C, the deformation structure was dominated by extended dynamic recovery, accompanied by localized evidence of continuous dynamic recrystallization, or cDRX. The researchers associated this state with elongated grains, serrated grain boundaries and dense networks of low-angle boundaries. In practical terms, the alloy was simultaneously retaining deformation-related defects and developing localized regions of new grain formation. The limited reduction in flow stress beyond the peak strain is consistent with the idea that recovery and dislocation storage continued to operate strongly at this temperature, tempering the expected macroscopic effect of the localized recrystallization.</p>
<p>At 900 °C, advanced cDRX became the more important restoration mechanism, producing extensive grain refinement and a larger population of fine, equiaxed recrystallized grains. The study also recorded an unusual intragranular necklace-like arrangement and abundant Σ3 annealing twins. These features indicate a more extensive reorganization of the alloy’s microstructure than was observed at the lower temperature. Across the tested range, the work demonstrates that reaching conditions favorable for dynamic recrystallization is not the same as observing a large drop in flow stress: at lower temperature, recovery and dislocation storage remained predominant alongside localized cDRX, whereas at 900 °C, substantially greater cDRX development accompanied pronounced grain refinement and flow softening. The study concerns hot-deformation behavior in a specific as-cast alloy composition and testing protocol, so its results describe the mechanisms observed under those conditions rather than universal behavior for all high-entropy alloys.</p>
<p><strong>Subject of Research:</strong> Temperature-dependent hot-deformation and microstructural restoration mechanisms in an as-cast Fe–Mn–Co–Cr high-entropy alloy</p>
<p><strong>Article Title:</strong> Temperature-dependent microstructural stability and dynamic restoration mechanisms in an as-cast nitrogen-containing Fe–Mn–Co–Cr high-entropy alloy</p>
<p><strong>Article References:</strong> Shamouni, Y., Zarei-Hanzaki, A., Ghorbani, M., Tajik, A., Moshiri, A., Abbasi, A., Park, H., Kim, H. S., &amp; Abedi, H. R. (2026). Temperature-dependent microstructural stability and dynamic restoration mechanisms in an as-cast nitrogen-containing Fe–Mn–Co–Cr high-entropy alloy. <em>Journal of Materials Science</em>. <a href="https://doi.org/10.1007/s10853-026-13702-y" rel="noopener noreferrer">https://doi.org/10.1007/s10853-026-13702-y</a></p>
<p><strong>Image Credits:</strong> AI Generated</p>
<p><strong>DOI:</strong> <a href="https://doi.org/10.1007/s10853-026-13702-y" rel="noopener noreferrer">10.1007/s10853-026-13702-y</a></p>
<p><strong>Keywords:</strong> high-entropy alloys, nitrogen-containing alloys, hot deformation, dynamic recovery, continuous dynamic recrystallization, microstructural stability, grain refinement, annealing twins, flow stress, Temperature-dependent, microstructural, stability</p>
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		<post-id xmlns="com-wordpress:feed-additions:1">317103</post-id>	</item>
		<item>
		<title>Cantor Alloy&#8217;s Hidden Shell Network Rewrites the Rules of Hot Deformation</title>
		<link>https://scienmag.com/cantor-alloys-hidden-shell-network-rewrites-the-rules-of-hot-deformation/</link>
		
		<dc:creator><![CDATA[Neil Sanderson]]></dc:creator>
		<pubDate>Mon, 05 Oct 2026 15:57:41 +0000</pubDate>
				<category><![CDATA[Technology and Engineering]]></category>
		<category><![CDATA[advanced materials engineering]]></category>
		<category><![CDATA[alloy mechanical milling]]></category>
		<category><![CDATA[bimodal grain structure]]></category>
		<category><![CDATA[Cantor alloy]]></category>
		<category><![CDATA[coarse grain pockets]]></category>
		<category><![CDATA[dynamic recovery]]></category>
		<category><![CDATA[dynamic recrystallization]]></category>
		<category><![CDATA[flow softening]]></category>
		<category><![CDATA[harmonic structure]]></category>
		<category><![CDATA[harmonic-structured alloy architecture]]></category>
		<category><![CDATA[heterostructured materials]]></category>
		<category><![CDATA[high entropy alloys]]></category>
		<category><![CDATA[high-temperature material properties]]></category>
		<category><![CDATA[hot deformation]]></category>
		<category><![CDATA[hot deformation behavior]]></category>
		<category><![CDATA[oxide particles]]></category>
		<category><![CDATA[severe plastic deformation]]></category>
		<category><![CDATA[shell network in alloys]]></category>
		<category><![CDATA[spark plasma sintering]]></category>
		<category><![CDATA[ultrafine grain network]]></category>
		<category><![CDATA[ultrafine grains]]></category>
		<guid isPermaLink="false">https://scienmag.com/?p=238692</guid>

					<description><![CDATA[A harmonic-structured CoCrFeMnNi high-entropy alloy shows pronounced flow softening at high temperatures because its ultrafine-grained shell network recovers preferentially while coarse-grained cores rotate cooperatively during deformation.]]></description>
										<content:encoded><![CDATA[<p>High-entropy alloys have spent two decades dazzling materials scientists with a deceptively simple idea: mix five or more metallic elements in roughly equal proportions and let the resulting chemical chaos produce extraordinary properties. The most famous of them all, the equiatomic CoCrFeMnNi alloy known as the Cantor alloy, has been poked, stretched, frozen, and heated in laboratories around the world. Yet a new study published in the Journal of Materials Science shows that when this celebrated alloy is given an unusual architectural makeover, it behaves in ways that conventional, uniformly grained versions of the same material simply cannot match at high temperatures.</p>
<p>The research, led by Nurul Nadiah Mahmud of Ritsumeikan University in Japan together with colleagues at Ritsumeikan and Pohang University of Science and Technology in South Korea, focused on a so-called harmonic-structured version of the Cantor alloy. The term harmonic describes a deliberately bimodal grain arrangement: a continuous three-dimensional network of ultrafine grains, called the Shell, completely envelops isolated pockets of coarse grains, called the Core. The team produced this architecture by mechanically milling alloy powder and then consolidating it using spark plasma sintering, a rapid consolidation technique that preserves the deformed, fine-grained powder surfaces while allowing the interiors to remain relatively coarse. A reference material with a homogeneous coarse-grained structure was prepared for comparison, giving the researchers a clean experimental contrast between two materials of identical chemistry but radically different microstructure.</p>
<p>Why does this matter? Because ultrafine-grained metals, while famously strong at room temperature, tend to lose their advantage when things get hot. At elevated temperatures, the abundance of grain boundaries in fine-grained materials becomes a liability: boundaries slide, migrate, and serve as fast lanes for diffusion-driven creep. The conventional wisdom has long been that if you want a metal to survive high-temperature service, you should coarsen its grains. The harmonic design challenges that assumption by pairing the two regimes instead of choosing between them, letting the fine-grained network and the coarse-grained cores share the mechanical burden in a way that neither could achieve alone.</p>
<p>To probe how the harmonic Cantor alloy copes with heat and stress, the team carried out compression tests across a wide thermal range, from room temperature up to 1173 kelvin, roughly 900 degrees Celsius, at several initial strain rates. The comparison revealed a striking divergence in flow behavior. The homogeneous coarse-grained material showed the textbook response: an initial period of strain hardening as dislocations multiplied, followed by a nearly steady-state flow in which hardening and softening processes balanced out. The harmonic material, by contrast, hardened briefly and then softened dramatically, with the flow stress falling steadily as deformation continued at 1073 and 1173 kelvin. That pronounced flow softening was the central puzzle the researchers set out to explain.</p>
<p>The answer lies in where the damage, or rather the restoration, happens. Detailed microstructural characterization showed that dynamic recovery and dynamic recrystallization, the two great softening mechanisms of hot deformation, occurred preferentially in the ultrafine-grained Shell region. This makes physical sense. The Shell is packed with grain boundaries and stored dislocation density left over from the severe plastic deformation of mechanical milling, so it possesses both the driving force and the short-circuit diffusion paths needed for recrystallization nuclei to form and grow. In effect, the Shell acts as a distributed softening layer, continuously renewing itself and absorbing strain while the coarse-grained Cores retain their load-bearing integrity.</p>
<p>The study also uncovered an unexpected microstructural player: cubic oxide particles enriched in chromium and manganese, observed within the deformed Shell. Comparing the deformed material with the as-sintered starting microstructure, the researchers concluded that these particles may have precipitated or grown during high-temperature exposure and deformation. The Cantor alloy is known from prior oxidation studies to form manganese- and chromium-rich oxides at elevated temperatures, so the observation is chemically plausible. However, the authors are careful to note a limitation: with the evidence available, the respective contributions of simple thermal exposure and active plastic deformation to the oxide particles&#8217; appearance could not be separated. Whether these particles help, hinder, or merely accompany the softening process, and what role the oxide-matrix interfaces might play, remains an open question the study explicitly leaves unresolved.</p>
<p>Perhaps the most visually compelling finding came from quasi-in-situ observations, in which the same microscopic regions were imaged at successive stages of deformation. These revealed something remarkable: as strain localized in the Shell, the adjacent coarse-grained Cores did not merely sit still and carry load. Instead, they underwent rotational deformation, physically pivoting and reorienting as the surrounding fine-grained network yielded. The result is a cooperative deformation mode in which the two structural domains work in concert across the entire harmonic architecture. Rather than the Shell simply acting as a weak phase that shears while the Cores remain rigid spectators, the whole structure participates in accommodating the imposed strain, with rotation of the Cores providing an additional channel for plastic flow that a homogeneous material cannot offer.</p>
<p>This cooperative mechanism connects the work to a broader and rapidly growing field of heterostructured materials research. Scientists such as Yuntian Zhu and Xiaofang Wu have argued in recent years that deliberately heterogeneous microstructures generate back stresses and hetero-deformation-induced hardening, in which strain partitioning between soft and hard domains produces extra strength and work-hardening capacity beyond what either domain achieves alone. Earlier work by the same harmonic-structure research community, including studies of harmonic CoCrMo alloys, pure nickel, and titanium alloys, established that the Shell-Core design boosts room-temperature strength-ductility combinations. The new study extends the concept into the hot-deformation regime, showing that the same architecture also reshapes how microstructural restoration and strain accommodation unfold at temperatures where engineers typically forge, extrude, or superplastically form metals.</p>
<p>The practical implications are tantalizing. Flow softening during hot working is generally desirable: it means the material becomes easier to shape as deformation proceeds, reducing forming loads and improving process stability. A high-entropy alloy whose softening is built into its microstructure, rather than relying on phase transformations or adiabatic heating, could offer more predictable and controllable thermomechanical processing. At the same time, the findings raise design questions for high-temperature service. If the Shell network preferentially recrystallizes and softens, engineers must understand how that network evolves over long exposures, and whether the Cr-Mn-rich oxide particles that appear along the way strengthen it as dispersoids or weaken it as interface sources of damage.</p>
<p>What the study ultimately delivers is a new mechanistic picture of a famous alloy. The pronounced flow softening of the harmonic Cantor alloy, the authors conclude, arises from preferential microstructural restoration and strain accommodation within the ultrafine-grained Shell network, working together with the cooperative rotation of the coarse-grained Cores. The possible contribution of the oxide particles and their interfaces remains unresolved, a candid acknowledgment that will surely drive follow-up experiments. For a field that has spent years cataloguing the room-temperature virtues of high-entropy alloys and the high-temperature virtues of coarse grains, this work demonstrates that architecture, not just chemistry or grain size alone, can be the decisive variable. The harmonic design, first proposed as a promising microstructure concept by Kei Ameyama and colleagues, now has a documented high-temperature personality of its own, one in which a softening skin and rotating cores dance together under load. As high-entropy alloys edge closer to real applications in energy, aerospace, and tooling, understanding how such designed heterogeneities behave when the heat is on may prove just as important as the extraordinary strength they display on the benchtop.</p>
<p><strong>Subject of Research:</strong> High-temperature deformation behavior and microstructural evolution of a harmonic-structured CoCrFeMnNi high-entropy alloy</p>
<p><strong>Article Title:</strong> High-temperature deformation and microstructural evolution of a harmonic-structured CoCrFeMnNi high-entropy alloy</p>
<p><strong>Article References:</strong> Mahmud, N. N., Kawano, H., Kim, J., Onoue, S., Kim, H. S., Fujiwara, H., &amp; Ameyama, K. (2026). High-temperature deformation and microstructural evolution of a harmonic-structured CoCrFeMnNi high-entropy alloy. <em>Journal of Materials Science</em>. <a href="https://doi.org/10.1007/s10853-026-13874-7" rel="noopener noreferrer">https://doi.org/10.1007/s10853-026-13874-7</a></p>
<p><strong>Image Credits:</strong> AI Generated</p>
<p><strong>DOI:</strong> <a href="https://doi.org/10.1007/s10853-026-13874-7" rel="noopener noreferrer">10.1007/s10853-026-13874-7</a></p>
<p><strong>Keywords:</strong> high-entropy alloys, Cantor alloy, harmonic structure, hot deformation, dynamic recrystallization, dynamic recovery, ultrafine grains, spark plasma sintering, flow softening, oxide particles, heterostructured materials, severe plastic deformation</p>
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