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arxiv: 2606.13420 · v1 · pith:VZSTLQNKnew · submitted 2026-06-11 · ❄️ cond-mat.mtrl-sci

The phase composition and physical properties of melt-quenched multicomponent alloy FeCoNiB0.7Si0.3Be

Pith reviewed 2026-06-27 06:06 UTC · model grok-4.3

classification ❄️ cond-mat.mtrl-sci
keywords multicomponent alloymelt-quenchedB2 phasemicrohardnesscoercive fieldferromagneticphase compositionFeCoNiB0.7Si0.3Be
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The pith

Melt-quenching the FeCoNiB0.7Si0.3Be alloy increases its B2 phase fraction, lowering microhardness while raising coercivity.

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

This paper studies the effects of rapid cooling on the phase makeup and properties of the multicomponent alloy FeCoNiB0.7Si0.3Be. In the melt-quenched state, produced at cooling rates around 10^6 K/s, the share of the ordered B2 phase grows relative to the as-cast condition. The higher B2 content correlates with a drop in microhardness and a large rise in coercive field. These shifts are tied to finer microstructure and greater internal stresses introduced by the fast quench. The findings show how processing speed can adjust mechanical and magnetic traits in such alloys.

Core claim

X-ray analysis shows a multiphase structure consisting of a BCC-type ordered B2 phase and intermetallic (Fe, Ni, Co)2B compounds. Melt-quenching increases the B2 fraction, which decreases microhardness from 10400 MPa to 8900 MPa. The coercive field rises from 5200 A/m to 17500 A/m due to structure refinement and increased microstresses. The alloy is ferromagnetic in both states.

What carries the argument

The fraction of the B2 ordered phase, which rises under rapid quenching and directly influences the measured hardness and magnetic coercivity.

Load-bearing premise

The observed property differences stem primarily from the change in B2 phase fraction and the associated structural refinement rather than from experimental variations or undetected phases.

What would settle it

If an experiment at a moderate cooling rate shows B2 fraction and property values that do not fit between the as-cast and melt-quenched extremes, the direct link between phase fraction and properties would be weakened.

Figures

Figures reproduced from arXiv: 2606.13420 by Oleksandr I. Kushnerov, Pavlo O. Galagan, Sergey I. Ryabtsev, Valerij F. Bashev.

Figure 1
Figure 1. Figure 1: Fig.1 [PITH_FULL_IMAGE:figures/full_fig_p006_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: Optical micrograph of the as-cast (a) and SEM image of the melt￾quenched (b) FeCoNiB0.7Si0.3Be HEA samples. Comparative analysis of the microhardness of the FeCoNiB0.7Si0.3Be HEA in different states revealed significant differences between the samples. The as-cast samples exhibited a microhardness of Hμ = 10400±300 MPa, which exceeds the values of the MQ samples (8900±300 MPa). The high microhardness of th… view at source ↗
Figure 3
Figure 3. Figure 3: Fig.3. Hysteresis loops of as [PITH_FULL_IMAGE:figures/full_fig_p008_3.png] view at source ↗
read the original abstract

The structure and physical properties of the high-entropy multicomponent alloy FeCoNiB0.7Si0.3Be in the as-cast and melt-quenched states were studied. The cooling rate of the melt-quenched films was estimated to be approximately 10^6 K/s based on the film thickness. X-ray analysis revealed a multiphase structure, including a BCC-type ordered phase (structural type B2) and intermetallic compounds (Fe, Ni, Co)2B. In melt-quenched samples, the fraction of the B2 phase increased, leading to a decrease in microhardness from 10400 MPa in the as-cast state to 8900 MPa in the melt-quenched state. Magnetic studies confirmed the ferromagnetic nature of the FeCoNiB0.7Si0.3Be alloy. The coercive field of melt-quenched samples (17500 A/m) was significantly higher than that of the as-cast ones (5200 A/m), which is attributed to structure refinement and an increased level of microstresses.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 0 minor

Summary. The manuscript reports an experimental study of the multicomponent alloy FeCoNiB0.7Si0.3Be in as-cast and melt-quenched states (cooling rate ~10^6 K/s). X-ray analysis indicates a multiphase structure consisting of an ordered BCC B2 phase and (Fe,Ni,Co)2B intermetallics; the B2 fraction is stated to increase upon melt-quenching. This is correlated with a drop in microhardness (10400 MPa to 8900 MPa) and a rise in coercive field (5200 A/m to 17500 A/m), with the latter attributed to structure refinement and increased microstresses. The alloy is confirmed to be ferromagnetic.

Significance. If the reported phase-fraction change and its causal link to the measured property shifts can be substantiated with quantitative XRD methods and error analysis, the work would add to the literature on rapid-solidification effects in boron-containing high-entropy alloys, particularly the interplay between ordered B2 formation, hardness, and magnetic coercivity. The numerical property deltas are clearly stated, but the absence of methodological detail on phase quantification limits the strength of the central mechanistic claim.

major comments (2)
  1. [Abstract] Abstract (and any Results section describing XRD): The central claim that an increase in B2 phase fraction drives the hardness drop (10400 → 8900 MPa) and Hc rise (5200 → 17500 A/m) requires reliable quantification of phase fractions. The manuscript states only that “X-ray analysis revealed” the increase without specifying the method (Rietveld, integrated intensities, etc.), background treatment, preferred-orientation corrections, handling of peak overlaps between B2 and boride phases, or uncertainty estimates. In multiphase alloys this omission makes it impossible to judge whether the reported fraction change exceeds typical XRD uncertainty (~5–10 %) or is an artifact of fitting choices.
  2. [Abstract] Abstract (magnetic and hardness data): The attribution of the coercive-field increase to “structure refinement and an increased level of microstresses” is presented without supporting microstructural metrics (grain-size distributions, residual-strain values from XRD line broadening, or TEM) or statistical sample information. This leaves open alternative explanations such as composition segregation during quenching or measurement artifacts.

Simulated Author's Rebuttal

2 responses · 1 unresolved

We thank the referee for the constructive feedback on our study of the FeCoNiB0.7Si0.3Be alloy. We address each major comment below with point-by-point responses and indicate revisions made to strengthen the manuscript.

read point-by-point responses
  1. Referee: [Abstract] Abstract (and any Results section describing XRD): The central claim that an increase in B2 phase fraction drives the hardness drop (10400 → 8900 MPa) and Hc rise (5200 → 17500 A/m) requires reliable quantification of phase fractions. The manuscript states only that “X-ray analysis revealed” the increase without specifying the method (Rietveld, integrated intensities, etc.), background treatment, preferred-orientation corrections, handling of peak overlaps between B2 and boride phases, or uncertainty estimates. In multiphase alloys this omission makes it impossible to judge whether the reported fraction change exceeds typical XRD uncertainty (~5–10 %) or is an artifact of fitting choices.

    Authors: We agree that the original description lacked sufficient methodological detail on phase quantification. In the revised manuscript we have added a dedicated paragraph in the Results section specifying that phase fractions were determined via integrated peak intensities after background subtraction and preferred-orientation correction using the March-Dollase model. Peak overlaps were handled by full-profile fitting with the Pseudo-Voigt function. Replicate measurements on three independent samples yield an estimated B2 fraction increase of 15 ± 4 %, which exceeds the ~5 % uncertainty. These additions directly address the concern and substantiate the central claim. revision: yes

  2. Referee: [Abstract] Abstract (magnetic and hardness data): The attribution of the coercive-field increase to “structure refinement and an increased level of microstresses” is presented without supporting microstructural metrics (grain-size distributions, residual-strain values from XRD line broadening, or TEM) or statistical sample information. This leaves open alternative explanations such as composition segregation during quenching or measurement artifacts.

    Authors: We acknowledge the absence of explicit microstructural metrics in the submitted version. The revised text now includes crystallite-size and microstrain values extracted from XRD line broadening via the Williamson-Hall method, showing a reduction from ~140 nm to ~75 nm and an increase in microstrain consistent with the observed Hc rise. Hardness and magnetic data are now reported with standard deviations from five independent measurements. EDS mapping confirms compositional homogeneity, making segregation unlikely at the stated cooling rate. While we agree that TEM would provide direct visualization, it was outside the scope of the present study; the XRD-derived metrics and literature on rapid solidification support the attribution. revision: partial

standing simulated objections not resolved
  • TEM imaging to directly confirm grain-size distributions and defect densities was not performed.

Circularity Check

0 steps flagged

No circularity: purely experimental observations with no derivation chain

full rationale

The manuscript is an experimental report describing X-ray phase identification, microhardness measurements, and magnetic hysteresis data on as-cast versus melt-quenched alloy samples. No equations, first-principles derivations, parameter fitting, or predictions appear. Attributions such as 'fraction of the B2 phase increased, leading to a decrease in microhardness' are interpretive statements linking measured quantities, not reductions of one quantity to another by construction. No self-citations, ansatzes, or uniqueness theorems are invoked. The work is therefore self-contained against external benchmarks and receives the default non-circularity finding.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

No mathematical model or derivation is present; the work relies on standard experimental techniques and phase identification from X-ray diffraction patterns using known structural types.

pith-pipeline@v0.9.1-grok · 5748 in / 1330 out tokens · 29134 ms · 2026-06-27T06:06:35.810335+00:00 · methodology

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Reference graph

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