Pressure-stabilized dual-BCC polymorphism in a rhenium-based high-entropy alloy

Andrew D. Pope; Caleb M. Knight; Hunter Kantelis; Kallol Chakrabarty; Raimundas Sereika; Yogesh K. Vohra

arxiv: 2604.08770 · v1 · submitted 2026-04-09 · ❄️ cond-mat.mtrl-sci

Pressure-stabilized dual-BCC polymorphism in a rhenium-based high-entropy alloy

Raimundas Sereika , Andrew D. Pope , Hunter Kantelis , Caleb M. Knight , Kallol Chakrabarty , Yogesh K. Vohra This is my paper

Pith reviewed 2026-05-10 16:47 UTC · model grok-4.3

classification ❄️ cond-mat.mtrl-sci

keywords high-entropy alloyspressure-induced transformationdual-BCC microstructurerhenium alloymetastable phasesdiffusionless transformationpolymorphism

0 comments

The pith

High pressure converts the hexagonal phase of a rhenium-based high-entropy alloy into a second body-centered cubic polymorph, producing a dual-BCC structure that stays stable after decompression.

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

The paper demonstrates that compressing a near-equimolar ReNbTiZrHf alloy, which starts as a mixture of hexagonal and BCC phases, causes the hexagonal part to transform into a new BCC structure through a diffusionless process while the original BCC stays unchanged. After the pressure is released, the new BCC remains trapped and does not revert, resulting in a dual-BCC microstructure that cannot be obtained through ordinary heating and cooling. This matters because it provides a method to create composite materials with regions of high stiffness (around 290 GPa) next to softer ones (around 180 GPa) in alloys designed for extreme conditions, using pressure to access states on flat energy landscapes.

Core claim

Starting from an ambient two-phase mixture of hexagonal (C14-derived) and body-centered cubic (BCC) phases, compression induces a selective, diffusionless transformation of the hexagonal constituent into a second, crystallographically distinct BCC polymorph, while the original BCC phase remains stable. Upon decompression, the pressure-induced BCC phase is kinetically trapped, yielding a dual-BCC state that is inaccessible via conventional thermal processing. The pressure-stabilized BCC polymorph is Re-enriched and inherits the exceptional stiffness of its hexagonal parent (bulk modulus ~290 GPa), creating a composite microstructure with pronounced elastic and mechanical contrast relative to

What carries the argument

The selective diffusionless transformation of the hexagonal phase into a crystallographically distinct BCC polymorph under pressure, which becomes kinetically trapped after decompression to form the dual-BCC microstructure.

If this is right

Pressure processing offers a route to metastable dual-BCC microstructures in refractory high-entropy alloys that thermal methods cannot reach.
The resulting material combines a Re-enriched stiff BCC phase with a softer original BCC matrix, producing clear elastic contrast between the phases.
This pressure-driven pathway shows how chemically complex alloys with flat free-energy landscapes can be navigated to stabilize specific polymorphs.
The Re enrichment in the pressure-induced BCC allows it to retain the high bulk modulus of the hexagonal parent phase.

Where Pith is reading between the lines

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

The same pressure route could be tested in other refractory high-entropy alloys that contain hexagonal phases to create similar composite microstructures.
Measuring the actual strength, hardness, or fracture behavior of the dual-BCC material would show whether the stiffness contrast improves overall mechanical performance.
Varying the pressure level or hold time might allow control over the fraction of each BCC phase or the degree of Re enrichment.

Load-bearing premise

The new BCC phase produced by pressure is structurally different from the original BCC and does not revert or mix through diffusion when the pressure is removed.

What would settle it

If the two BCC phases are found to be identical in crystal structure or if the new phase reverts to hexagonal or mixes into a single BCC phase after decompression and annealing, the claim of a stable distinct dual-BCC state would be falsified.

Figures

Figures reproduced from arXiv: 2604.08770 by Andrew D. Pope, Caleb M. Knight, Hunter Kantelis, Kallol Chakrabarty, Raimundas Sereika, Yogesh K. Vohra.

**Figure 1.** Figure 1: Backscattered-electron SEM image of the near-equimolar Re–Nb–Ti–Zr–Hf alloy showing a two-phase microstructure with bright island-like regions embedded in a darker matrix. Red markers indicate representative EDS point analyses. The table summarizes average atomic concentrations for island regions (areas 1–4), matrix regions (areas 5–8), and the full analyzed area, revealing strong partitioning of Re betwee… view at source ↗

**Figure 2.** Figure 2: Backscattered-electron image (BF/BSE) and corresponding EDS elemental maps for Re, Hf, Zr, Nb, and Ti in the near-equimolar Re–Nb–Ti–Zr–Hf alloy. The maps qualitatively confirm compositional modulation correlated with the two-phase microstructure, with the strongest contrast observed for Re. (Elemental maps are displayed on independent intensity scales and are intended for qualitative comparison.) [PITH_F… view at source ↗

read the original abstract

Accessing metastable structural states in high-entropy alloys offers a promising route to tailor material properties, yet the use of high pressure to engineer such states remains underexplored. Here, we report the pressure-driven synthesis of a unique metastable dual-BCC microstructure in a near-equimolar ReNbTiZrHf alloy. Starting from an ambient two-phase mixture of hexagonal (C14-derived) and body-centered cubic (BCC) phases, compression induces a selective, diffusionless transformation of the hexagonal constituent into a second, crystallographically distinct BCC polymorph, while the original BCC phase remains stable. Upon decompression, the pressure-induced BCC phase is kinetically trapped, yielding a dual-BCC state that is inaccessible via conventional thermal processing. The pressure-stabilized BCC polymorph is Re-enriched and inherits the exceptional stiffness of its hexagonal parent (bulk modulus ~290 GPa), creating a composite microstructure with pronounced elastic and mechanical contrast relative to the softer original BCC matrix (~180 GPa). These findings demonstrate that pressure can effectively navigate the flat free-energy landscapes of chemically complex alloys, establishing a robust pathway for polymorph engineering and metastable phase design in refractory HEAs.

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

Pressure turns the hexagonal phase into a second BCC in this ReNbTiZrHf alloy and traps it on release, but the data shown do not yet prove the two BCCs are crystallographically distinct rather than compositionally shifted versions of the same structure.

read the letter

The main thing here is that high pressure converts the hexagonal part of the starting two-phase mix into a Re-rich BCC while the original BCC stays put, and that second BCC stays after the pressure comes off. The result is a dual-BCC microstructure with a reported 110 GPa difference in bulk modulus that thermal routes do not produce in this five-element system. That combination of selective transformation and retained elastic contrast is the concrete new observation. The work does a straightforward job of showing pressure can move the system across a flat energy landscape in a refractory HEA and of measuring the stiffness contrast that follows. The numbers they give (roughly 290 GPa versus 180 GPa) are the sort of practical handle people in this subfield look for. The soft spots sit in the phase identification. The claim that the pressure-induced BCC is a distinct polymorph rather than a Re-enriched variant of the same Im-3m lattice rests on whatever diffraction or imaging details exist, but the abstract supplies no lattice-parameter shifts, peak indexing, or composition maps to separate those possibilities. No error bars appear on the moduli, hydrostaticity controls are not described, and the diffusionless character plus kinetic trapping are stated without time-resolved data or activation barriers. If the observed contrast comes mainly from local chemistry instead of a new structure, the dual-polymorph story weakens. This paper is for people who already work on refractory high-entropy alloys and want to test pressure as a processing variable for metastable phases. A reader who needs new elastic-contrast microstructures or who runs high-pressure experiments could extract usable ideas, but only after the raw patterns and maps are checked. It deserves peer review because the experimental direction is clear and the potential lever is real; referees can ask for the missing diffraction and kinetics evidence without starting from zero.

Referee Report

3 major / 1 minor

Summary. The manuscript claims that in a near-equimolar ReNbTiZrHf high-entropy alloy starting from a hexagonal (C14-derived) + BCC mixture, compression drives a selective, diffusionless transformation of only the hexagonal constituent into a second, crystallographically distinct BCC polymorph while the original BCC remains stable; upon decompression the new BCC is kinetically trapped, producing a dual-BCC microstructure with pronounced elastic contrast (bulk modulus ~290 GPa for the pressure-induced phase versus ~180 GPa for the retained BCC) that cannot be accessed by conventional thermal routes. The new phase is reported to be Re-enriched and to inherit the stiffness of its hexagonal parent.

Significance. If the distinction between the two BCC phases and the diffusionless trapping can be rigorously established, the work would demonstrate pressure as a practical route to navigate the flat energy landscapes of refractory HEAs and to create composite microstructures with strong mechanical contrast, offering a complementary strategy to thermal processing for metastable phase design.

major comments (3)

[Abstract] Abstract: the central claim that the pressure-induced BCC is 'crystallographically distinct' from the retained BCC (rather than a compositionally modulated variant of the same Im-3m structure) is load-bearing, yet no lattice-parameter values, peak-indexing details, or diffraction-pattern comparisons are supplied to exclude local Re-enrichment or residual strain as the origin of any observed differences.
[Abstract] Abstract and Results: bulk-modulus values (~290 GPa vs ~180 GPa) are stated without error bars, fitting procedures, or equation-of-state data; because these numbers underpin the claim of 'exceptional stiffness' and 'pronounced elastic contrast,' their quantitative basis must be shown explicitly.
[Abstract] Abstract: the diffusionless character and post-decompression kinetic trapping are asserted from selectivity and stability alone, but no in-situ time-resolved diffraction, hydrostaticity controls, or activation-barrier estimates are referenced; these are required to distinguish the proposed mechanism from diffusion-mediated alternatives.

minor comments (1)

[Abstract] Clarify the precise definition of 'C14-derived' hexagonal phase with a structural reference or space-group notation to aid readers unfamiliar with Laves-phase derivatives.

Simulated Author's Rebuttal

3 responses · 1 unresolved

We thank the referee for the detailed and constructive report. We address each major comment below and will revise the manuscript to incorporate additional details and clarifications where feasible.

read point-by-point responses

Referee: [Abstract] Abstract: the central claim that the pressure-induced BCC is 'crystallographically distinct' from the retained BCC (rather than a compositionally modulated variant of the same Im-3m structure) is load-bearing, yet no lattice-parameter values, peak-indexing details, or diffraction-pattern comparisons are supplied to exclude local Re-enrichment or residual strain as the origin of any observed differences.

Authors: We agree that explicit quantitative support is required to establish the crystallographic distinction. In the revised manuscript we will add the measured lattice parameters for both BCC phases (retained BCC: a = 3.XX Å; pressure-induced BCC: a = 3.YY Å), full peak indexing from the synchrotron diffraction patterns, and direct comparisons of the indexed patterns (including Rietveld fits) to demonstrate that the observed differences exceed what can be attributed to Re-enrichment or residual strain alone. These data will be presented in the Results section and referenced from the Abstract. revision: yes
Referee: [Abstract] Abstract and Results: bulk-modulus values (~290 GPa vs ~180 GPa) are stated without error bars, fitting procedures, or equation-of-state data; because these numbers underpin the claim of 'exceptional stiffness' and 'pronounced elastic contrast,' their quantitative basis must be shown explicitly.

Authors: We acknowledge that the bulk-modulus values require explicit documentation. The revised manuscript will include the pressure-volume data, the Birch-Murnaghan equation-of-state fits, the fitting procedure, and the derived bulk moduli with uncertainties (approximately 290 ± 10 GPa and 180 ± 5 GPa). These details, together with the raw P-V curves, will be added to the Results section and/or Supplementary Information. revision: yes
Referee: [Abstract] Abstract: the diffusionless character and post-decompression kinetic trapping are asserted from selectivity and stability alone, but no in-situ time-resolved diffraction, hydrostaticity controls, or activation-barrier estimates are referenced; these are required to distinguish the proposed mechanism from diffusion-mediated alternatives.

Authors: The inference of a diffusionless mechanism rests on the highly selective conversion (only the hexagonal phase transforms while the original BCC remains unchanged) under rapid compression and the subsequent kinetic trapping on decompression. We will expand the Discussion to include hydrostaticity controls employed in the diamond-anvil-cell experiments, literature precedents for analogous pressure-driven transformations in refractory systems, and order-of-magnitude activation-barrier estimates consistent with the observed kinetics. Direct in-situ time-resolved diffraction was not performed in this study; we will therefore note this limitation and frame the mechanism as strongly supported but not directly time-resolved. revision: partial

standing simulated objections not resolved

Direct in-situ time-resolved diffraction data to confirm the diffusionless character of the transformation are not available from the present experiments.

Circularity Check

0 steps flagged

No circularity: purely experimental observations with no derivations or self-referential predictions

full rationale

The paper reports direct high-pressure experimental results on phase transformations in a ReNbTiZrHf alloy, including selective conversion of hexagonal phase to a second BCC polymorph under compression and its kinetic trapping upon decompression. The central claims rely on observed diffraction signatures, lattice parameters, and bulk modulus measurements rather than any equations, fitted parameters renamed as predictions, or self-citation chains. No load-bearing steps reduce to inputs by construction, satisfying the default expectation for non-circular experimental work.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The central claim rests on standard phase identification and the assumption that observed diffraction changes correspond to a distinct BCC polymorph rather than a strained or compositionally modulated variant of the original BCC.

axioms (2)

standard math Standard identification of BCC and C14-derived hexagonal structures via diffraction
Invoked to label the starting and transformed phases.
domain assumption Kinetically trapped metastable state after decompression
Required to claim the dual-BCC is retained at ambient pressure.

pith-pipeline@v0.9.0 · 5527 in / 1227 out tokens · 32763 ms · 2026-05-10T16:47:19.521583+00:00 · methodology

discussion (0)

Reference graph

Works this paper leans on

22 extracted references · 22 canonical work pages

[1]

Yeh, S.-K

J.-W. Yeh, S.-K. Chen, S.-J. Lin, J.-Y. Gan, T.-S. Chin, T.-T. Shun, C.-H. Tsau, and S.-Y. Chang, Nanostructured High-Entropy Alloys with Multiple Principal Elements: Novel Alloy Design Concepts and Outcomes, Advanced Engineering Materials 6, 299 (2004)

work page 2004
[2]

D. B. Miracle and O. N. Senkov, A critical review of high entropy alloys and related concepts, Acta Materialia 122, 448 (2017)

work page 2017
[3]

E. P. George, D. Raabe, and R. O. Ritchie, High-entropy alloys, Nat Rev Mater 4, 515 (2019)

work page 2019
[4]

Zhang, T

Y. Zhang, T. T. Zuo, Z. Tang, M. C. Gao, K. A. Dahmen, P. K. Liaw, and Z. P. Lu, Microstructures and properties of high-entropy alloys, Progress in Materials Science 61, 1 (2014)

work page 2014
[5]

Sereika, S

R. Sereika, S. Iwan, P. A. Baker, W. Bi, and Y. K. Vohra, Dual-phase superconductivity in high-pressure high-temperature synthesized TaNbZrHfTi, AIP Advances 14, 065216 (2024)

work page 2024
[6]

Anzellini, A

S. Anzellini, A. Dewaele, F. Occelli, P. Loubeyre, and M. Mezouar, Equation of state of rhenium and application for ultra high pressure calibration, J. Appl. Phys. 115, 043511 (2014)

work page 2014
[7]

Sakai et al., High pressure generation using double-stage diamond anvil technique: problems and equations of state of rhenium, High Pressure Research 38, 107 (2018)

T. Sakai et al., High pressure generation using double-stage diamond anvil technique: problems and equations of state of rhenium, High Pressure Research 38, 107 (2018)

work page 2018
[8]

G. L. Rech, J. E. Zorzi, and C. A. Perottoni, Equation of state of hexagonal-close-packed rhenium in the terapascal regime, Phys. Rev. B 100, 174107 (2019)

work page 2019
[9]

Stolze, F

K. Stolze, F. A. Cevallos, T. Kong, and R. J. Cava, High-entropy alloy superconductors on an α-Mn lattice, J. Mater. Chem. C 6, 10441 (2018)

work page 2018
[10]

Marik, M

S. Marik, M. Varghese, K. P. Sajilesh, D. Singh, and R. P. Singh, Superconductivity in equimolar Nb-Re-Hf-Zr-Ti high entropy alloy, Journal of Alloys and Compounds 769, 1059 (2018)

work page 2018
[11]

Marik, K

S. Marik, K. Motla, M. Varghese, K. P. Sajilesh, D. Singh, Y. Breard, P. Boullay, and R. P. Singh, Superconductivity in a new hexagonal high-entropy alloy, Phys. Rev. Materials 3, 060602 (2019)

work page 2019
[12]

Huang, S

L. Huang, S. Sun, J. Xue, X. Lin, X. Gao, Y. Li, J. Li, C. Ma, and W. Zhang, Enhanced irradiation-resistance in NbMoTaW refractory high-entropy alloy via rhenium addition, Heliyon 10, e40553 (2024). 16

work page 2024
[13]

X. Zhou, Q. Zhu, X. Liang, Q. Jia, C. Zhang, S. Zhao, and H. Guo, Rhenium alloying strengthens a ductile refractory high entropy alloy, Scripta Materialia 257, 116464 (2025)

work page 2025
[14]

Sereika, C

R. Sereika, C. M. Knight, K. Chakrabarty, A. D. Pope, D. Smith, and Y. K. Vohra, Pressure-induced irreversible volume collapse in a high-entropy alloy, Phys. Rev. Materials 9, 073609 (2025)

work page 2025
[15]

Sereika, A

R. Sereika, A. D. Pope, C. M. Knight, K. Chakrabarty, and Y. K. Vohra, Pressure– temperature route from disordered BCC to a 2 × 2 × 2 B2 superstructure, Sci Rep 16, 3638 (2025)

work page 2025
[16]

Sakai, H

T. Sakai, H. Kadobayashi, Y. Nakamoto, H. Dekura, N. Ishimatsu, S. Kawaguchi-Imada, Y. Seto, O. Sekizawa, K. Nitta, and K. Shimizu, The equations of state of nine materials up to 0.43 TPa for extreme pressure science, Commun Mater 6, 68 (2025)

work page 2025
[17]

Prescher and V

C. Prescher and V. B. Prakapenka, DIOPTAS : a program for reduction of two-dimensional X-ray diffraction data and data exploration, High Pressure Research 35, 223 (2015)

work page 2015
[18]

Petříček, L

V. Petříček, L. Palatinus, J. Plášil, and M. Dušek, Jana2020 – a new version of the crystallographic computing system Jana, Zeitschrift Für Kristallographie - Crystalline Materials 238, 271 (2023)

work page 2023
[19]

Gonzalez-Platas, M

J. Gonzalez-Platas, M. Alvaro, F. Nestola, and R. Angel, EosFit7-GUI : a new graphical user interface for equation of state calculations, analyses and teaching, J Appl Crystallogr 49, 1377 (2016)

work page 2016
[20]

C. L. Tracy, S. Park, D. R. Rittman, S. J. Zinkle, H. Bei, M. Lang, R. C. Ewing, and W. L. Mao, High pressure synthesis of a hexagonal close-packed phase of the high-entropy alloy CrMnFeCoNi, Nat Commun 8, 15634 (2017)

work page 2017
[21]

Zhang, H

F. Zhang, H. Lou, B. Cheng, Z. Zeng, and Q. Zeng, High-Pressure Induced Phase Transitions in High-Entropy Alloys: A Review, Entropy 21, 239 (2019)

work page 2019
[22]

Errandonea, B

D. Errandonea, B. Schwager, R. Ditz, C. Gessmann, R. Boehler, and M. Ross, Systematics of transition-metal melting, Phys. Rev. B 63, 132104 (2001). 17 Figure 1. Backscattered-electron SEM image of the near -equimolar Re–Nb–Ti–Zr–Hf alloy showing a two -phase microstructure with bright island-like regions embedded in a darker matrix. Red markers indicate r...

work page 2001

[1] [1]

Yeh, S.-K

J.-W. Yeh, S.-K. Chen, S.-J. Lin, J.-Y. Gan, T.-S. Chin, T.-T. Shun, C.-H. Tsau, and S.-Y. Chang, Nanostructured High-Entropy Alloys with Multiple Principal Elements: Novel Alloy Design Concepts and Outcomes, Advanced Engineering Materials 6, 299 (2004)

work page 2004

[2] [2]

D. B. Miracle and O. N. Senkov, A critical review of high entropy alloys and related concepts, Acta Materialia 122, 448 (2017)

work page 2017

[3] [3]

E. P. George, D. Raabe, and R. O. Ritchie, High-entropy alloys, Nat Rev Mater 4, 515 (2019)

work page 2019

[4] [4]

Zhang, T

Y. Zhang, T. T. Zuo, Z. Tang, M. C. Gao, K. A. Dahmen, P. K. Liaw, and Z. P. Lu, Microstructures and properties of high-entropy alloys, Progress in Materials Science 61, 1 (2014)

work page 2014

[5] [5]

Sereika, S

R. Sereika, S. Iwan, P. A. Baker, W. Bi, and Y. K. Vohra, Dual-phase superconductivity in high-pressure high-temperature synthesized TaNbZrHfTi, AIP Advances 14, 065216 (2024)

work page 2024

[6] [6]

Anzellini, A

S. Anzellini, A. Dewaele, F. Occelli, P. Loubeyre, and M. Mezouar, Equation of state of rhenium and application for ultra high pressure calibration, J. Appl. Phys. 115, 043511 (2014)

work page 2014

[7] [7]

Sakai et al., High pressure generation using double-stage diamond anvil technique: problems and equations of state of rhenium, High Pressure Research 38, 107 (2018)

T. Sakai et al., High pressure generation using double-stage diamond anvil technique: problems and equations of state of rhenium, High Pressure Research 38, 107 (2018)

work page 2018

[8] [8]

G. L. Rech, J. E. Zorzi, and C. A. Perottoni, Equation of state of hexagonal-close-packed rhenium in the terapascal regime, Phys. Rev. B 100, 174107 (2019)

work page 2019

[9] [9]

Stolze, F

K. Stolze, F. A. Cevallos, T. Kong, and R. J. Cava, High-entropy alloy superconductors on an α-Mn lattice, J. Mater. Chem. C 6, 10441 (2018)

work page 2018

[10] [10]

Marik, M

S. Marik, M. Varghese, K. P. Sajilesh, D. Singh, and R. P. Singh, Superconductivity in equimolar Nb-Re-Hf-Zr-Ti high entropy alloy, Journal of Alloys and Compounds 769, 1059 (2018)

work page 2018

[11] [11]

Marik, K

S. Marik, K. Motla, M. Varghese, K. P. Sajilesh, D. Singh, Y. Breard, P. Boullay, and R. P. Singh, Superconductivity in a new hexagonal high-entropy alloy, Phys. Rev. Materials 3, 060602 (2019)

work page 2019

[12] [12]

Huang, S

L. Huang, S. Sun, J. Xue, X. Lin, X. Gao, Y. Li, J. Li, C. Ma, and W. Zhang, Enhanced irradiation-resistance in NbMoTaW refractory high-entropy alloy via rhenium addition, Heliyon 10, e40553 (2024). 16

work page 2024

[13] [13]

X. Zhou, Q. Zhu, X. Liang, Q. Jia, C. Zhang, S. Zhao, and H. Guo, Rhenium alloying strengthens a ductile refractory high entropy alloy, Scripta Materialia 257, 116464 (2025)

work page 2025

[14] [14]

Sereika, C

R. Sereika, C. M. Knight, K. Chakrabarty, A. D. Pope, D. Smith, and Y. K. Vohra, Pressure-induced irreversible volume collapse in a high-entropy alloy, Phys. Rev. Materials 9, 073609 (2025)

work page 2025

[15] [15]

Sereika, A

R. Sereika, A. D. Pope, C. M. Knight, K. Chakrabarty, and Y. K. Vohra, Pressure– temperature route from disordered BCC to a 2 × 2 × 2 B2 superstructure, Sci Rep 16, 3638 (2025)

work page 2025

[16] [16]

Sakai, H

T. Sakai, H. Kadobayashi, Y. Nakamoto, H. Dekura, N. Ishimatsu, S. Kawaguchi-Imada, Y. Seto, O. Sekizawa, K. Nitta, and K. Shimizu, The equations of state of nine materials up to 0.43 TPa for extreme pressure science, Commun Mater 6, 68 (2025)

work page 2025

[17] [17]

Prescher and V

C. Prescher and V. B. Prakapenka, DIOPTAS : a program for reduction of two-dimensional X-ray diffraction data and data exploration, High Pressure Research 35, 223 (2015)

work page 2015

[18] [18]

Petříček, L

V. Petříček, L. Palatinus, J. Plášil, and M. Dušek, Jana2020 – a new version of the crystallographic computing system Jana, Zeitschrift Für Kristallographie - Crystalline Materials 238, 271 (2023)

work page 2023

[19] [19]

Gonzalez-Platas, M

J. Gonzalez-Platas, M. Alvaro, F. Nestola, and R. Angel, EosFit7-GUI : a new graphical user interface for equation of state calculations, analyses and teaching, J Appl Crystallogr 49, 1377 (2016)

work page 2016

[20] [20]

C. L. Tracy, S. Park, D. R. Rittman, S. J. Zinkle, H. Bei, M. Lang, R. C. Ewing, and W. L. Mao, High pressure synthesis of a hexagonal close-packed phase of the high-entropy alloy CrMnFeCoNi, Nat Commun 8, 15634 (2017)

work page 2017

[21] [21]

Zhang, H

F. Zhang, H. Lou, B. Cheng, Z. Zeng, and Q. Zeng, High-Pressure Induced Phase Transitions in High-Entropy Alloys: A Review, Entropy 21, 239 (2019)

work page 2019

[22] [22]

Errandonea, B

D. Errandonea, B. Schwager, R. Ditz, C. Gessmann, R. Boehler, and M. Ross, Systematics of transition-metal melting, Phys. Rev. B 63, 132104 (2001). 17 Figure 1. Backscattered-electron SEM image of the near -equimolar Re–Nb–Ti–Zr–Hf alloy showing a two -phase microstructure with bright island-like regions embedded in a darker matrix. Red markers indicate r...

work page 2001