2016
DOI: 10.1073/pnas.1512127113
|View full text |Cite
|
Sign up to set email alerts
|

Dynamic X-ray diffraction observation of shocked solid iron up to 170 GPa

Abstract: Investigation of the iron phase diagram under high pressure and temperature is crucial for the determination of the composition of the cores of rocky planets and for better understanding the generation of planetary magnetic fields. Here we present X-ray diffraction results from laser-driven shock-compressed single-crystal and polycrystalline iron, indicating the presence of solid hexagonal close-packed iron up to pressure of at least 170 GPa along the principal Hugoniot, corresponding to a temperature of 4,150… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

0
15
1

Year Published

2017
2017
2023
2023

Publication Types

Select...
6
2
1

Relationship

0
9

Authors

Journals

citations
Cited by 37 publications
(16 citation statements)
references
References 47 publications
0
15
1
Order By: Relevance
“…The principle shock Hugoniot passes through those two phases before begining to melt at about 195 GPa and 4800 K, completion of melt is then at about 290 GPA and 5850 K. The gamma phase extends to a maximum pressure of 100 GPa. It has been speculated in the past that there exists a phase other than epsilon below the melt curve at higher pressures than this, but current theory [6] and experiment [58,59] do not support this and we have no such phase in our EOS. The epsilon phase has been shown through DFT studies to be the stable ground-state phase up to 7 TPa [60], where fcc, and at much higher pressure bct phases become the stable phase.…”
Section: B Resultscontrasting
confidence: 63%
“…The principle shock Hugoniot passes through those two phases before begining to melt at about 195 GPa and 4800 K, completion of melt is then at about 290 GPA and 5850 K. The gamma phase extends to a maximum pressure of 100 GPa. It has been speculated in the past that there exists a phase other than epsilon below the melt curve at higher pressures than this, but current theory [6] and experiment [58,59] do not support this and we have no such phase in our EOS. The epsilon phase has been shown through DFT studies to be the stable ground-state phase up to 7 TPa [60], where fcc, and at much higher pressure bct phases become the stable phase.…”
Section: B Resultscontrasting
confidence: 63%
“…We shocked iron up to the solid‐liquid mixed‐phase region to obtain the melting temperatures of iron according to the previous sound velocity measurements and phase diagram of iron under shock loading (Denoeud et al, 2016; Harmand et al, 2015; Nguyen & Holmes, 2004). The shock temperature ( T H ) of the mixed‐phase iron is on the melting curve ( T M ) at the Hugoniot pressure ( P H ).…”
Section: Methodsmentioning
confidence: 99%
“…Phase transition under high pressures has been attracting a great interest in condensed matter physics (Duvall and Graham, 1977;Kadau et al, 2002;Takahashi and Bassett, 1964), geophysics (Coppari et al, 2013;Shen et al, 2016), materials science (Li et al, 2014;Talonen and Hä nninen, 2007) and engineering mechanics (Guthikonda and Elliott, 2013). Recent breakthrough on the ultrafast X-ray diagnostics (Denoeud et al, 2016;Milathianaki et al, 2013) under dynamic loadings has prompted a renewed interest in phase transformation of iron from α (bcc) to ε (hcp) phase which is a prototype of martensite phase transition under high pressures. In the past thirty years, mechanical behaviors of materials exhibiting martensite phase transition have been simulated with methods at different hierarchical levels from macroscopic phenomenological models to microscopic-mechanism-based models.…”
Section: Introductionmentioning
confidence: 99%