New metastable ice phases via supercooled water

Water exhibits rich polymorphism, where more than 20 crystalline phases have been experimentally reported. Five of them are metastable and form at low temperatures by either heating amorphous ice or degassing clathrate hydrates. However, such metastable phases rarely crystallise directly from liquid water, making it challenging to study metastable phase relations at relatively high temperatures. Here, we report that high-pressure metastable phases of ice, including two unknown phases named ices XXI and XXII, crystallise directly from liquid water in a deeply supercooled region around the homogeneous nucleation temperature. The key is to use emulsified water to stabilise supercooled water in laboratory timescales. Ices XXI and XXII are obtained by isothermal compression of emulsified water at 295 K and 250 K, respectively. Our powder x-ray and neutron diffraction analyses combined with molecular dynamics (MD) simulations revealed the surprisingly complex structures of these new phases with Z = 152 (ice XXI) and 304 (ice XXII). Ice XXI is topologically identical to 'ice T2' previously predicted by MD simulations, and our experimental structural model can be used as a benchmark for its structures in simulations, which depend on the force fields. On cooling, ice XXI transforms into an orientationally ordered counterpart named ice XXIII. Our results revealed the "hidden" structural complexity of water underlying the phase diagram, as implied by previous computational works. Further efforts at unveiling such metastable phase relations will bridge the large gaps between computational and experimental phase diagrams of water.

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Publication Details

Journal
ArXiv.org
Published
2025-07-18
Citations
1
Primary Topic
Material Dynamics and Properties
Type
article
Field-Weighted Citation Impact
0.52
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article

New metastable ice phases via supercooled water

Misaki Sato, Kenji Mochizuki, Kunio Hirata, Hiroyuki Kagi et al.
1 citations
ArXiv.org
Material Dynamics and Properties
0.52
article

New metastable ice phases via supercooled water

Misaki Sato, Kenji Mochizuki, Kunio Hirata, Hiroyuki Kagi, Qianli Xue, Koji Yonekura, Saori Maki-Yonekura, Kiyofumi Takaba, Koichi Momma, Kazuki Komatsu, Hiroki Kobayashi, Takanori Hattori, Yoshiaki Kawano, Shinichi Machida, Hayate Ito
article en
1 citations

Abstract

Water exhibits rich polymorphism, where more than 20 crystalline phases have been experimentally reported. Five of them are metastable and form at low temperatures by either heating amorphous ice or degassing clathrate hydrates. However, such metastable phases rarely crystallise directly from liquid water, making it challenging to study metastable phase relations at relatively high temperatures. Here, we report that high-pressure metastable phases of ice, including two unknown phases named ices XXI and XXII, crystallise directly from liquid water in a deeply supercooled region around the homogeneous nucleation temperature. The key is to use emulsified water to stabilise supercooled water in laboratory timescales. Ices XXI and XXII are obtained by isothermal compression of emulsified water at 295 K and 250 K, respectively. Our powder x-ray and neutron diffraction analyses combined with molecular dynamics (MD) simulations revealed the surprisingly complex structures of these new phases with Z = 152 (ice XXI) and 304 (ice XXII). Ice XXI is topologically identical to 'ice T2' previously predicted by MD simulations, and our experimental structural model can be used as a benchmark for its structures in simulations, which depend on the force fields. On cooling, ice XXI transforms into an orientationally ordered counterpart named ice XXIII. Our results revealed the "hidden" structural complexity of water underlying the phase diagram, as implied by previous computational works. Further efforts at unveiling such metastable phase relations will bridge the large gaps between computational and experimental phase diagrams of water.

ArXiv.org
Openalex Percentile: Top 29%
Material Dynamics and Properties
0.52
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