Liquid–liquid critical point

A liquid–liquid critical point (or LLCP) is the endpoint of a liquid–liquid phase transition line (LLPT); it is a critical point where two types of local structures coexist at the exact ratio of unity. This hypothesis was first developed by Peter Poole, Francesco Sciortino, Uli Essmann and H. Eugene Stanley in Boston^[1] to obtain a quantitative understanding of the huge number of anomalies present in water.^[2]

Near a liquid–liquid critical point, there is always a competition between two alternative local structures. For instance, in supercooled water, two types of local structures have been predicted: a low-density local configuration (LD) and a high-density local configuration (HD), so above the critical pressure, the liquid is composed by a majority of HD local structure, while below the critical pressure a higher fraction of LD local configurations is present. The ratio between HD and LD configurations is determined according to the thermodynamic equilibrium of the system, which is often governed by external variables such as pressure and temperature.^[3]

The liquid–liquid critical point theory can be applied to several liquids that possess the tetrahedral symmetry. The study of liquid–liquid critical points is an active research area with hundreds of articles having been published, though only a few of these investigations have been experimental^{[4][5][6][7][8][9]} since most modern probing techniques are not fast and/or sensitive enough to study them.

References

1. Poole, P. H.; Sciortino, F.; Essmann, U.; Stanley, H. E. (1992). "Phase Behavior of Metastable Water". Nature. 360 (6402): 324–328. Bibcode:1992Natur.360..324P. doi:10.1038/360324a0. S2CID 4302774.
2. "Anomalous properties of water". Retrieved 30 August 2015.
3. Holten, V.; Palmer, J. C.; Poole, P. H.; Debenedetti, P. G.; Anisimov, M. A. (2014). "Two-state thermodynamics of the ST2 model for supercooled water". J. Chem. Phys. 140 (10): 104502. arXiv:1312.4871. Bibcode:2014JChPh.140b4502M. doi:10.1063/1.4867287. PMID 24628177. S2CID 18158514.
4. Mishima, O.; Stanley, H. E. (1998). "Decompression-Induced Melting of Ice IV and the Liquid–Liquid Transition in Water". Nature. 392 (6672): 164–168. Bibcode:1998Natur.392..164M. doi:10.1038/32386. S2CID 4388755.
5. Vasisht, V. V.; Saw, S.; Sastry, S. (2011). "Liquid–Liquid Critical Point in Supercooled Silicon". Nat. Phys. 7 (7): 549–555. arXiv:1103.3473. Bibcode:2011NatPh...7..549V. doi:10.1038/nphys1993. S2CID 118861818.
6. Katayama, Y.; Mizutani, T.; Utsumi, W.; Shimomura, O.; Yamakata, M.; Funakoshi, K. (2000). "A First-Order Liquid–Liquid Phase Transition in Phosphorus". Nature. 403 (6766): 170–173. Bibcode:2000Natur.403..170K. doi:10.1038/35003143. PMID 10646596. S2CID 4395377.
7. Cadien, A.; Hu, Q. Y.; Meng, Y.; Cheng, Y. Q.; Chen, M. W.; Shu, J. F.; Mao, H. K.; Sheng, H. W. (2013). "First-Order Liquid–Liquid Phase Transition in Cerium". Phys. Rev. Lett. 110 (12): 125503. Bibcode:2013PhRvL.110l5503C. doi:10.1103/PhysRevLett.110.125503. PMID 25166820.
8. Yen, F.; Chi, Z. H.; Berlie, A.; Liu, X. D.; Goncharov, A. F. (2015). "Dielectric Anomalies in Crystalline Ice: Indirect Evidence of the Existence of a Liquid−Liquid Critical Point in H₂O". J. Phys. Chem. C. 119 (35): 20618–20622. arXiv:1501.02380. doi:10.1021/acs.jpcc.5b07635. S2CID 102225912.
9. Gomes, Gabriel O.; Stanley, H. Eugene; Souza, Mariano de (2019-08-19). "Enhanced Grüneisen Parameter in Supercooled Water". Scientific Reports. 9 (1): 12006. arXiv:1808.00536. Bibcode:2019NatSR...912006O. doi:10.1038/s41598-019-48353-4. ISSN 2045-2322. PMC 6700159. PMID 31427698.