Glass polymorphism in TIP4P/2005 water: A description based on the potential energy landscape formalism

被引:25
|
作者
Handle, Philip H. [1 ]
Sciortino, Francesco [2 ]
Giovambattista, Nicolas [3 ,4 ,5 ]
机构
[1] Univ Innsbruck, Inst Phys Chem, Innrain 52c, A-6020 Innsbruck, Austria
[2] Sapienza Univ Rome, Dept Phys, Piazzale Aldo Moro 5, I-00185 Rome, Italy
[3] CUNY Brooklyn Coll, Dept Phys, New York, NY 10016 USA
[4] CUNY, Grad Ctr, PhD Program Chem, New York, NY 10016 USA
[5] CUNY, Grad Ctr, PhD Program Phys, New York, NY 10016 USA
来源
JOURNAL OF CHEMICAL PHYSICS | 2019年 / 150卷 / 24期
基金
美国国家科学基金会; 奥地利科学基金会;
关键词
DENSITY AMORPHOUS ICE; X-RAY-DIFFRACTION; PURE LIQUID WATER; CONFIGURATIONAL ENTROPY; INDUCED AMORPHIZATION; 1ST-ORDER TRANSITION; SUPERCOOLED LIQUIDS; RELAXATION-TIME; DYNAMICS; MODEL;
D O I
10.1063/1.5100346
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
The potential energy landscape (PEL) formalism is a statistical mechanical approach to describe supercooled liquids and glasses. Here, we use the PEL formalism to study the pressure-induced transformations between low-density amorphous ice (LDA) and high-density amorphous ice (HDA) using computer simulations of the TIP4P/2005 molecular model of water. We find that the properties of the PEL sampled by the system during the LDA-HDA transformation exhibit anomalous behavior. In particular, at conditions where the change in density during the LDA-HDA transformation is approximately discontinuous, reminiscent of a first-order phase transition, we find that (i) the inherent structure (IS) energy, e(IS)(V), is a concave function of the volume and (ii) the IS pressure, P-IS(V), exhibits a van der Waals-like loop. In addition, the curvature of the PEL at the IS is anomalous, a nonmonotonic function of V. In agreement with previous studies, our work suggests that conditions (i) and (ii) are necessary (but not sufficient) signatures of the PEL for the LDA-HDA transformation to be reminiscent of a first-order phase transition. We also find that one can identify two different regions of the PEL, one associated with LDA and another with HDA. Our computer simulations are performed using a wide range of compression/decompression and cooling rates. In particular, our slowest cooling rate (0.01 K/ns) is within the experimental rates employed in hyperquenching experiments to produce LDA. Interestingly, the LDA-HDA transformation pressure that we obtain at T = 80 K and at different rates extrapolates remarkably well to the corresponding experimental pressure. Published under license by AIP Publishing.
引用
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页数:14
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