Unusual phase behavior in one- Unusual phase behavior in one- component component system with isotropic interaction system with isotropic interaction Limei Xu Limei Xu WPI-AIMR, Tohoku WPI-AIMR, Tohoku University, Japan University, Japan In collaboration with: C. A. Angell Arizona State University S. V. Buldyrev Yeshiva University S.-H. Chen MIT N. Giovambattista New York Brookline college F. Sciortino University of Rome
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Unusual phase behavior in one-component system with isotropic interaction Limei Xu WPI-AIMR, Tohoku University, Japan WPI-AIMR, Tohoku University, Japan.
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Unusual phase behavior in one-Unusual phase behavior in one-componentcomponent
system with isotropic interaction system with isotropic interactionLimei Xu Limei Xu
WPI-AIMR, Tohoku University, JapanWPI-AIMR, Tohoku University, Japan
In collaboration with: C. A. Angell Arizona State UniversityS. V. Buldyrev Yeshiva UniversityS.-H. Chen MITN. Giovambattista New York Brookline collegeF. Sciortino University of RomeH. E. Stanley Boston University
Similar phase behaviors shared by very different materials:
Liquid-liquid phase transition: Tetrahedrally structured systems: water, Si, Ge, SiO2, BeF2 Metallic system: such as Y3Al5O12
Polyamorphism (amorphous-amorphous transition under pressure)
Tetrahedrally structured systems: water, Ge Metallic system: Ce55Al45
Motivation
Common feature: involving two local structures, with one having larger open spaces between particles that collapse under pressure.
Question: Universal model that determine whether these features and phenomena are related or exist independently
OutlineOutline
Understand water anomalies with isotropic potential
Liquid-liquid transition and polyamorphism (glass-glass)
Fractional Stokes-Einstein Relation and its structural origin
has importance as a solvent of solutes, such as chemical reactants and bio-molecules (proteins)
prototype of anomalous liquids, relevance to other liquids, such as Silicon, Silica
Why do we care about water?Why do we care about water?
P. G. Debenedetti, J. Phys.: Condens. Matter 15, R1669 (2003)
<(V)2>=VkBTT <(S)2>=N kB Cp
Anomalous Properties of Water Anomalous Properties of Water
Density Compressibility Specific Heat
Anomalous thermodynamic properties of supercooled bulk waterAnomalous thermodynamic properties of supercooled bulk water
C. A. Angell et al., J. Phys. Chem. 77, 3092 (1973)
TS=228K
319K
308K
R. J. Speedy et al. J. Chem. Phys. 65, 851 (1976)
Cp and KT diverge upon approaching T=228K?
Anomalous behavior is more pronounced in deep supercooled region
Phases of liquid waterPhases of liquid water
Courtesy of Dr. O. Mishima HypothesisHypothesis
Poole et al., Nature (1992)Poole et al., Nature (1992)
Tc=215K , Pc=100MPa
Experimental results in confined nanopores at 1 barExperimental results in confined nanopores at 1 bar
Specific Heat
S. Maruyama, K. Wakabayashi, M. Oguni, AIP conference proceedings 708, 675 (2004)
T=227K
Cp shows a peak at 227K, instead of diverges upon approaching T=228K
Self Diffusion
Mallamace et al, J. Chem. Phys. 124, 161102 (2006)
Diffusion coefficient shows a kink
How to interpret the experimental results– dynamic crossover and response function maximum?
Related to a hypothesized liquid-liquid critical point?
If yes, how to locate this critical point in water?
What are the questions?What are the questions?
E. A. Jagla, J. Chem. Phys. 111, 8980 (1999)Xu et. al, PNAS (2005); PRE(2006)
MD simulationNumber of particles: N=1728
Two-scale ramp modelTwo-scale ramp model
Effective potential of water at T=280K
T. Head-Gordon and F. H. Stilinger. J. Chem. Phys. 98, 3313 (1993)
U( r ) ~ ln g ( r )
Stable liquid-liquid critical point (LLCP)
Density anomaly (TMD)
Phase diagramPhase diagram
L. Xu, S. V. Buldyrev, C. A. Angell, H. E. Stanley, Phys. Rev. E (2006); JC(2009)
Changes in response functions: Specific heat Changes in response functions: Specific heat
P>Pc : CP has maxima Anomaly occurs upon crossing the Widom line ( Cpmax )
P<Pc : CP increase monotonically, No anomalous behaviour!
CPmax
HDL
Pc =0.24
How to effectively trace liquid-liquid critical point: not upon crossing coexistence line, but the Widom line the Widom line terminates at the Liquid-liquid critical point
Changes in diffusivityChanges in diffusivity
CPmax
How to trace LL critical point using dynamic properties?
Appearance or disappearance of a kink in diffusivity
Pc =0.24
L. Xu, S. V. Buldyrev, C. A. Angell, H. E. Stanley, Phys. Rev. E (2006); PNAS(2005)
Experimentally locating the Liquid-liquid critical pointExperimentally locating the Liquid-liquid critical point
The Widom line terminates at the liquid-liquid critical point
Self Diffusion
Specific Heat
L. Liu et al., Phys. Rev. Lett. (2005)
Tw
Conclusion IConclusion I
The two-scale model can reproduce water-like anomalies
Thermodynamic and dynamic quantities shows changes upon crossing the Widom line, not upon crossing the coexistence line
Provide a way for experiments to locate the possible existence of liquid-liquid critical point
Maybe not hydrogen bond, not tetrahedral local structure, but the two-scale matters for water-like anomalies?
OutlineOutline
Understand water anomalies with isotropic potential
Liquid-liquid transition and polyamorphism (glass-glass)
Fractional Stokes-Einstein Relation and its structural origin
Two glass states obtained upon cooling LDL LDA HDL HDA
Two glass states upon cooling: HDA and LDA
L. Xu, S. V. Buldyrev, N. Giovambattista, C. A. Angell, H. E. Stanley, JCP (2009)
L. Xu, S. V. Buldyrev, N. Giovambattista, C. A. Angell H. E. Stanley, JCP (2009)
H=U+PV
Detection of glass transition: thermal expansion and specific heatThe second approach is more pronounced, indicating that: Glass transition is the onset of the kinetics, while liquid-liquid Phase transition is the onset of the volume/density change
HDL-HDA glass transition and liquid-liquid phase transition
L. Xu, S. V. Buldyrev, H. E. Stanley, M. Tokuyama (in preparition)
HDA is stable at low pressure upon decompression
Polyamorphism
Stability of liquid-liquid critical point and polyamorphism
Appearance of Fractional Stokes-Einstein relation is at Tx >> Tw
No effect is observed at Tw!!
Structural changes upon cooling Structural changes upon cooling (Simulation)(Simulation)
Tx occurs at the appearance of a new species
Tw is related to the maximal change of the structure
Structural information: IRStructural information: IR
F. Mallamace et.al, PNAS (2007)
Structural changes upon cooling Structural changes upon cooling (Experiment)(Experiment)
Tx occurs at the appearance of a new species
Tw is related to the maximal change of the structure
L. Xu, F. Mallamce, Z. Yan, F. W. Starr, S. V. Buldyrev, H. E. Stanley, Nature Physics (2009)
Structural changes upon cooling Structural changes upon cooling (Simulation)(Simulation)
Tx occurs at the appearance of a new species
Tw is related to the maximal change of the structure
L. Xu, F. Mallamce, Z. Yan, F. W. Starr, S. V. Buldyrev, H. E. Stanley, Nature Physics (2009)
Conclusion IIIConclusion III
Fractional Stokes-Einstein Relation is correlated with the onset of a different structure
A structural origin for the failure of the SER can be understood by recognizing that the SE relation defines an effective hydrodynamic radius.
The different species have different hydrodynamic radii, so when their relative population changes, the classical SER breaks down.
Changes in StructuresChanges in Structures
Mallamace et al, PNAS(2006)
What makes water waterWhat makes water water
Perfect Crystal: Q6=0.57; Random configuration: Q6=0.28
Orientational order parameter:
Changes in structures upon crossing Widom Changes in structures upon crossing Widom lineline
compressibility
TW(P)
Pc=0.24
P<Pc : No anomalous behaviour! (Metastability)
P>Pc : Response functions show peaks. The location of the peaks decreases approaching to the critical pressure
Changes in thermodynamics upon crossing Changes in thermodynamics upon crossing widom linewidom line
Low T High T
As in water, solubility of non-polar solutes decreases in the Jagla model upon heating
Can Jagla model explain the decrease of methane solubility upon heating?
Stable liquid-liquid critical point (LLCP)
Negative sloped melting line
LDA and HDA
L. Xu, S. V. Buldyrev, C. A. Angell, H. E. Stanley, Phys. Rev. E (2006)L. Xu, P. Kumar, S. V. Buldyrev, P. H. Poole, F. Sciortino, S.-H Chen, H. E. Stanley, PNAS (2005)
Widom line
Phase DiagramPhase Diagram
CPmax
KTmax
Changes in response functions: Compressibility Changes in response functions: Compressibility
P>Pc : KT has maxima Anomaly occurs upon crossing the Widom line (KTmax)
P<Pc: KT increase monotonically, No anomalous behaviour!
Heating rate dependence of HDA-HDL glass Heating rate dependence of HDA-HDL glass transition and Widom line crossovertransition and Widom line crossover
α
q1≈7∙108K/s
S. R. Becker, P. H. Poole, F. W. Starr, PRL 97, 055901 (2006)F. Ferandez-Alonson, F. J. Bermejo, S. E. McLain, J. F. C. Turner, J. J. Molaison, K. W. Herwig. PRL 98, 077801 (2007)