Fractal atomic-level percolation in metallic glasses

Slides:



Advertisements
Similar presentations
Anandh Subramaniam & Kantesh Balani
Advertisements

p = 0.50 Site percolation Square lattice 400 x 400
Percolation Percolation is a purely geometric problem which exhibits a phase transition consider a 2 dimensional lattice where the sites are occupied with.
Electronic Properties of Glassy Metals MSE 410 Rochan Mehta.
Percolation Percolation is a purely geometric problem which exhibits a phase transition consider a 2 dimensional lattice where the sites are occupied with.
Fig. 1 Methods of light-sheet microscopy
Notes Ch. 6.2 Classifying the Elements
Po-chia Chen, Jochen S. Hub  Biophysical Journal 
by Xinchang Pang, Yanjie He, Jaehan Jung, and Zhiqun Lin
Volume 92, Issue 8, Pages (April 2007)
Geometrical Properties of Gel and Fluid Clusters in DMPC/DSPC Bilayers: Monte Carlo Simulation Approach Using a Two-State Model  István P. Sugár, Ekaterina.
Atsushi Matsumoto, Hisashi Ishida  Structure 
Atomically thin two-dimensional organic-inorganic hybrid perovskites
Volume 74, Issue 5, Pages (May 1998)
Peter J. Mulligan, Yi-Ju Chen, Rob Phillips, Andrew J. Spakowitz 
Hydration Force in the Atomic Force Microscope: A Computational Study
by Chuan-Chao Wang, Qi-Liang Ding, Huan Tao, and Hui Li
Structure of the Yeast RNA Polymerase II Holoenzyme
Accurate design of megadalton-scale two-component icosahedral protein complexes by Jacob B. Bale, Shane Gonen, Yuxi Liu, William Sheffler, Daniel Ellis,
Volume 110, Issue 4, Pages (February 2016)
by Hao Ye, and George Sugihara
R. Jay Mashl, H. Larry Scott, Shankar Subramaniam, Eric Jakobsson 
Volume 107, Issue 11, Pages (December 2014)
Partially Assembled Nucleosome Structures at Atomic Detail
Determination of the Hydrocarbon Core Structure of Fluid Dioleoylphosphocholine (DOPC) Bilayers by X-Ray Diffraction Using Specific Bromination of the.
Phase Transitions in Biological Systems with Many Components
Volume 96, Issue 2, Pages (January 2009)
Origin of dramatic oxygen solute strengthening effect in titanium
Jean-Pierre Kocher, Martine Prévost, Shoshana J Wodak, Byungkook Lee 
by Dane W. deQuilettes, Sarah M. Vorpahl, Samuel D
by Mark A. Silver, Samantha K. Cary, Jason A. Johnson, Ryan E
by Zhiqiang Luo, Yuanwen Jiang, Benjamin D
New online ecology of adversarial aggregates: ISIS and beyond
Volume 5, Issue 4, Pages e4 (October 2017)
Taeyoon Kim, Margaret L. Gardel, Ed Munro  Biophysical Journal 
Joe G. Greener, Ioannis Filippis, Michael J.E. Sternberg  Structure 
Emergence of room-temperature ferroelectricity at reduced dimensions
by Jungwon Park, Hans Elmlund, Peter Ercius, Jong Min Yuk, David T
Michael E Wall, James B Clarage, George N Phillips  Structure 
Pattern Selection by Dynamical Biochemical Signals
Using Atomic Force Microscopy to Study Nucleosome Remodeling on Individual Nucleosomal Arrays in Situ  H. Wang, R. Bash, J.G. Yodh, G. Hager, S.M. Lindsay,
Quantum criticality with two length scales
by Haiming Zhu, Kiyoshi Miyata, Yongping Fu, Jue Wang, Prakriti P
Volume 100, Issue 7, Pages (April 2011)
V.P. Ivanova, I.M. Makarov, T.E. Schäffer, T. Heimburg 
X-ray–driven reaction front dynamics at calcite-water interfaces
Shock-Wave Exploration of the High-Pressure Phases of Carbon
Grischa R. Meyer, Justin Gullingsrud, Klaus Schulten, Boris Martinac 
Volume 103, Issue 5, Pages (September 2012)
Volume 104, Issue 5, Pages (March 2013)
Volume 1, Issue 1, Pages (July 2016)
Mechanism of Anionic Conduction across ClC
by Lawrence W. Cheuk, Matthew A. Nichols, Katherine R
Fig. 2 Evolution of structural and magnetic properties.
Meeting 1, Tuesday, Jan. 8, 2019 Goals for this Meeting:
STATES OF MATTER Crystalline/polycrystalline/amorphous Solids- Ionic
by Alberto Ambrosetti, Nicola Ferri, Robert A
Fig. 4 Twist grain boundary free energies as a function of misalignment angle for the (110)-(100) crystal planes of a nanocrystal with 1135 atoms. Twist.
Partially Assembled Nucleosome Structures at Atomic Detail
Matthieu Chavent, Elena Seiradake, E. Yvonne Jones, Mark S.P. Sansom 
Volume 88, Issue 6, Pages (June 2005)
Scattering and Interference in Epitaxial Graphene
Mechano-thermo-chromic device with supersaturated salt hydrate crystal phase change by Hyunmin Cho, Jinhyeong Kwon, Inho Ha, Jinwook Jung, Yoonsoo Rho,
Po-chia Chen, Jochen S. Hub  Biophysical Journal 
Fig. 1 Operation mechanism and scanning electron microscopy images of MTC device. Operation mechanism and scanning electron microscopy images of MTC device.
Fig. 4 Memristive characteristics in a 1T-TaS2 nano-thick crystal.
Dislocation-accommodated grain boundary sliding as the major deformation mechanism of olivine in the Earth’s upper mantle by Tomohiro Ohuchi, Takaaki Kawazoe,
by Ding Pan, and Giulia Galli
Evidence of Cholesterol Accumulated in High Curvature Regions: Implication to the Curvature Elastic Energy for Lipid Mixtures  Wangchen Wang, Lin Yang,
Fig. 5 Classical MD simulations.
Presentation transcript:

Fractal atomic-level percolation in metallic glasses by David Z. Chen, Crystal Y. Shi, Qi An, Qiaoshi Zeng, Wendy L. Mao, William A. Goddard, and Julia R. Greer Science Volume 349(6254):1306-1310 September 18, 2015 Published by AAAS

Fig. 1 In situ diffraction and volume results. In situ diffraction and volume results. (A) Three-dimensional reconstructed sample volumes from in situ transmission x-ray microscopy data at ~0 GPa. (B) In situ x-ray diffraction data with increasing pressure (arb., arbitrary units). (C) Volume scaling with scattering vectors q1 and q2 for Cu46Zr46Al5Be3 and La62Al14Cu11.7Ag2.3Ni5Co5 metallic glasses. David Z. Chen et al. Science 2015;349:1306-1310 Published by AAAS

Fig. 2 Dimensionality crossover in simulations. Dimensionality crossover in simulations. (A) The Cu46Zr54 from FF1 and FF2 both exhibit a transition in dimensionality from ~2.5 to 3 between r2 and r3. (B) Ni80Al20 exhibits a transition in dimensionality from ~2.5 to 3 between r1 and r2. The insets show corresponding RDF curves with the correlation lengths ξ indicated. David Z. Chen et al. Science 2015;349:1306-1310 Published by AAAS

Fig. 3 Concepts in fractals and percolation. Concepts in fractals and percolation. (A and B) Site lattice percolation for p < pc (A) and p > pc (B). White squares are “occupied,” black squares are “unoccupied,” and blue squares are percolating. (C) Illustrative example of a lattice made up of Sierpinski gaskets with correlation length ξ, adopted from (23). This lattice is fractal over the short range and homogeneous over the long range. (D) MD simulation of the Cu46Zr54 system at room temperature with full periodic boundaries (Cu, blue; Zr, yellow). (E) Cu46Zr54 with all atoms removed, except for those belonging to icosahedrons. David Z. Chen et al. Science 2015;349:1306-1310 Published by AAAS

Fig. 4 Simulated properties during supercooling. Simulated properties during supercooling. (A) Dimensionality from r1 during supercooling. (B) Volume versus temperature behavior (solid black line), shown with guidelines (red dotted line) and Tg (~763 K, solid black arrow). Inset snapshots show atom vectors (red) generated from reference temperatures ~540 K above the indicated temperatures (dotted black arrows) for a slice 3 Å thick (roughly the nearest-neighbor distance). Dots are atom centers (Cu, blue; Zr, yellow). David Z. Chen et al. Science 2015;349:1306-1310 Published by AAAS