Download presentation
Presentation is loading. Please wait.
Published byAshlyn Lewis Modified over 9 years ago
2
Non-Harvard Collaborators: Ben Ocko, Elaine DiMasi, Olaf Magnussen Physics Dept. Brookhaven National Laboratory Moshe Deutsch: Bar Ilan University, Israel Binhua Lin, Mati Meron, Tim Graber, Jeff Gerbhardt, Advanced Photon Source Harvard Students/Postdocs Alexei Grigoriev, Patrick Huber, E.H. Kawamoto, Holger Tostmann, Mike Regan, Oleg Shpyrko. The Surface Structure of Liquid Metals and Alloys Support: DE-FG02-88-ER45379/NSF- DMR-0124936 * Current associates are underlined Oleg Shpyrko
3
Liquid Surfaces: Metals/Non-Metals Are Different For Metals Particle-Particle Interactions Change Across The Surface D'Evelyn &. Rice, J. Chem. Phys., 1983. 78: p. 5225. This influences the structure of the surface! Interactions are Same in Vapor and Liquid Dielectric Liquids Vapor: Neutral Atoms Liquid: Positive Ions in Sea of Negative Fermi Liquid Different Interactions Metallic Liquids
4
Non-Metal Liquids Predictions of Monte Carlo Calculations Average Density vs Distance From Surface(z) Chapela & Saville, 1978 Hard Wall = > Layers Free Surface No-Layer D'Evelyn & Rice, 1983 Metallic Liquids: Layers @Free Surface Liquid/Vapor Surface Structure Factor (Q z )
5
X-ray Reflectivity: R(Q z ) & (Q z ) Quantitative Measure of (Q z )! Surface Structure Factor Prediction: Constructive Interference Q z =(4 )sin =(2 /D) R(Q z )~| (Q z )| 2 QzQz Surface Normal Wave vector Transfer Measured Hg (1995) Ga (1996) In (1999) Hg In Ga Note Difference
6
Thermal Effects on Reflectivity R(Q z ) = Ideal Flat Surface: Fresnel R F (Q z ) Structure Factor (Q z ) Thermal Factor Differential Cross Section: Thermal Roughness Phase Shifts QxQx Parallel Surface Wave Vector Transfer
7
Liquid vs Solid Surfaces Depends on Resolution Liquid Liquid Surface 2D SurfaceTension Gravity (|x-x’|~mm) Solid Independent of Resolution Resolution
8
Measure of Structure Factor Requires Thermal Effects be Removed R(Q z ) = Ideal Flat Surface: Fresnel R F (Q z ) Structure Factor (Q z ) Thermal Factor (Q z,T) R(Q z ) Large (T/ Q z 2 No specular peak if ~2! Surface Tension
9
To Understand Thermal Effects Diffuse Scattering From Liquid Surface Q x =(2 )[cos -cos ] Q z =(2 )[sin +sin ] Diffuse Scattering for Liquid Indium Solid Lines: Theory Known Surface Tension is Only Adjustable Parameter
10
Demonstration of Thermal Removed: Liquid Gallium Electron Density: Ga and In Average Electron Density Indium (with/without T effects). Electron Density Profile
11
Issue 1 What other metals can be studied? ElementTm (K) Tm/ P_melt(mm) Ga302.937180.42 Hg234.284980.471.2E-06 Sn505.1185600.90 In429.325560.77 K336.83880.87~1.0E-6 Zn692.737820.892.2E-01 Al933.529141.02 Cu1356.613031.049.7E-04 Cd594.15701.041.1E-01 Bi544.53781.44 Li (Chemistry)453.693981.14 Au1337.5811691.141.6E-05 Tl576.74641.24 Pb600.644581.31 (i.e. T/ ) must be small P & T : low enough for UHV(Hg, K, Na are special)
12
Measurement of Potassium Good: Oxides Dissolve in Bulk Liquid Clean Surface Bad: Low at layering peak is large, R(Q z ) too small Ga In K Maximum Q z ~0.85Q Peak Data Layering in K is same as Ga, In. Debye-Waller X 10 -2
13
R(Q z ) Possible ModelSpacing of 1st Layer Reduced~10% Anomalous Layering of Liquid Sn Surface Bump Not seen in Ga,In Bump Surface Density Is Higher Than Bulk!
14
Ga K H 2 O Is there experimental evidence that dielectric liquids are not layered? Water: dynes/cmK: dynes/cm R(Q z ) R(Q z )/R F (Q z ) Water does not show indication of surface layering!
15
If we can’t study other pure metals, what can we do? Alloys Surface Chemistry of Liquid Metals (oxidation) Surface: Heavier Bi rich liquid Bulk: lighter Ga rich liquid! GaBi: Binary Phase Diagram BiGa Thickness of heavier Bi rich layer. Short Range Wetting
16
Keep Looking: i.e. Alloys for Electronics Example: AuSi Low Temperature Eutectic AuSi Diffuse Scattering Alloy is Liquid =780 dynes/cm
17
Summary 1- To Measure Liquid Surface Structure Factor | (Q z )| Effects of Capillary Waves. 2- | (Q z )| of Free Surface of Liquid Metals Exhibits Atomic Layering! 3- Water does Not! What about other non-metallic liquids. 4- Surfaces of Liquid Alloys: Interesting Physics Sn: Anomalous Surface GaBi: Short Range Wetting AuSi: Enormously Intense Future
Similar presentations
© 2025 SlidePlayer.com. Inc.
All rights reserved.