Adsorption of Hydrocarbons on Complex Metallic Alloy Surfaces - Lubricants and Superlubricity Renee D. Diehl, Physics, Pennsylvania State University, University.

Slides:



Advertisements
Similar presentations
Reflection High Energy Electron Diffraction Wei-Li Chen 11/15/2007.
Advertisements

Influence of Substrate Surface Orientation on the Structure of Ti Thin Films Grown on Al Single- Crystal Surfaces at Room Temperature Richard J. Smith.
IPCMS-GEMME, BP 43, 23 rue du Loess, Strasbourg Cedex 2
Surface Enhanced Infrared Absorption (SEIRA) Spectroscopy
Alloy Formation at the Co-Al Interface for Thin Co Films Deposited on Al(001) and Al(110) Surfaces at Room Temperature* N.R. Shivaparan, M.A. Teter, and.
Epitaxial Overlayers vs Alloy Formation at Aluminum- Transition Metal Interfaces Richard J. Smith Physics Department Montana State University Bozeman MT.
Alloy Formation at the Epitaxial Interface for Ag Films Deposited on Al(001) and Al(110) Surfaces at Room Temperature* N.R. Shivaparan, M.A. Teter, and.
Applications of MeV Ion Channeling and Backscattering to the Study of Metal/Metal Epitaxial Growth Richard J. Smith Physics Department Montana State University.
NWAPS-May Evolution of Ni-Al interface alloy for Ni deposited on Al surfaces at room temperature R. J. Smith and V. Shutthanandan* Physics Department,
7th Sino-Korean Symp June Evolution of Ni-Al interface alloy for Ni deposited on Al surfaces at room temperature R. J. Smith Physics Department,
Warren J. Hehre. The electrostatic potential is the energy of interaction of a point positive charge (an electrophile) with the nuclei and.
Thin Film Quantitation of Chemistry and Thickness Using EPMA John Donovan Micro Analytical Facility CAMCOR (Characterization of Advanced Materials in Oregon)
Spectroscopic Techniques for Probing Solid Surfaces Part II of Surface Primer.
I. Brief introduction Several questions to ask in this course: 1. What is the objective of the course - “introduction to crystal structure and diffraction.
Quantum Dots. Optical and Photoelectrical properties of QD of III-V Compounds. Alexander Senichev Physics Faculty Department of Solid State Physics
Synchrotron Radiation Interaction with Matter; Different Techniques Anders Nilsson Stanford Synchrotron Radiation Laboratory What can we hope to learn?
Buckling Delamination with Application to Films and Laminates
Grazing Incidence X-ray Scattering from Patterned Nanoscale Dot Arrays D.S. Eastwood, D. Atkinson, B.K. Tanner and T.P.A. Hase Nanoscale Science and Technology.
X. Low energy electron diffraction (LEED)
Methods in Surface Physics Experimentation in Ultra-High Vacuum Environments Hasan Khan (University of Rochester), Dr. Meng-Fan Luo (National Central University)
Ionic and Covalent Compounds. How many valence electrons do atoms need in the highest energy level to be stable? 8.
2D Islanding of Dodecane on an Au(111) Surface: An Investigation Using He beam Reflectivity and Monte Carlo Modeling Timothy C. Arlen 1, Craig J.D. Webster.
Delocalization of Electrons Section Introduction Delocalization allows the pi electrons to spread over more than two nuclei This spreading out of.
ENC Practice. If ENC increases, size _____ Size decreases ENC pulls the electrons in tighter, therefore the total size of the atom (created by the electron.
Coupling Single Molecule Magnets to Ferromagnetic Substrates.
Delocalized electrons in pi bonds What is a delocalized electron?  – Describe the delocalization of pi electrons and explain how this.
Thin Films Observations In small groups, take turns blowing bubbles from your bubble mix. Notice the color of the bubbles and when it appears that.
Center for Materials for Information Technology an NSF Materials Science and Engineering Center Substrate Preparation Techniques Lecture 7 G.J. Mankey.
X-ray Standing Wave Fluorescence for the Analysis of Bacterial Biofilms X-ray Standing Wave Fluorescence for the Analysis of Bacterial Biofilms C. A. Crot,¹.
Electronic Structure and Chemical Reactivity
Quantum Methods For Adsorption
A.E. GunnæsMENA3100 V08 Electron Diffraction (ED) in the transmissions electron microscope.
Lecture 3 More on Adsorption and Thin Films 1.Monolayer adsorption 2.Several adsorption sites 3.Thin Films (S ~ constant, multilayer adsorption) 1Lecture.
Planar Chiral Metamaterials & their application to optoelectronics devices W. Zhang, A. Papakostas, A. Potts, D. M. Bagnall, N. I. Zheludev Microelectronic.
High Resolution Energy Loss Spectroscopy of “Sheet” Plasmons Roy F. Willis, Department of Physics, The Pennsylvania State University University Park, PA.
Day Which metal would you expect to be more reactive - Fr OR Cu? WHY? 2.Which nonmetal would you expect to be more reactive - F OR Ne? WHY?
EXPERIMENTAL AND THEORETICAL STUDIES ON GLUCOSE HYDROGENATION TO PRODUCE SORBITOL M.Banu ( ) Marcia C. Martins Castoldi, React.Kinet.Catal.Lett.
Laue equations and reciprocal lattice  . Laue camera Unfiltered X-radiation through collimator back reflexion photo (spots on hyperbolas) forward.
Characterizing Multi- layer thin films Janez Kosir
Periodic Trends Section 6.3. Periodic Law The pattern of properties within a period repeats as you move across a period from left to right… When elements.
Paul Frank Institute of Solid State Physics, Graz University of Technology Financially supported by the Austrian Science Fund.
A) good b) poor c) small molecules d) ionic e) poor f) covalent g) giant.
Controlling the CO adsorption on Pt clusters by dopant induced electronic structure modification Piero Ferrari, [a] Luis M. Molina, [b] Vladimir E. Kaydashev,
Ch.4 Atomic Structure of Solid Surfaces.
DFT calculations of metal/ceramic interfaces
Electron probe microanalysis EPMA
Study of vacuum stability at cryogenic temperature
CH-4: Imperfections in Solids
What is XPS? XPS (x-ray photoelectron spectroscopy) is also known as ESCA (electron spectroscopy for chemical analysis). XPS provides chemical information.
Periodic Trends Section 6.3.
Three-dimensional reconstruction of mesoporous materials from gas adsorption and structure factor data Lev D. Gelb, Department of Chemistry, Washington.
Graphene doping with single atoms – a theoretical survey of energy surface  Elad Segev and Amir Natan* Department of Physical Electronics , Electrical.
Study of vacuum stability at cryogenic temperature
Structure and Dynamics of Aqueous and Aqueous-Hydrocarbon Fluids between Charged Surfaces Yongsheng Leng, Department of Mechanical and Aerospace Engineering,
Periodic Trends Section 6.3.
REMOVING SURFACE CONTAMINATES FROM SILICON WAFERS
Adsorption of Hydrocarbons on Complex Metallic Alloy Surfaces - Lubricants and Superlubricity Renee D. Diehl, Physics, Pennsylvania State University, University.
Please see slide 2 for the caption of this figure.
Riccardo DeSalvo (Cal State LA)
Materials Science and Metallurgy Course C6: Crystallography
IC AND NEMS/MEMS PROCESSES
Edmar A. Soares, Rosa M. C. Marques, Vagner E. de Carvalho, Hans-D
Growth Behavior of Co on Al(001) substrate
Volume 124, Issue 5, Pages (March 2006)
Mass Transport of Xe Multi-layers on Cu(111)
Anandh Subramaniam & Kantesh Balani
Kristen E. Norman, Hugh Nymeyer  Biophysical Journal 
Vibrational state distributions of (1) scattered unoriented NO(v = 3) (green bars), (2) NO(v = 3) with an incidence orientation of O atoms pointing toward.
Anandh Subramaniam & Kantesh Balani
The Density and Refractive Index of Adsorbing Protein Layers
Presentation transcript:

Adsorption of Hydrocarbons on Complex Metallic Alloy Surfaces - Lubricants and Superlubricity Renee D. Diehl, Physics, Pennsylvania State University, University Park, PA For the application of low-friction quasicrystalline surface coatings, it is important to understand the interaction between hydrocarbon lubricants and quasicrystals. We are studying the surface of an Al13Co4 alloy, which is an approximant of the Al-Ni-Co quasicrystal. We have performed a low-energy electron diffraction (LEED) experiments of this complex surface (movie, left). An extensive LEED I(E) analysis, which is an order of magnitude larger than any other LEED study, is nearly complete. This will provide input for the analysis of adsorption experiments. Surface structure model, the layer is buckled with red (blue) atoms located above (below) the plane Movie of the LEED patterns as a function of incident beam energy. Xe Benzene The adsorption of Xe was studied as a prototypical adsorbate. Xe adsorbs layer-by-layer, and does not order until the second layer begins to adsorb. The multilayer Xe appears to form a bulk-like structure which has a specific but non-symmetry alignment with the substrate. This film is observe to rotate to a symmetry direction under the influence of the electron beam, presumably due to cracking of residual gas molecules, indicating that this surface is very sensitive to contamination. Simulations are underway to gain a deeper understanding of this adsorption.