Probing Interlayer States in 2D Materials Randall M. Feenstra, Carnegie-Mellon University, DMR 1205275 Two-dimensional (2D) materials possess a special.

Slides:



Advertisements
Similar presentations
The resistivity of bulk ferromagnetic metals depends on the angle between the magnetization and the electric current. This phenomenon was discovered by.
Advertisements

Morphological Evolution during Graphene Formation on SiC(0001) Randall Feenstra, Carnegie Mellon University, DMR Graphene, consisting of monolayer.
Yat Li Department of Chemistry & Biochemistry University of California, Santa Cruz CHEM 146C_Experiment #3 Identification of Crystal Structures by Powder.
Specs and Design Options for a 8”-flat-panel MCP-PMT Fabrication Facility Dean Walters Argonne National Laboratory.
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.
Atomic Force Microscopy Studies of Gold Thin Films
1 Oxidation Effects on the Optical Constants of Heavy Metals in the Extreme Ultraviolet Amy Grigg R. Steven Turley Brigham Young University.
Spin-Polarised Scanning Tunnelling Microscopy of Thin Film Cr(001)?
First Principles Calculations of Complex Oxide Perovskites David-Alexander Robinson Sch., Theoretical Physics, The University of Dublin, Trinity College.
Basic Imaging Modes Contact mode AFM Lateral Force Microscopy ( LFM)
Large-Scale Density Functional Calculations James E. Raynolds, College of Nanoscale Science and Engineering Lenore R. Mullin, College of Computing and.
Quantum Electronic Effects on Growth and Structure of Thin Films P. Czoschke, Hawoong Hong, L. Basile, C.-M. Wei, M. Y. Chou, M. Holt, Z. Wu, H. Chen and.
New magneto-optical fingerprints in graphene John Cerne, SUNY at Buffalo, DMR We developed powerful new measurement and analysis techniques to.
Materials Process Design and Control Laboratory ON THE DEVELOPMENT OF WEIGHTED MANY- BODY EXPANSIONS USING AB-INITIO CALCULATIONS FOR PREDICTING STABLE.
Magnetic domain characterization  Lorentz transmission electron microscopy (LTEM) imaging techniques are used to image the magnetic domain structure of.
Engineering 1182 College of Engineering Engineering Education Innovation Center Solid Modeling Introduction Rev: , AJPSolid Modeling Introduction1.
Interface Characterization of Organic Bistable Devices (OBD) Y.Gao, U. Rochester, Y.Yang, UCLA, DMR One of us (YY) observed that inserting a metal.
1 Li Xiao and Lichang Wang Department of Chemistry & Biochemistry Southern Illinois University Carbondale The Structure Effect of Pt Clusters on the Vibrational.
Tunneling Outline - Review: Barrier Reflection - Barrier Penetration (Tunneling) - Flash Memory.
Quantum Electronic Structure of Atomically Uniform Pb Films on Si(111) Tai C. Chiang, U of Illinois at Urbana-Champaign, DMR Miniaturization of.
Interface Structure for Graphene on SiC(000-1) Randall Feenstra, Carnegie-Mellon University, DMR The interface of graphene on SiC(0001) is known.
1 K. Overhage, Q. Tao, G. M. Jursich, C. G. Takoudis Advanced Materials Research Laboratory University of Illinois at Chicago.
Detection plan for STEIN, telescope of the space mission CINEMA 1 August 3td 2011-Diana Renaud.
Revisit of the Growth of Co on Cu(111) Introduction  Cobalt thin films on Cu(111) are model systems for magnetic investigations and their structures and.
LaBella Group Towards an Atomic Scale Understanding of Spin Polarized Electron Transport Towards an Atomic.
Determining Chemical Order Parameter from Small Volumes Gregory B. Thompson, University of Alabama Tuscaloosa, DMR Intellectual Merit Ta enrichment.
K.R. Roos, F. Meyer zu Heringdorf, et al. J. Phys: Cond. Mat. 17 (2005) S1407 Diffusion Made Visible DMR James H. Craig, Jr. Kelly R. Roos The.
Electrical Transport in Thin Film Nanostructures Hanno H. Weitering, The University of Tennessee, DMR Competing periodicities in a single atom.
Influence of carrier mobility and interface trap states on the transfer characteristics of organic thin film transistors. INFM A. Bolognesi, A. Di Carlo.
Fiber optic networks –must be fast-acting –must integrate into fiber systems –must operate at infrared wavelengths Eye protection –scope sights –binoculars.
A ‘Writable’ Next-generation Magnetic Media Material Gregory B. Thompson, University of Alabama Tuscaloosa, DMR Intellectual Merit Ta enrichment.
Electronic Properties of Thin Film Organic Superconductors studied using Synchrotron Radiation-based Soft X-Ray Spectroscopies Kevin E. Smith, Boston University,
University of Alabama MRSEC William H. Butler DMR Theory of Tunneling Magnetoresistance Leads to New Discoveries with Potential Technological Impact.
Lecture 6: Microscopy II PHYS 430/603 material Laszlo Takacs UMBC Department of Physics.
Thin films are basic building blocks for devices. As device size shrinks, quantum effects become important, and traditional thinking in terms of electron.
Real-Time Optical Diagnostics of Rapid Graphene Growth CNMS Staff Science Highlight Real-time Raman spectroscopy, optical reflectivity, and microscope.
Accomplishments in the third year: Thus far, three papers have been published in 2008 and one manuscript entitled “Induced smectic phase in mixtures of.
Electronic Structure and Chemical Reactivity
LaBella Group cnse.albany.edu Towards an Atomic Scale Understanding of Spin Polarized Electron Transport Towards.
From quasi-2D metal with ferromagnetic bilayers to Mott insulator with G-type antiferromagnetic order in Ca 3 (Ru 1−x Ti x ) 2 O 7 Zhiqiang Mao, Tulane.
Materials Process Design and Control Laboratory ON THE DEVELOPMENT OF WEIGHTED MANY- BODY EXPANSIONS USING AB-INITIO CALCULATIONS FOR PREDICTING STABLE.
NSF Nugget for FY06 Computational thermodynamics of the Mg-B-C ternary system Sept FRG on Two Gap Superconductivity Wisconsin-Penn State- Arizona.
Fiber optic networks –must be fast-acting –must integrate into fiber systems –must operate at infrared wavelengths Eye protection –scope sights –binoculars.
Materials World Network: Structures and Mechanical Behavior of Amorphous Solids Peter K. Liaw, University of Tennessee Knoxville, DMR Findings:
Morphology and Mobility of Graphene on SiC(0001) Randall M. Feenstra, Carnegie-Mellon University, DMR Graphene formed on the (0001) surface of.
Multi-Scale Modeling of Co-Fired Ceramics' Fabrication Eugene Olevsky, San Diego State University Foundation, DMR A multi-scale framework for the.
Radiation Damage Quick Study Edward Cazalas 3/27/13.
Theoretical Characterization of Interfacial Bonding in Self-Assembled Carbon Nanotubes Igor Vasiliev, New Mexico State University, DMR Assembly.
Role of Grain Boundary Character on Dynamic Recrystallization Megan E. Frary, Boise State University, DMR Dynamic recrystallization occurs when.
Nanoscale Schottky Barrier Measured Using STM Peter Bennett, Arizona State University, DMR The current-voltage (I-V) behavior of nanoscale metallic.
Controlled fabrication and optical properties of one-dimensional SiGe nanostructures Zilong Wu, Hui Lei, Zhenyang Zhong Introduction Controlled Si and.
November 2005NASA Electronic Parts and Packaging (NEPP) Program Tin Whiskers Growing Inside ~45 Year Old AF114 Germanium Transistors Parts Analysis by:
First-Principles Based Prediction of High-Temperature Defect Chemistry and Conductivity of TiO 2 Elizabeth C. Dickey, Pennsylvania State Univ University.
Using a tight-binding approximation to compute the electronic structure of sensitizer molecules adsorbed onto TiO 2 surfaces. Daniel R. Jones & Alessandro.
How Do We Control Material Processes at the Level of Electrons? Progress on Grand Challenge New Horizons for Grand Challenge Remaining ChallengeRefreshed.
Identifying Radiative Polaritons in Thin Oxide Films with Experimental and Simulated Dispersion Relations Anita J. Vincent-Johnson 1, James S. Hammonds.
Investigation of dendritic structures forming during chemical vapour deposition growth of graphene Istanbul Technical University, Department of Physics,
Basic Planar Processes
Ultrasonic Welding Welding Technology/ 3.4 Ultrasonic Welding.
DFT calculations of metal/ceramic interfaces
Institute of Electronics, Bulgarian Academy of Sciences,
Partnership between NMHU and OSU in Electronic, Optical and Magnetic Materials; DMR One step synthesis of fluorescent graphene quantum dots through.
Fig. 5: Energy diagram of the PBHM-plasmonic coupled system.
Classical and Quantum Diffusion of Hydrogen Atoms on Cu(111)
Structural Quantum Size Effects in Pb/Si(111)
Atomistic simulations of contact physics Alejandro Strachan Materials Engineering PRISM, Fall 2007.
Atomistic materials simulations at The DoE NNSA/PSAAP PRISM Center
Partnership between NMHU and OSU in Electronic, Optical and Magnetic Materials; DMR One step synthesis of fluorescent graphene quantum dots through.
Conduction of Electricity in Solids
Through the Looking Glass at the Atomic Scale
Presentation transcript:

Probing Interlayer States in 2D Materials Randall M. Feenstra, Carnegie-Mellon University, DMR Two-dimensional (2D) materials possess a special type of electronic state that is localized between the atomic planes (not on the planes). The energies of such interlayer states are sensitive to the interplanar separation, as well as to the presence of e.g. intercalants between planes. We have measured the energies of interlayers states for graphene on Cu(001) and Cu(111) using a low- energy electron microscope. In spectra of electron reflectivity vs. energy, minima occur at the energies of interlayer states. By comparing the measured spectra with theoretical predictions, the separation between the graphene and the substrate is determined. Comparison of experiment and theory for low- energy electron reflectivity of graphene on copper. Srivastava, Gao, Widom, Feenstra, Nie, McCarty, and Vlassiouk, Phys. Rev. B 87, (2013).

WaveTrans – for obtaining wavefunctions from VASP Randall M. Feenstra, Carnegie-Mellon University, DMR VASP, the Vienna Ab-Initio Simulation Package, is used by hundreds of researchers worldwide to perform density-functional computations for solids. Remarkably, a computer program that enabled the extraction of complete, real-space wavefunctions from VASP was lacking. Rather, the decomposition of wavefunctions in terms of atomic basis states on specified atoms was provided, although that is insufficient for many applications. For example, the PI has studied interlayer states formed between graphene and metal surfaces such as copper. These wavefunctions, examples of which are shown in the figure, have peaks (marked by arrows) located between the atomic planes. To obtain the complete wavefunctions, the PI and his collaborator Michael Widom of CMU, developed a program that extracted the Fourier coefficients of the wavefunction from a binary file output by VASP. The routine is posted at and a link to that site has been placed on the VASP user bulletin board. Wavefunction for graphene on copper for different spacings and energies.

Undergrad Project Development of Vacuum System Randall M. Feenstra, Carnegie-Mellon University, DMR Photo shows Maddie McKay, an undergrad Physics major at CMU, who has worked in Prof. Feenstra’s laboratory during her junior and senior years developing a small vacuum system. This system will be employed in a Physics Laboratory Class to enable deposition of thin films that will be subsequently oxidized to form tunnel barriers. Maddie’s work included design of all components, procurement of parts (through purchase orders, or with mechanical drawings of pieces that were then fabricated), assembly, and testing. Use of the system to form tunnel junction is presently in progress. The photo was taken during the department’s annual poster session, held at the end of each Spring semester.