Spatially Resolved and Atom Specific Microscopy and Spectroscopy “New Characterization Tools” What can we do now that we could not do before and how will.

Slides:



Advertisements
Similar presentations
High Resolution Imaging structure and morphology phase heterogeneity & defects Electron Diffraction determine crystallography SAED CBED XEDS (energy-dispersive.
Advertisements

Ion Beam Analysis techniques:
UIC Physics Analysis of Al x Ga 1-x N Nanowires through Simulated Methods of Scanning Transmission Electron Microscopy and Electron Energy-Loss Spectroscopy.
Electron Microscopy for Catalyst Characterization Dr. King Lun Yeung Department of Chemical Engineering Hong Kong University of Science and Technology.
AMCF Materials Characterization School 2012 X-Ray Photoelectron Spectroscopy Tim Morgan.
X-ray Imaging and Spectroscopy of Individual Nanoparticles A. Fraile Rodríguez, F. Nolting Swiss Light Source Paul Scherrer Institut, Switzerland J. Bansmann.
Sub-picosecond Megavolt Electron Diffraction International Symposium on Molecular Spectroscopy June 21, 2006 Fedor Rudakov Department of Chemistry, Brown.
Intense Field Femtosecond Laser Interactions AMP TalkJune 2004 Ultrafast Laser Interactions with atoms, molecules, and ions Jarlath McKenna Supervisor:
Emre Ertuğrul Emin Şahin Seçkin Gökçe KMU 396 Material Science and Technology.
For energy generation, capture storage and transportation.
Electron microscopy analysis of nm- sized particles and segregations Frank Krumeich and Reinhard Nesper ETH Zurich, Laboratory of Inorganic Chemistry
An STM Measures I(r) Tunneling is one of the simplest quantum mechanical process A Laser STM for Molecules Tunneling has transformed surface science. Scanning.
XPS and SIMS MSN 506 Notes.
Ionization and Mass Analyzers Ionizations –Electron Ionization - “hard” –Chemical Ionization - “soft” –MALDI - desorption –FAB - desorption –Laser Post.
X-Ray Photoelectron Spectroscopy (XPS)
Surface Characterization by Spectroscopy and Microscopy
Single Molecule Dissociation by Tunneling Electrons.
Introduction to Electron Energy Loss Spectroscopy
J. R. Edwards Pierre Emelie Mike Logue Zhuang Wu
Synchrotron Radiation Interaction with Matter; Different Techniques Anders Nilsson Stanford Synchrotron Radiation Laboratory What can we hope to learn?
Scanning Probe Microscopy (SPM) Real-Space Surface Microscopic Methods.
1 Femtosecond Time and Angle-Resolved Photoelectron Spectroscopy of Aqueous Solutions Toshinori Suzuki Kyoto University photoelectron.
III. Analytical Aspects Summary Cheetham & Day, Chapters 2, 3 Chemical Characterization of Solid-State Materials Chemical Composition: Bulk, Surface, …
X. Low energy electron diffraction (LEED)
Surface Analysis Surface interface controls many aspects of chemistry
by M. S. Dresselhaus, A. Jorio, A. G. Souza Filho, and R. Saito
Demolding ENGR Pre Lab.
Anomalous Small-Angle X-ray Scattering Beamline B1 at HASYLAB, DESY MM Ulla Vainio 1, Günter Goerigk 2, Rainer Gehrke 1 1 HASYLAB at DESY, Notkestr.
Geok Mei CHONG Master Candidate of Advanced Spectroscopy in Chemistry University of Leipzig, ASC Network 4 th December
Scanning tunneling microscopy (STM) Atomic force microscopy (AFM) Scanning electrochemical microscopy (SECM) UV & visible spectroscopy Transmission experiments.
X-Rays and Materials A Vision of the Future Joachim Stöhr Stanford Synchrotron Radiation Laboratory.
Other modes associated with SEM: EBIC
Magnetization dynamics
Spectroscopy of Nanostructures
EEW508 Structure of Surfaces Surface structure Rice terrace.
TEM charcaterization Basic modes – Bright field microscopy – Dark field Microscopy –STEM – EDAX – EELS.
Reminders for this week Homework #4 Due Wednesday (5/20) Lithography Lab Due Thursday (5/21) Quiz #3 on Thursday (5/21) – In Classroom –Covers Lithography,
Engr College of Engineering Engineering Education Innovation Center Engr 1182 Nano Pre-Lab Demolding Rev: 20XXMMDD, InitialsPresentation Short.
Department of Synchrotron Radiation Research Lund University
Lecture 6: Microscopy II PHYS 430/603 material Laszlo Takacs UMBC Department of Physics.
Heterometallic Carbonyl Cluster Precursors Heterometallic molecular cluster precursor - mediate transport and growth of nanoscale bimetallic particles.
Pattersons The “third space” of crystallography. The “phase problem”
1 Institute of Isotopes, Budapest, Hungary; 2 Research Institute for Technical Physics and Materials Science, Budapest Hungary; 3 Chemical Physics of Materials,
Probing of Nanostructured Surfaces at Attosecond Timescales Emma Catton 1 st year PhD student in the Atomic Manipulation Group at NPRL Based in Birmingham.
Metal surface area What do we mean by metal surface area ?
Past and Future Insights from Neutron Scattering Collin Broholm * Johns Hopkins University and NIST Center for Neutron Research  Virtues and Limitations.
Scanning tunneling microscopy (STM) Atomic force microscopy (AFM) Scanning electrochemical microscopy (SECM) UV & visible spectroscopy Transmission experiments.
Pt-Ru Bulk Phase Diagram. + H2H2 673 K ? Supported Metal NanoparticleMetal Salt Precursor Characterization of final nanoparticles: X-ray Photoelectron.
IC T IC-1/35 Lecture Characterzation of Catalysts Investigate: Structure/morphology Surface area Number of active sites Pore distributions.
Activity and Stability of Ceria Supported Bimetallic Ni-Au in the Reforming of Ethanol By Sakun Duwal.
Department of Electronics
X-ray photoemission electron microscopy (XPEEM)
Ching-Rong “Ada” Chung Mentor: Dr. Jing Zhou Department of Chemistry
What is XPS? XPS (x-ray photoelectron spectroscopy) is also known as ESCA (electron spectroscopy for chemical analysis). XPS provides chemical information.
Extending IBA Analysis:
Optical band gaps from tetrahedral cation vacancy and variation of cation ordering in NCO films Weiwei Zhao.
Comparison of in situ XAS and in situ PES in the soft
Electron Transfer in cluster Anions:
Surface and Interface Characterization of Polymers
by Baran Eren, Danylo Zherebetskyy, Laerte L
Types of Microscopy Type Probe Technique Best Resolution Penetration
Advances in Scanning Probe Microscopy
Planck’s law: E=hn =hc/l
SLAC National Accelerator Laboratory &
Multiscale Modeling and Simulation of Nanoengineering:
Structural analysis of graphene-embedded FeN4 (FeN4/GN) catalysts
Fig. 2 Characterization of ZnxCo1−xO NRs.
Structure of the laser-chemical tailored spongy Ni(TPA/TEG) catalyst
Surface analysis techniques part I
Presentation transcript:

Spatially Resolved and Atom Specific Microscopy and Spectroscopy “New Characterization Tools” What can we do now that we could not do before and how will it change the world

Complementarity of techniques Broad beam: good statistics average over sites Local probe: poor statistics probes individual sites Time resolutionSpatial resolution Species specificSite specific Insight  N N where N = number of tools We want everything at once!

“Real-time” surface imaging methods Nanoscale [“atomic” resolution] –Fast Scanning Tunneling Microscopy (STM) –Field Ion Microscopy (FIM/FEM) Mesoscale [chemically sensitive] –Low Energy Electron Microscopy (LEEM) –Photoemission Electron Microscopy (PEEM) –Ellipsomicroscopy for Surface Imaging (EMSI) –Imaging FT-IR spectroscopy

Pattern formation on catalysts J. Lauterbach, et al., Surface Science 294 (1993) 116

Ellipsomicroscopy for Surface Imaging (EMSI)

P > mbar -> EMSI T = 540 K, CO/O 2 = Image size:1mm x 1.25 mm, dt = 0.33 s Lele, T. and J. Lauterbach, Chaos 12(1) (2002) Video

Low Energy Electron Microscopy & Synchrotron-based Photoemission Electron Microscopy Sample -20 keV Image Electron emitter Photons (uv, x-rays) 777°C 761°C 755°C 0.5  m 755°C Dark field TiO2 surface structure - LEEM RuO 2 growth

Probing of Valence Electrons with X-rays Atom specific Orbital symmetry selective Experiment--Theory

Catalytic Chemistry with Orbitals Theoretical simulations, Mats Nyberg, Stockholm University Probe pulse at different delay time  t Both N atoms New Ru Catalyst Active site at steps Hansen et.al. Science 294, 1508 (2001) Haber-Bosch N 2 + 3H 2 2NH 3

XASpectroelectrochemistry Element specific Resolves multiple redox sites Perfect for fuel cells

New Tools for Neutron Scattering: Determination of Chloroform Adsorption site in Faujasite From H pair distribution function. (J. Eckert, C. Mellot-Draznieks and A. K. Cheetham, J. Am. Chem. Soc. 2002, 124, 170 ) Parallel detectors offer more sensitivity Vibrational spectroscopy without selection rules

Paraboloid: Height h 0 = 3.1 nm ± 0.1 nm radius r 0 = 24 nm +2 nm(tip) Volume V = pi/2 h 0 r 0 2 = 2800 nm 3 density [PE] = 25 molecules/nm 3 TOF = 19 ± 2 molecules / s AFM image 100 x 100 nm heigth 3 nm AFM image of polyethylene formed by a single catalytic site: Cr on SiO 2 / Si(100) Peter Thüne, Joachim Loos, Piet Lemstra, Hans Niemantsverdriet, Macromol Symposia 2001

Laegsgaard, Osterlund, Thostrup, Rasmussen, Stensgaard and Besenbacher, Rev. Sci. Instrum. 72 (2001), Pressure-induced reconstructions on Cu(110) exposed to H bar (before) 1 bar H 2 (during) bar (after) Atomic Resolution Images Under High Pressure Conditions In-situ HRTEM offers defect analysis - identification of active sites in vanadyl pyrophosphate catalysts

Ga EELS 1.4Å As Z-contrast STEM Z=31 Z=33

EELS profile across a single particle 2nm Co L 2,3 -edges Ni L 2,3 -edges Energy Loss (eV) Intensity (a.u.) Co Ni Co/Ni Concentration profile

Pt on  -alumina 1.3 Å probe Pt on  -alumina 0.5 Å probe Imaging of Active Catalyst Atom Configurations Pt atoms sit in surface vacancies [001] [110]