RECX Thin film metrology.

Slides:



Advertisements
Similar presentations
MIT Center for Materials Science and Engineering
Advertisements

(see Bowen & Tanner, High
1 X-ray Scattering from Thin Films Experimental methods for thin films analysis using X-ray scattering –Conventional XRD diffraction –Glancing angle X-ray.
Another example of interference that is often observed is interference from a thin film. Light incident on the surface of a thin film is reflected from.
Optical Modeling of a-Si:H Thin Film Solar Cells with Rough Interfaces Speaker : Hsiao-Wei Liu 08/18/2010 Wed.
Chapters 29 Interference and Diffraction. Topics Huygens Principal Diffraction Interference –two slit –thin film Polarization Holography.
Plan : lattices Characterization of thin films and bulk materials using x-ray and electron scattering V. Pierron-Bohnes IPCMS-GEMME, BP 43, 23 rue du Loess,
Determination of Crystal Structures by X-ray Diffraction
AP Physics Mr. Jean March 30 th, The plan: Review of slit patterns & interference of light particles. Quest Assignment #2 Polarizer More interference.
The X-Ray SEF Scott Speakman
Lecture 2.1 Crystalline Solids. Poly-crystalline solids - Grains Mono-crystalline solids- Whiskers, Wafers.
Crystallography and Diffraction Techniques Myoglobin.
I am not an expert on any of this!
Characterizing the Nanoscale Layers of Tomorrow’s Electronics : An Application of Fourier Analysis Chris Payne In Collaboration With: Apurva Mehta & Matt.
MODULE 4 - Introduction to EBSD
The X-Ray SEF Scott Speakman
Applying X-Rays in Material Analysis
IPCMS-GEMME, BP 43, 23 rue du Loess, Strasbourg Cedex 2
Ellipsometry and X-ray Reflectivity (XRR)
Tuesday, May 15 - Thursday, May 17, 2007
1 Sodium Doped Lanthanum Manganites Thin Films: Synthesis, Substrate Effect and Thickness Dependence Paolo Ghigna Dipartimento di Chimica Fisica “M. Rolla”,
John Bargar 2nd Annual SSRL School on Hard X-ray Scattering Techniques in Materials and Environmental Sciences May 15-17, 2007 What use is Reciprocal Space?
Beam Lines At SSRL Cathie Condron SSRL Scattering Workshop May 2007.
Nomenclature Usually, it is sufficient to know the energy En(k) curves - the dispersion relations - along the major directions. Directions are chosen that.
Submitted By:- Nardev Kumar Bajaj Roll NO Group-C
Thin films II Kinematic theory - works OK for mosaic crystals & other imperfect matls Doesn't work for many, more complicated films Kinematic theory -
Chapter 5: Wave Optics How to explain the effects due to interference, diffraction, and polarization of light? How do lasers work?
Neutron Scattering 102: SANS and NR
Magnetoelastic Coupling and Domain Reconstruction in La 0.7 Sr 0.3 MnO 3 Thin Films Epitaxially Grown on SrTiO 3 D. A. Mota IFIMUP and IN-Institute of.
Daniel Wamwangi School of Physics
Peak intensities Peak widths
Stanford Synchrotron Radiation Laboratory More Thin Film X-ray Scattering: Polycrystalline Films Mike Toney, SSRL 1.Introduction (real space – reciprocal.
Applying X-Ray Diffraction in Material Analysis Dr. Ahmed El-Naggar.
X-rays techniques as a powerful tool for characterisation of thin film nanostructures Elżbieta Dynowska Institute of Physics Polish Academy of Sciences,
Near-surface diffraction capabilities at NECSA TP Ntsoane Diffraction Section 11 September 2015.
Neutron Metrology for Fuel Cells David Jacobson, National Institute of Standards & Technology (NIST) Phenomena Probed in Hydrogenous Materials Very large.
Surface Plasmon Resonance (SPR)
Last Time Brillouin Zones and Intro to Scattering
XRD allows Crystal Structure Determination What do we need to know in order to define the crystal structure? - The size of the unit cell and the lattice.
Artifacts in the characterization of skin layers and ultrathin films by X-ray diffraction X. Marti, V. Holy Charles University, Prague P. Ferrer, T. Schulli.
National Science Foundation GOALI: Epitaxial Growth of Perovskite Films and Heterostructures by Atomic Layer Deposition and Molecular Beam Epitaxy John.
SUPERLATTICE PHOTOCATHODES: An Overview Tarun Desikan PPRC, Stanford University
Center for Materials for Information Technology an NSF Materials Science and Engineering Center Scattering Techniques Lecture 17 G.J. Mankey
Unit 12: Part 1 Physical Optics: The Wave Nature of Light.
Reciprocal Lattices to SC, FCC and BCC
Announcements HW set 10 due this week; covers Ch (skip 24.8) and Office hours: Prof. Kumar’s Tea and Cookies 5-6 pm today My office hours.
The Muppet’s Guide to: The Structure and Dynamics of Solids XRD.
X-Ray Reflectivity Measurement
Center for Materials for Information Technology an NSF Materials Science and Engineering Center Sputtering Procedures Lecture 11 G.J. Mankey
Pattersons The “third space” of crystallography. The “phase problem”
The Structure and Dynamics of Solids
Preferred orientation Stereographic projections of pole density random single crystal oriented polycrystalline material.
The Muppet’s Guide to: The Structure and Dynamics of Solids Single Crystal Diffraction.
IPCMS-GEMME, BP 43, 23 rue du Loess, Strasbourg Cedex 2
By Abdullah Framalawi Aly Abouhaswa Polarized Neutron Spectrometry : Studying nanostructure magnetism with the use of polarized neutron reflectometry.
Electrical Transport Properties of La 0.33 Ca 0.67 MnO 3 R Schmidt, S Cox, J C Loudon, P A Midgley, N D Mathur University of Cambridge, Department of Materials.
Structural and Optical Properties of SrTiO 3 on Different Substrates N. Samarasingha, Cesar Rodriguez, Jaime Moya, Stefan Zollner, Nalin Fernando Department.
Strain dependence of the band structure and critical points of pseudomorphic Ge1-ySny alloys on Ge Nalin Fernando,1 John Hart,2 Ryan Hickey,2 Ramsey Hazbun,2.
MBE Growth of Graded Structures for Polarized Electron Emitters
Davide De Salvador INFN-Laboratori Nazionali di Legnaro &
Reflectivity Measurements on Non-ideal Surfaces
X-ray Scattering from Thin Films
Crystallography H. K. D. H. Bhadeshia Introduction and point groups
Reflectivity Measurements of Oxide Layers on Glass
Phys102 Lecture 25 The Wave Nature of Light; Interference
Chapter 1 Crystallography
Crystallography H. K. D. H. Bhadeshia Introduction and point groups
Deformation and texture
Max. max Figure 37.4 (a) Constructive interference occurs at point P when the waves combine. (b) Constructive interference also occurs at point Q.
Reciprocal Lattice & Diffraction
Presentation transcript:

RECX Thin film metrology

XRR Phi-scan GIXRD Rocking curve Polar plot HRXRD / RSM Film thickness Roughness Density Phi-scan In plane orientation GIXRD Enhance material probed Phase Stress Depth profiling Rocking curve Miscut Orientation Polar plot Texture HRXRD / RSM Texture Strain Orientation

XRR Phi-scan GIXRD Rocking curve Polar plot HRXRD / RSM Film thickness Roughness Density Phi-scan In plane orientation GIXRD Enhance material probed Phase Stress Depth profiling Rocking curve Miscut Orientation Polar plot Texture HRXRD / RSM Texture Strain Orientation

XRR (X-ray reflectometry) Reflectivity as function of angle to obtain information on: Film thickness Surface roughness Density

XRR (X-ray reflectometry) Scattering from surfaces and interfaces at low angles, ~0-8o Variations in electron density arise from film thickness, roughness and density which can be determined for each layer ~50nm LaNiO3 on SrTiO3 Density Thickness Roughness k’ k Q Scattering occurs from variations in electron density Electron density Fouriertransform Refined parameters: LaNiO3 Thickness 48.98nm “ Roughness 0.30 nm “ Density 7.05 g/cm3 A surface layer of 1.4nm is also required to fully explain the results

XRR (X-ray reflectometry) Layered thin films of Eu2O3 and TiO2 grown by ALD as conversion material with the aim of controlling the Eu-Eu distance.

XRR (X-ray reflectometry) Layered thin films of Eu2O3 and TiO2 grown by ALD as conversion material with the aim of controlling the Eu-Eu distance. The double layer thicknesses: 10N = 7.5 Å 20N = 15.9 Å 50N = 29.1 Å Half the double layer thickness of the 10N sample, 3.8 Å, is approx the same as the shortest Eu – Eu distance in cubic Eu2O3, 3.6 Å

XRR (X-ray reflectometry)

XRR Phi-scan GIXRD Rocking curve Polar plot HRXRD / RSM Film thickness Roughness Density Phi-scan In plane orientation GIXRD Enhance material probed Phase Stress Depth profiling Rocking curve Miscut Orientation Polar plot Texture HRXRD / RSM Texture Strain Orientation

GIXRD (Grazing incident x-ray diffraction) Increase the pathway through the sample Conventional q-2q

GIXRD (Grazing incident x-ray diffraction) Increase the pathway through the sample GIXRD

GIXRD (Grazing incident x-ray diffraction) A ZnO film of 200 nm deposited by ALD Conventional q-2q GIXRD

GIXRD (Grazing incident x-ray diffraction) Depth profile analysis

XRR Phi-scan GIXRD Rocking curve Polar plot HRXRD / RSM Film thickness Roughness Density Phi-scan In plane orientation GIXRD Enhance material probed Phase Stress Depth profiling Rocking curve Miscut Orientation Polar plot Texture HRXRD / RSM Texture Strain Orientation

HRXRD (High-resolution x-ray diffraction) Increase the pathway through the sample

HRXRD (High-resolution x-ray diffraction) Map the reciprocal space to obtain information on: Orientation Strain Texture … and a lot more…

HRXRD (High-resolution x-ray diffraction)

HRXRD (High-resolution x-ray diffraction)

HRXRD (High-resolution x-ray diffraction)

HRXRD (High-resolution x-ray diffraction) Film of NaNbO3 on LaAlO3

XRR Phi-scan GIXRD Rocking curve Polar plot HRXRD / RSM Film thickness Roughness Density Phi-scan In plane orientation GIXRD Enhance material probed Phase Stress Depth profiling Rocking curve Miscut Orientation Polar plot Texture HRXRD / RSM Texture Strain Orientation