COMPARISON OF FOUR DATA ANALYSIS SOFTWARE FOR COMBINED X-RAY REFLECTIVITY AND GRAZING INCIDENCE X-RAY FLUORESCENCE MEASUREMENTS



Similar documents
X-ray diffraction techniques for thin films

h e l p s y o u C O N T R O L

Jorge E. Fernández Laboratory of Montecuccolino (DIENCA), Alma Mater Studiorum University of Bologna, via dei Colli, 16, Bologna, Italy

CALCULATION METHODS OF X-RAY SPECTRA: A COMPARATIVE STUDY

Laue lens for Nuclear Medicine

PHYSICAL METHODS, INSTRUMENTS AND MEASUREMENTS Vol. III - Surface Characterization - Marie-Geneviève Barthés-Labrousse

Applications of New, High Intensity X-Ray Optics - Normal and thin film diffraction using a parabolic, multilayer mirror

Atomic and Nuclear Physics Laboratory (Physics 4780)

X-ray thin-film measurement techniques

Glancing XRD and XRF for the Study of Texture Development in SmCo Based Films Sputtered Onto Silicon Substrates

BIG data big problems big opportunities Rudolf Dimper Head of Technical Infrastructure Division ESRF

Basic Concepts of X-ray X Fluorescence by Miguel Santiago, Scientific Instrumentation Specialist

Scanning Electron Microscopy: an overview on application and perspective

Raman spectroscopy Lecture

Passive Remote Sensing of Clouds from Airborne Platforms

Amptek Application Note XRF-1: XRF Spectra and Spectra Analysis Software By R.Redus, Chief Scientist, Amptek Inc, 2008.

2 Absorbing Solar Energy

STRUCTURAL STUDIES OF MULTIFERROIC THIN FILMS

Etudes in situ et ex situ de multicouches C/FePt

Secondary Ion Mass Spectrometry

Fundamentals of modern UV-visible spectroscopy. Presentation Materials

ON-STREAM XRF ANALYSIS OF HEAVY METALS AT PPM CONCENTRATIONS

Lectures about XRF (X-Ray Fluorescence)

EDS system. CRF Oxford Instruments INCA CRF EDAX Genesis EVEX- NanoAnalysis Table top system

Quantitative Analysis Software for X-Ray Fluorescence. XRF-FP is a full-featured quantitative analysis package for XRF

Introduction to X-Ray Powder Diffraction Data Analysis

6) How wide must a narrow slit be if the first diffraction minimum occurs at ±12 with laser light of 633 nm?

Acousto-optic modulator

Coating Thickness and Composition Analysis by Micro-EDXRF

Electron Microscopy 3. SEM. Image formation, detection, resolution, signal to noise ratio, interaction volume, contrasts

X-ray Diffraction and EBSD

Manual for simulation of EB processing. Software ModeRTL

X-ray Diffraction (XRD)

Stanford Rock Physics Laboratory - Gary Mavko. Basic Geophysical Concepts

EXPERIMENTAL CONDITIONS FOR CROSS SECTION MEASUREMENTS FOR ANALYTICAL PURPOSES. L. Csedreki 1. Abstract. I. Introduction

bulk 5. Surface Analysis Why surface Analysis? Introduction Methods: XPS, AES, RBS

Introduction to Powder X-Ray Diffraction History Basic Principles

Optical Design Tools for Backlight Displays

Lecture 2 Macroscopic Interactions Neutron Interactions and Applications Spring 2010

How To Understand Light And Color

Introduction to the Monte Carlo method

MODELING AND IMPLEMENTATION OF THE MECHANICAL SYSTEM AND CONTROL OF A CT WITH LOW ENERGY PROTON BEAM

Rapid structure determination of disordered materials: study of GeSe 2 glass

EDXRF of Used Automotive Catalytic Converters

Powder diffraction and synchrotron radiation

Does Quantum Mechanics Make Sense? Size

Reprint (R22) Avoiding Errors in UV Radiation Measurements. By Thomas C. Larason July Reprinted from Photonics Spectra, Laurin Publishing

X-Rays and Magnetism From Fundamentals to Nanoscale Dynamics

Vincent FAVRE-NICOLIN Univ. Grenoble Alpes & CEA Grenoble/INAC/SP2M XDISPE (ANR JCJC SIMI )

P R E A M B L E. Facilitated workshop problems for class discussion (1.5 hours)

Graduate Student Presentations

Proton tracking for medical imaging and dosimetry

Physics 441/2: Transmission Electron Microscope

Spectral distribution from end window X-ray tubes

The Role of Electric Polarization in Nonlinear optics

STAR: State of the art

Improved predictive modeling of white LEDs with accurate luminescence simulation and practical inputs

Chapter 8. Low energy ion scattering study of Fe 4 N on Cu(100)

GRID AND PRISM SPECTROMETERS

Preface Light Microscopy X-ray Diffraction Methods

Analytical Techniques for Trace Elemental Analyses on Wafer Surfaces for Monitoring and Controlling Contamination

Coating Technology: Evaporation Vs Sputtering

Nanoelectronics 09. Atsufumi Hirohata Department of Electronics. Quick Review over the Last Lecture

PUMPED Nd:YAG LASER. Last Revision: August 21, 2007

Introduction to Energy Dispersive X-ray Spectrometry (EDS)

Cross section, Flux, Luminosity, Scattering Rates

Polarization Dependence in X-ray Spectroscopy and Scattering. S P Collins et al Diamond Light Source UK

Clinical Photon Beams

Bruker AXS. D2 PHASER Diffraction Solutions XRD. think forward

Diffractive Optical Elements (DOE) for FLEXPOINT Laser Modules

A PHOTOGRAMMETRIC APPRAOCH FOR AUTOMATIC TRAFFIC ASSESSMENT USING CONVENTIONAL CCTV CAMERA

The promise of ultrasonic phased arrays and the role of modeling in specifying systems

Physical Properties and Functionalization of Low-Dimensional Materials

Production of X-rays. Radiation Safety Training for Analytical X-Ray Devices Module 9

Scanning Near Field Optical Microscopy: Principle, Instrumentation and Applications

Diffraction Course Series 2015

Optical Properties of Sputtered Tantalum Nitride Films Determined by Spectroscopic Ellipsometry

Crystal Structure of High Temperature Superconductors. Marie Nelson East Orange Campus High School NJIT Professor: Trevor Tyson

GAFCHROMIC DOSIMETRY MEDIA TYPE MD-V3

Experiment #5: Qualitative Absorption Spectroscopy

Chemical Sputtering. von Kohlenstoff durch Wasserstoff. W. Jacob

POWDER X-RAY DIFFRACTION: STRUCTURAL DETERMINATION OF ALKALI HALIDE SALTS

- thus, the total number of atoms per second that absorb a photon is

Near-field scanning optical microscopy (SNOM)

Robert G. Hunsperger. Integrated Optics. Theory and Technology. Fourth Edition. With 195 Figures and 17 Tables. Springer

Dose enhancement near metal electrodes in diamond X- ray detectors. A. Lohstroh*, and D. Alamoudi

Fiber Optics: Fiber Basics

Sputtering by Particle Bombardment I

ESRF Upgrade Phase II: le nuove opportunitá per le linee da magnete curvante

Excimer Laser Technology

DETECTION OF SUBSURFACE DAMAGE IN OPTICAL TRANSPARENT MATERIALSS USING SHORT COHERENCE TOMOGRAPHY. Rainer Boerret, Dominik Wiedemann, Andreas Kelm

Appendix A. An Overview of Monte Carlo N-Particle Software

Waves - Transverse and Longitudinal Waves

1090 IEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 50, NO. 4, AUGUST Intelligent Gamma-Ray Spectroscopy Using 3-D Position-Sensitive Detectors

Electron spectroscopy Lecture Kai M. Siegbahn ( ) Nobel Price 1981 High resolution Electron Spectroscopy

Simultaneous data fitting in ARXPS

Transcription:

COMPARISON OF FOUR DATA ANALYSIS SOFTWARE FOR COMBINED X-RAY REFLECTIVITY AND GRAZING INCIDENCE X-RAY FLUORESCENCE MEASUREMENTS Bérenger Caby (1), Fabio Brigidi (2), Dieter Ingerle (3), Blanka Detlefs (1), Gaël Picot (1), Luca Lutterotti (2), Emmanuel Nolot (1), Giancarlo Pepponi (2), Christina Streli (3), Magali Morales (4), Daniel Chateigner (5) (1) CEA, LETI, MINATEC Campus, Grenoble, France (2) Fondazione Bruno Kessler, Trento, Italy (3) Atominstitut, Vienna University of Technology, Vienna, Austria (4) CIMAP, Caen, France (5) CRISMAT-Ensicaen, IUT-Caen UCBN, Caen, France

OUTLINE GiXRF XRR combined analysis Comparison of 4 data analysis software GIMPY, JGIXA, MAUD, MEDEPY Main features Key differences Material Database Sample definition Instrumental function XRR simulation GiXRF simulation Fitting capabilities Summary and outlook 2

NON-DESTRUCTIVE ELEMENTAL DEPTH PROFILING WITH X-RAYS Analysis of (ultra)thin layered films for advanced applications (micro/nano electronics, memory, photonics, PV, ) Analytical challenges Reduced material quantities limits of detection Material properties different from bulk non-existent standards Analysis of interfaces and buried layers destructive or indirect methods Accuracy, standardization Need for non-destructive depth-profiling method Avoid artifacts (preferential sputtering, atom mixing, implantation) Limited (if any) degradation of the sample On beamlines, in the Labs, in R&D cleanrooms, in industry Combined GIXRF/XRR? 3

GIXRF+XRR ANALYSIS 4

GIXRF+XRR DEPTH PROFILING Propagation of GiXRF-XRR requires : X-ray dedicated tools Optimized protocols Fundamental parameters (cross sections, absorption coefficients), densities, XSW enhancement Thicknesses of layers to fit Quantification of the XRF dose (geometrical factors) Same model for XRR and GiXRF : increase the level of information. Add constraints & reduce uncertainties Data reduction software 5

ANALYSIS SOFTWARE SOFTWARE AUTHORS KEY FEATURES REFERENCES GIMPY Grazing Incidence Material analysis with Python G. Pepponi, F. Brigidi XRR, XRF, GiXRF Integrated intensities JGIXA D. Ingerle XRR, GiXRF Integrated intensities MAUD Material Analysis Using Diffraction MEDEPY Material Elemental DEpth profiling using PYthon L. Lutterotti XRR, XRF, GiXRF, XRD Full spectrum B. Detlefs, G. Picot, E. Nolot, H. Rotella XRR, GIXRF, XSW Integrated intensities TXRF 15 : Frid. 10.10 am Spectrochimica Acta Part B 99 (2014) 121 128 TXRF 15 : Wed. 3.30 pm Nuclear Inst. and Methods in Physics Research, B, 268, 334-340, 2010 http://maud.radiographema.c om/ TXRF 15 : Frid. 9.30 am 6

OVERVIEW Common points XRR based on Parrat formalism (L. G. Parratt, Phys. Rev., vol. 95, no. 2, p.359, 1954) GiXRF based on De Boer formalism (D. K. G. de Boer, http://dx.doi.org/10.1103/physrevb.44.498) Key differences XRF : full spectrum vs integrated intensity Additional SW (e.g PyMCA) is required to extract the integrated XRF intensities for each angle / each XRF line Material database Sample definition Instrumental function Other features (simulation & fitting modules) 7

MATERIAL DATABASE The values of parameters such as: Fluorescence yield, Atomic scattering factors, Photoelectric, elastic and inelastic scattering cross sections may not be constant over publications / material database SOFTWARE MATERIAL DATABASE GIMPY, JGIXA, MAUD https://data-minalab.fbk.eu/txrf/xraydata/element/ MEDEPY User defined Xray Lib (http://ftp.esrf.eu/pub/scisoft/xraylib/readme.html) 8

MATERIAL DATABASE NiO 2 (5nm, d=6.0g/cc) Ni (50 nm, d=8.9 g/cc) Si (sub, d=2.33 g/cc) 9

SAMPLE DEFINITION SOFTWARE PARAMETERS REMARKS GIMPY, JGIXA Thickness Roughness Mass density Stoichiometry No correlation between mass density and stoichiometry MAUD MEDEPY Thickness Roughness Phase Stoichiometry Thickness Roughness Mass density or atomic density Stoichiometry XRD-based definition of the sample structure Compatible with XRR- GiXRF-XRD combined analysis Mass density and stoichiometry are correlated GENX-based definition 10

SAMPLE DEFINITION (MAUD) 11

INSTRUMENTAL FUNCTION XRR Divergence ~ overall resolution GiXRF Divergence (convolution ~ approximation ) Geometrical correction 12

GEOMETRICAL CORRECTION Geometrical correction Acceptance function (detected area corrected by solid angle of detection) Spatial intensity distribution of the incident beam (e.g gaussian) theta-theta configuration Detector angle = 90 W. Li et al, Review of Scientific Instruments 83, 053114 (2012) 13

GEOMETRICAL CORRECTION theta-theta configuration Detector angle 90 theta-2theta configuration Detector angle 90 14

ACCEPTANCE FUNCTION JGIXA Rectangular function (width L d ) Parameter = L d 1/cos(θ) correction for θ-2θ geometry GIMPY, MEDEPY Parameters d 1, d 2, d p Heumans lambda function (solid angle of detection) Independent (resp. dependent) of theta in θ-θ (resp. θ-2θ) geometry 15

GEOMETRICAL CORRECTION W Li et al, Reviewof Scientific Instruments 83, 053114 (2012) GIMPY MEDEPY 16

SIMULATION XRR simulation GiXRF simulation For NiO 2 /Ni/Si subcase studywherethicknesses, densitiesand roughness werevariedand when usingthe samedatabase: the simulated XRR data obtained with the 4 different software were found almost perfectly identical the simulatedgixrfdata obtainedwith the 4 different software on a «perfect» tool(no divergence, no instrumental function) were found almost perfectly identical Impact of the instrumental function (overall divergence) is almost perfectly identical for the different software Limiteddiscrepancy induced by divergence Significant impact of the geometrical correction Only GIMPY includes secondary fluorescence 17

FITTING CAPABILITIES SOFTWARE CAPABILITIES REMARKS GIMPY Fitting module under development JGIXA Combinedfitting of XRR and GiXRF datasets acquired at the sameenergy MAUD Unique capability for XRR- XRD-GiXRF combined analysis Stoichiometry MEDEPY Combined fitting of various XRR and GiXRF datasets acquired at various energies Stoichiometry Fast and user friendly Monochromatic primary radiation Full spectrum only GiXRFinstrumental function to be corrected! Monochromatic and polychromatic primary radiation Monochromatic primary radiation Stillunderoptimization(definition of FOM for combined analysis ) 18

SUMMARY AND OUTLOOK Analysis of (ultra)thin layered films for advanced applications (micro/nano electronics, memory, photonics, PV, ) Need for combined GIXRF/XRR as a non-destructive depth-profiling method On beamlines, in the Labs, in R&D cleanrooms, in industry GiXRF/XRR software 4 powerful software have been tested Need for standardization (reduced instrumental function ) in order to meet the needs for depth-dependent quantitative analysis in Labs, R&D facilities and industry 19

Thank you for your attention!