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    Apri l, 2005

    Microscopic Composition Measurement at NanoscaleMicroscopic Composition Measurement at Nanoscale

    DSSC Seminar

    Lin Wang

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    OutlineOutline

    General Introduction

    Energy Dispersive Spectroscopy (EDS)

    Wavelength Dispersive Spectroscopy (WDS) Electron Energy Loss Spectroscopy (EELS)

    Auger Electron Spectroscopy (AES)

    X-Ray Photoelectron Spectroscopy (XPS) Summary

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    General IntroductionGeneral Introduction

    When High Energy Electron Beam Meets MaterialWhen High Energy Electron Beam Meets Material

    By Analyzing Emitted X-RayEnergy Dispersive Spectroscopy (EDS) + SEM/ TEMWavelength Dispersive Spectroscopy (WDS) + SEM

    By Analyzing Inelastically Scattered ElectronsElectron Energy Loss Spectroscopy (EELS) +TEM

    By Analyzing Emitted Auger ElectronsAuger Electron Spectroscopy (AES)

    When XWhen X--Ray Meets MaterialRay Meets Material By Analyzing Emitted Photoelectrons

    X-Ray Photoelectron Spectroscopy (XPS)

    AnalyticalElectronMicroscope(AEM)

    SurfaceCharacterization

    Take a thin TransmittingSpecimen as an example

    {AEM with EDS}

    (AEM with EELS)

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    Principles of EDSPrinciples of EDS

    EnergyEnergy DispersiveDispersive (X(X--Ray) Spectroscopy (EDS)Ray) Spectroscopy (EDS)

    X-Ray counting is done by measuring the x-ray photon energies with aSi(Ni)solid state detector

    Different characteristic X-Ray lines of elements represent the typesand relative amounts of elements in the sample

    The number of counts of each peak may be converted to weightconcentration using standard (more accurate) or standardlesscalculations

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    Energy Resolution (Peak Broadening) measured by FWHM (Full Width

    at Half Maximum of the peak)

    Peak overlap

    Principles of EDS (cont.)Principles of EDS (cont.)

    With TEMWith SEM

    Gaussian Distribution

    Y=AAexp{-1/2*[(EA-E)/ ]2}

    FWHM=2.355

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    Application Examples of EDSApplication Examples of EDS

    EDS Line Profile Software automationallows simplified composition profiling atnanometer resolution using EDS.

    Sample: Si80Ge20 islands grown on Si at800C followed by Si capping.

    EDS Mapping - EDS Mapping allowsvisualization of the phase separationprocess, which can be coupled with point-by-point quantitative analysis.

    Sample: Cu50Ag50 ball milled at 230 C

    PointPoint

    AnalysisAnalysis11--D ProfilingD Profiling 22--D MappingD Mapping

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    Principles of WDSPrinciples of WDS

    WavelengthWavelength DispersiveDispersive (X(X--Ray) Spectroscopy (WDS)Ray) Spectroscopy (WDS)

    With SEM

    X-Ray counting is done by using a Bragg

    reflector to wavelength-filter the x-rays on their

    way to the detector

    Braggs Law

    N

    =2dsin

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    Capacities of WDSCapacities of WDS

    Advantages

    Superior spectral resolution (X10 times better than EDS)

    Can detect light element Z 4

    Can detects 0.1%-several ppm More accurate

    Disadvantages

    The equipment is more expensive

    More Time consuming

    More difficult to use

    Usage Identification of spectrally overlapped elements such as W or Ta in Si,

    or N in Ti Detect of low concentration species (down to 100 or even 10ppm)

    such as P or S in metals Analysis of Low atomic number elements such as oxidation in metals

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    Comparison between EDS&WDSComparison between EDS&WDS

    EDS: Normally detects Z 10(below

    Na) thus typically cant be

    detected O, N, C. Sometimes ifusing windowless or thin

    window it can detect Z 4

    Parallel technique

    Can quickly scan for a widerang of possible elements

    Good for use both with SEM orTEM specimen

    Time of a typical run take a few

    minutes

    WDS: Detects Z 4

    Serial technique

    slow but can provide excellentresolution

    Requires very high x-raygeneration rates thus TEM

    samples cant provide highcount (x-ray generation) rate

    Time of a typical run take hours

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    Principles of EELSPrinciples of EELS

    Electron Energy Loss Spectroscopy (EELS)Electron Energy Loss Spectroscopy (EELS)

    With TEM

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    Principles of EELS (continued)Principles of EELS (continued)

    Electron Energy Loss Spectroscopy (EELS)Electron Energy Loss Spectroscopy (EELS)

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    Capacities of EELSCapacities of EELS

    Usage

    Light element spectroscopy for concentration, electronic and chemicalstructure analysis at ultrahigh lateral resolution

    Sample Requirements

    Solids and specimens must be transparent to electrons with about 10-200nm thickness;

    sample size: 3mm diameter thin foil

    Not destructive to sample

    Limitation

    Range of elements: Z=3-92

    Lateral resolution: 1nm-10m, depending on the diameter of the incidentelectron probe size and the thickness of the specimen

    Sampling depth: with thickness of specimen 10-200nm

    Detection limits:10-21g

    Accuracy: with standards 1-2 at.%, without standards 10-20 at.%

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    Application Examples of EELSApplication Examples of EELS

    EELS Mapping - The breakdown of the Li/Ni ordering at the surfacecan be seen as changes in the EELS fine structure and Ni-to-O ratio.

    Sample: LiNi0.80Co0.20O2 from Li-Ion battery after aging

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    Principles of AESPrinciples of AES

    Auger Electron Spectroscopy (AES)Auger Electron Spectroscopy (AES)

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    Capacities of AESCapacities of AES

    Sample Requirements

    vacuum compatible materials

    no destruction except to electron beam sensitive materials and duringdepth profiling

    Vacuum Requirements: 10-10 torr

    Limitation

    Range of elements: All except H and He

    Lateral resolution: 10-30nm for Auger analysis and even less for imaging

    Sampling depth: 0.5-10nm

    Detection limits: 0.1-1at.% Accuracy: 30% if using published elemental sensitivity

    10% if using standards that closely resemble the sample

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    Applications of AESApplications of AES

    Composition analysis of the 0-3nm region near the surface for allelements except H and He

    Scanning Auger Microscopy

    Depth-composition profiling and thin film analysis High lateral resolution surface chemical analysis and

    inhomogeneity studies to determine compositional variations

    Surface diffusion and segregation

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    Principles of XPSPrinciples of XPS

    XX--Ray Photoelectron Spectroscopy (XPS)Ray Photoelectron Spectroscopy (XPS)

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    Capacities of XPSCapacities of XPS

    Sample Requirements

    vacuum compatible materials, flat samples preferred

    no destruction except to X-ray sensitive materials and during

    depth profiling

    Limitation

    Range of elements: All except H and He Lateral resolution: 5mm-75m

    Sampling depth:0.5-5nm

    Detection limits: 0.01-0.3at.%

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    Applications of XPSApplications of XPS

    Routinely used in industry and research whenever elemental orchemical state analysis is needed at surfaces and interfaces as well asspatial resolution requirements are not demanding (typically greaterthan 150m).

    Eg.s:

    examination for and identification of surface contaminations

    Evaluation of materials processing steps (cleaning, plasma etching, thermal

    oxidation, silicide thin-film formation etc.) Evaluation of thin-film coating or lubricants

    Failure analysis for adhesion between components(air oxidation , corrosionetc.)

    Tribological (or wear) activity

    Effectiveness of surface treatment of polymers or plastics

    Surface composition differences for alloys

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    SummarySummary

    All of the five methods can give both microscopic imaging functionand qualitative plus quantitative composition analysis function

    Quantitative composition measurement will be more accurate withstandards esp. standards in similar composition range

    For EDS, the major limitation is the peak broadening and light elementincapability

    For WDS, comparing with EDS, it has high spectral resolution but ittakes longer for each run

    EELS can detect light element and has a high lateral resolution

    AES and XPS are surface composition detection techniques but AEShas a nm-scale lateral resolution which is much better than XPS

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    ReferenceReference

    J. Goldstein, D. Newbury, D. Joy, C. Lyman, P. Echlin, E. Lifshin, L,Sawyer, J. Michael, Scanning Electron Microscopy and X-RayMicroanalysis, Kluwer Academic / Plenum Publishers (2003)

    C. Brundle, C. Evans, S. Wilson, L. Fitzpatrick, Encyclopedia ofMaterials Characterization, Butterworth-Heinemann (1992)

    D. Williams, C. Carter, Transmission Electron Microscopy, Pledum(1996)

    D. J. OConnor, B. A. Sexton, R.St. C. Smart, Surface Analysis Methods

    in Materials Science, Springer (2003) http://cmm.mrl.uiuc.edu/Gallery/STEM/STEMGallery.htm