X-RAY ENERGY DISPERSIVE SPECTROSCOPY: OVERVIEW...

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X-RAY ENERGY DISPERSIVE SPECTROSCOPY: OVERVIEW, APPLICATIONS, & ANALYSIS DAVE STALLA, M.S. SENIOR RESEARCH TECHNICIAN, ELECTRON MICROSCOPY CORE & PH.D. CANDIDATE, PHYSICS UNIVERSITY OF MISSOURI Electron Microscopy Core University of Missouri

Transcript of X-RAY ENERGY DISPERSIVE SPECTROSCOPY: OVERVIEW...

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X - R AY E N E R G Y D I S P E R S I V E S P E C T RO S C O P Y: OV E RV I E W, A P P L I C AT I O N S , & A N A LYS I S

D AV E S TA L L A , M . S .

S E N I O R R E S E A R C H T E C H N I C I A N , E L E C T RO N M I C RO S C O P Y C O R E

& P H . D. C A N D I D AT E , P H Y S I C S

U N I V E R S I T Y O F M I S S O U R I

Electron Microscopy CoreUniversity of Missouri

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ABOUT ME

• Ph.D candidate in physics (ant. grad: June 2017) with Prof. Peter Pfeifer

– Dissertation focuses on H2 and CH4 storage via adsorption in carbonaceous materials

– Characterization: XPS, XRD, U/SAXS, U/SANS, PGAA, FTIR, N2 sorption (BET)

– Experience with synthesizing raw (high-Σ carbons) and functionalized (B-doped carbons, bulk C3N4)

materials

– Technical experience includes Mathematica programming and Arduino microcontroller

design/implementation

• Hired as Senior Research Technician 9/2016

– EMC user since 2010

– Travelled to Bruker HQ 11/14-17 for “Nano Analytics QUANTAX User School”

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E-BEAM INTERACTIONQuanta/Hitachi/Scios

JEOL/F30

F30

Quanta/Hitachi/Scios/F30

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CHARACTERISTIC X-RAYS

e- beam

incident electron

secondary electron

generation

Incident electrons scatter

electrons from the

sample, resulting in

secondary electron

generation for imaging.

The electron ejection

results in a vacancy in it’s

former orbital.

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CHARACTERISTIC X-RAYS

e- beam

Ex-ray = Eshell1 – Eshell2

Electrons from higher orbitals

will fill this vacancy as is

energetically favorable.

As the electron jumps to a

lower energy state, it emits the

excess energy (ΔE) in the form of an x-ray photon.

The energies associated with these transitions are unique and well-tabulated.

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CHARACTERISTIC X-RAYS

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SI-LI VS. SDD

SDD design – significant improvements to collection efficiency!

capable of detecting elements as low as B

Si-Li detectors: ~10,000-20,000 CPS, above which data becomes unreliable

SDD detectors: routinely >100,000 CPS

specifications list upwards of 1,500,000 CPS possible

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HIGH THROUGHPUT ON BRUKER EDS SYSTEM AT EMC

High count rate (routinely work at ~150-200kcps) generates remarkable

data output - with the exception of mapping, quantifiable EDS data

collection comprises a marginal amount of instrument time.

Bruker Esprit – powerful microanalysis suite associated with the

QUANTAX detector. Unlimited network license allows users to the

software on their own machines and process data offsite: all instrument

time can be dedicated to maximizing the amount of data collected!

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ESPRIT: 4 MAIN ANALYSES

Increasing

spatial

information

‘Higher order’ analyses retain

functionalities of earlier ones

Windowed mode

Fullscreen mode

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I. SPECTRUM COLLECTION

• Collects a spectrum

across the entire

imaged area

• ~20s / scan

• Peak deconvolution

aids in identification

from overlapping

features

• Standards-based &

standardless quant.

available

• Many options for

easy plot generation

and exporting

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SPECTRUM ACQUISITION

• Total counts in spectrum

• Fixed real/live time

• Counts across a particular element’s

energy region

• Manual: collect until requisite statistics are

achieved

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PEAK IDENTIFICATION

• Manual selection of elements

• Auto ID for well-resolved features

• Finder tool: highlight a region, and the

software will list lines that fall within that

region in order of ‘likelihood’: α > β > γ,

distance from line from the center of the

region, etc

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ONLINE PEAK DECONVOLUTION

Initial assignments appear

to successfully account

for all features present

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ONLINE PEAK DECONVOLUTION

Reconstruction of elemental lines

shows that Kβ signals (calculated from associated Kα lines) don’t account for all detected counts

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ONLINE PEAK DECONVOLUTION

Deconvolution indicates

the presence of Mn and V

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II. OBJECT ANALYSIS

User-defined

regions:

• Point

• Rectangle

• Oval

• Freeform

polygon

• Iterative

auto grid

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III. LINE ANALYSIS

• Collects elemental

profiles across a

user-defined line

• Good for analyzing

phase interfaces

and non-discrete

boundaries

• ~5min / scan

• Can generate/

analyze/quantify a

spectrum across

entire line or a

selected segment

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IV. HYPERMAPPING

• Distinct from traditional

elemental maps, which

was essentially ‘filtered’

imaging: elements

predetermined &

individually collected

• Collected as a data cube:

spatial information from

pixels in x & y, each with

associated spectral

information (“z-axis”)

• A single collection yields

virtually limitless data

upon post-processing

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IV. HYPERMAPPING

• MASSIVE amount of data

(600x400 image has 240k

individual spectra) – most

versatile method

• Elemental maps

• Object analysis

• Line analysis

• Phase deconvolution

• ~10-20 min / region

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INDIVIDUAL/COMPOSITE MAPS

Can generate individual and

composite maps for any

combination of elements

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PHASE ANALYSIS

Identify discrete chemical phases via CPU-aided

analysis or manual assignment

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ELEMENTAL HEAT MAP

BSE Image Standard Al Map

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ELEMENTAL HEAT MAP

BSE Image Standard Al Map

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MAXIMUM PIXEL SPECTRUMReference BSE Image Associated elemental map

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MAXIMUM PIXEL SPECTRUM

Maximum pixel spectrum

Indicates the presence of several

additional elements, each of which may

only exist in single-digit no. of pixels

Net hypermap spectrum

Represents the sum of each energy

channel’s counts across ALL analyzed

pixels – high spatial concentrations

dominate

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MAXIMUM PIXEL SPECTRUMReference BSE Image ‘Trace’ features map

Most features comprise significantly less than 0.1wt% in the bulk, below the accepted detection limit of EDS

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PARTICLE ANALYSIS

• Image analysis utility independent of X-ray data

• Particles are partitioned from CPU-aided filtering and binarization

• A number of different geometric characteristics can be quantified

• May be followed by EDS measurements in defined particle regions for joint particle/phase

analysis

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PARTICLE ANALYSIS

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VARIABLE Z

15 mm4 mm

WD = 9mm WD = 50mm

Field of view is limited by working distance; most EDS systems

require a fixed WD for sufficient counting (detector must be

pointed at sample surface). EMC QUANTAX system is capable of

alignment to longer working distances for wider analysis regions