X-RAY ENERGY DISPERSIVE SPECTROSCOPY: OVERVIEW...
Transcript of X-RAY ENERGY DISPERSIVE SPECTROSCOPY: OVERVIEW...
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
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”
E-BEAM INTERACTIONQuanta/Hitachi/Scios
JEOL/F30
F30
Quanta/Hitachi/Scios/F30
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.
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.
CHARACTERISTIC X-RAYS
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
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!
ESPRIT: 4 MAIN ANALYSES
Increasing
spatial
information
‘Higher order’ analyses retain
functionalities of earlier ones
Windowed mode
Fullscreen mode
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
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
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
ONLINE PEAK DECONVOLUTION
Initial assignments appear
to successfully account
for all features present
ONLINE PEAK DECONVOLUTION
Reconstruction of elemental lines
shows that Kβ signals (calculated from associated Kα lines) don’t account for all detected counts
ONLINE PEAK DECONVOLUTION
Deconvolution indicates
the presence of Mn and V
II. OBJECT ANALYSIS
User-defined
regions:
• Point
• Rectangle
• Oval
• Freeform
polygon
• Iterative
auto grid
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
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
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
INDIVIDUAL/COMPOSITE MAPS
Can generate individual and
composite maps for any
combination of elements
PHASE ANALYSIS
Identify discrete chemical phases via CPU-aided
analysis or manual assignment
ELEMENTAL HEAT MAP
BSE Image Standard Al Map
ELEMENTAL HEAT MAP
BSE Image Standard Al Map
MAXIMUM PIXEL SPECTRUMReference BSE Image Associated elemental map
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
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
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
PARTICLE ANALYSIS
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