Post on 22-Mar-2020
MEN
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Secondary ion mass spectrometrySecondary ion mass spectrometry (SIMS)(SIMS)
Lasse
Vines
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Secondary ion mass spectrometrySecondary ion mass spectrometry
0 20 40 60 80 1001
10
100
1000
10000
Cou
nts/
sec
Mass (AMU)
Li
OO2
K
Zn
ZnO
ZnO2
Na Cr
1014
1015
1016
1017
1018
1019
1020
1021
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7
PBAs
Atom
ic c
once
ntra
tion
(cm
-3)
Depth (um)
Si07
Ge0.3
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ChemicalChemical identificationidentification
Impurity
identification Isotope ratio
64Zn 66Zn67Zn
68Zn
70Zn
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Characterization of device structureCharacterization of device structure
1014
1015
1016
1017
1018
1019
1020
1021
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7
PBAs
Atom
ic c
once
ntra
tion
(cm
-3)
Depth (um)
Si07
Ge0.3
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Characterization of solar cellCharacterization of solar cell
Characterization•Optimization of processing•Trouble shooting
1,2
1,0
0,8
0,6
0,4
0,2
0,01E16 1E17 1E18 1E19 1E20
Dep
th (µ
m)
P Concentration (cm-3)
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Ion Ion imagingimaging
Na distribution
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OutlineOutline
•
Characteristic features–
Comparison with other techniques
•
Physical processes–
Sputtering
–
Ionization
•
SIMS instrumentation–
Types of mass spectrometers
–
Measurement modes: Mass spectra, Depth profiling, Ion imaging
•
Examples of applications–
Diffusion studies
–
Material development
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Characteristic featuresCharacteristic features
•
Quantitative chemical analysis•
High detection sensitivity–
1016
– 1013
atoms/cm3 (ppm-ppb)–
Can measure H
•
Large dynamic range–
> 5 orders of magnitude
•
Very high depth resolution–
Resolution of 20 Å
can be obtained
•
Ion microscopy–
Lateral resolution < 0.5 µm
But,•
Limited to concentration <5%
•
Samples must be vacuum compatible •
Samples must be partially conductive
•
Destructive technique
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Comparison to other techniquesComparison to other techniques
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OutlineOutline
•
Characteristic features–
Comparison with other techniques
•
Physical processes–
Sputtering
–
Ionization
•
SIMS instrumentation–
Types of mass spectrometers
–
Measurement modes: Mass spectra, Depth profiling, Ion imaging
•
Examples of applications–
Diffusion studies
–
Material development
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Ion Ion –– solid interactionsolid interaction
Matrix atom
Impurityatom
Primary ion
Secondary ions are accelerated by an applied sample voltage
Primary beam
Energy is transferred from the energetic primary ions to atoms in the sample. Some of these receive enough energy to escape the sample.
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SputteringSputtering
Sigmund P. Theory of Sputtering, Phys. Rev. 184(2), 383 (1969)
Sputtering Yield:number of sputtered atoms per incoming ion
it
in
0
iti E
ESUKES
8/3n 383/1ln5.0 S
Sputtering yield:
50.05for 3
keV5.321
it6/5
tiit
2/13/2t
3/2ititiit
ZZZZK
ZZZZMME
Mi , Zi : Ion mass and atomic numberMt , Zt : Target mass and atomic numberU0 : Surface escape barrier in eVEi : Ion energy
Nuclear stopping cross-section:Sputtering is a multiple collision process involving a cascade of moving target atoms, this cascade may extend over a considerable region inside the target.
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SputteringSputtering
•
Dependence of ion
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SputteringSputtering
•
Example of dependence of target on sputtering yield: (Si1-x
Gex
)
0 20 40 60 80 100
1
2
3
Nor
mal
ized
ion
yiel
d
Ge content (%)
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SputteringSputtering
•
Example of sputtering of polycrystalline Fe surface
The erosion rate is different for the different grains: Sputtering yield vary with the crystal orientation
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SputteringSputtering
•
Example of sputtering yield:
200 µm
0 100 200 300 400 500
-1,0
-0,8
-0,6
-0,4
-0,2
0,0
Dep
th (µ
m)
Width (µm)
Material removed: 1200200 µ3
= 410-8
cm3
≈
21015
atoms
Current: 200 nASputtering time: 700 sec
Incoming ions: 20010-9A
6.241018
ions/C
700 sec = 9x1014
ions
Sputtering Yield = 2.2 atoms/ion
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Sputtering Sputtering –– Secondary ionsSecondary ions
•
Energy distribution of secondary ions
0 20 40 60 80 10010
100
1000
10000
100000
28Si4
28Si3
28Si2
Sec
onda
ry in
tens
ity (a
rb. u
nit)
Energy (eV)
28Si
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IonizationIonization
•
Ion yield/ionization efficiency : The fraction of sputtered ions that becomes ionized.
•
Ion yield can generally not be predicted theoretically.•
Ion yield can vary by several orders of magnitude depending on element and chemistry of the sputtered surface.
•
Oxygen on the surface will increase positive ion yield•
Cesium on the surface will increase negative ion yield
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IonizationIonizationNegative secondary
Positive secondary
vAC
vEC i
/exp YieldIon Negative
/exp YieldIon Positive
EiA
C±: Constantsv: velocity perpendicular to surface: work function
(Cs)
(O)
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IonizationIonization
64 66 68 70100
101
102
103
104
105
106
107
Sec
onda
ry In
tens
ity(c
ps)
M/q (AMU)
Negative modePositive mode
Mass
spectrum
of ZnO, Zn peaks.64Zn
(48.6%)66Zn
(27.9%)
67Zn
(4.1%)
68Zn
(18.8%)
70Zn
(0.6%)
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IonizationIonization
0.4
0.5
0.6
0.7
0.8
0.9
1
1.1
0 20 40 60 80 100
Nor
mal
ized
P- - y
ield
Ge concentration (%)
Phosphorus in Si1-x Gex
•
Limits the quantification procedure:–
SIMS is mainly a tool for measuring small concentrations in a given matrix
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General YieldGeneral Yield
•
Measured intensity It for a specific target atom
TCYII ttPt
IP : Primary ion current Y : Sputtering yield
(number of sputtered particles per impinging primary ion)
[Ct ]: Concentration of species t t : Secondary ion formation and
survival probability (ionization efficiency)
T: Instrument transmission function
t
is highly dependent on species and matrix
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OutlineOutline
•
Characteristic features–
Comparison with other techniques
•
Physical processes–
Sputtering
–
Ionization
•
SIMS instrumentation–
Types of mass spectrometers
–
Measurement modes: Mass spectra, Depth profiling, Ion imaging
•
Examples of applications–
Diffusion studies
–
Material development
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The SIMS instrumentThe SIMS instrument
Focused
ion beamMass
Spectrometer
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The SIMS instrumentThe SIMS instrument
•
Instruments are usually classified by the type of mass spectrometer:–
Time of Flight•
Simultaneous detection of many elements
•
High transmission•
Measures large molecules
–
Quadrupole•
Low impact energy
–
Magnetic Sector•
High mass resolution
•
High transmission•
Low detection limit
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Time of Time of FlightFlight SIMSSIMS
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QuadrupoleQuadrupole SIMSSIMS
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Magnetic sector Magnetic sector -- mass mass spectrometer spectrometer
sample
detector
ion source
electrostatic sector analyser
magnetic sector analyser
Primary beam
Seco
ndar
y be
amre rm
E0B
Lorenz’ force: BvEF qq
Centripetal force:rr
mv rF2
2
e0 r
mvqE
Electrostaticsector analyser
2
mrmvqvB
Magneticsector analyser
2
0e
m
ErBr
qm
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Secondary ion mass spectrometrySecondary ion mass spectrometry
2m
0 e
Brmq E r
sample
detector
ion source
electrostatic sector analyser
magnetic sector analyser
Primary beam
Seco
ndar
y be
am
re rm
E0B
0 100 200 300 400 500 6001
10
100
1000
10000
Inte
nsity
(cou
nts/
sec)
Sputter time (sec)
Depth profile
0 20 40 60 80 1001
10
100
1000
10000
Cou
nts/
sec
Mass (AMU)
Mass spectrum
Ion image
20 µm
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InstrumentationInstrumentationion sources
sample chamber
electrostatic
sector
analysermagnetic
sector
analyser
detectors
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MassMass spectrumspectrum
0 20 40 60 80 1001
10
100
1000
10000
Cou
nts/
sec
Mass (AMU)
Li
OO2
K
Zn
ZnO
ZnO2
Na Cr
Mass
spectrum
of a ZnO-sample
with
traces of Li, Na, K, and Cr.
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MassMass InterferenceInterference
11,5 12,0 12,5 13,0 13,5
100
101
102
103
104
105
106
Sec
onda
ry in
tens
ity (c
ps)
Mass (AMU)
Mass
spectrum of graphite
91.6%
8.4%
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Mass interferenceMass interference
•
Several ions/ionic molecules have similar mass to charge ratios:
10B -
30Si3+ Monitor 11B
75As - 29Si30Si16O
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Energy selectionEnergy selectionelectrostatic sector analyser
Seco
ndar
y be
am
re
E0
2
e0 r
mvqE
Increasing kinetic energy
Energy selection slit
Ejection energy (eV)lo
g (
ion
in
ten
sity
)
75As
29Si30Si16O
0 50 100
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MassMass interferenceinterference
•
Several
ions/ionic
molecules
have similar mass
to charge
ratios:
10B -
30Si3+ Monitor 11B
75As - 29Si30Si16O Energy selection
31P - 30Si1H
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HighHigh massmass resolutionresolution
30,85 30,90 30,95 31,00 31,05 31,10
100
1000
10000
Inte
nsity
(cou
nts/
sec)
Mass (AMU)
magnetic sector analyser
rm
B
2
mrmvqvB
Exit slit
Discriminating
between
31P and 30Si1H:
M(31P) = 30.973761M(30Si1H) =30.98160
30,85 30,90 30,95 31,00 31,05 31,10
100
1000
10000
Inte
nsity
(cou
nts/
sec)
Mass (AMU)
31P
30Si1H
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Mass interferenceMass interference
•
Several ions/ionic molecules have similar mass to charge ratios:
10B -
30Si3+ Monitor 11B
75As - 29Si30Si16O Energy selection
31P - 30Si1H High mass resolution
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SIMS SIMS –– depth profilingdepth profiling
0 100 200 300 400 500 6001
10
100
1000
10000
Inte
nsity
(cou
nts/
sec)
Sputter time (sec)
Primary beam
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0 100 200 300 400 500 600 700
1
10
100
Inte
nsity
(cou
nts/
sec)
Sputter time (sec)
CalibrationCalibration of of depthdepth profilesprofiles
”Raw”
phosphorus
profile
0 100 200 300 400 500
-1,0
-0,8
-0,6
-0,4
-0,2
0,0
Dep
th (µ
m)
Width (µm)
Depth calibration
Sputter time: 700 sec Depth: 9310 Å
Erosion rate:13,3 Å/sec
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0 100 200 300 400 500 600 700
1
10
100
Inte
nsity
(cou
nts/
sec)
Sputter time (sec)
CalibrationCalibration of of depthdepth profilesprofiles
TCYII ttPt
”Raw”
phosphorus
profile
t1 CS
S: Sensitivity
factor
0 100 200 300 400 500 6000,1
1
10
100
1000
10000
Inte
nsity
(cou
nts/
sec)
Sputter time (sec)
Concentration calibration
Ion implanted sample:P dose 1e15 P/cm2
sensitivity factor:Relate the intensity to atomic concentration
xxIS
d Dose
Sensitivity factor:1 count/sec = 3,41015
P/cm3
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Calibration of depth profilesCalibration of depth profiles
0,0 0,2 0,4 0,6 0,81E14
1E15
1E16
1E17
1E18
P co
ncen
tratio
n (c
m-3)
Depth (µm)0 100 200 300 400 500 600 700
1
10
100
Inte
nsity
(cou
nts/
sec)
Sputter time (sec)
”Raw”
phosphorus profile
Calibratedphosphorus profile
Erosion rate:13,3 Å/sec
Sensitivity factor:1 count/sec = 3,41015
P/cm3
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Ion imagingIon imaging
Distribution of given atoms at the surface
Primary
beam
Secondary beam to detector
Intensity recorded as a function of primary beam position
Sample Surface
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Ion Ion imagingimaging