ligo-t1000126-v1 rand dannenberg 1 some defect counting microscope results – lessons learned dark...
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LIGO-T1000126-v1Rand Dannenberg
1
Some Defect Counting Microscope Results – Lessons
LearnedDark Field Particle Counting on
LMA Micromap Sample&
Tinsley Scatter Master Sample
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LIGO-T1000126-v1Rand Dannenberg
2
LMA Micromap Sample
• 3” diameter fused silica.
• 20X objective, 99 frames analyzed - 26.8 mm2 total area.
• Histogram bin size varied: 2 um, 0.5 um, 0.1 um.
• Same Data manipulated from single map for fixed microscope, contrast & analysis settings.Same Data manipulated from single map for fixed microscope, contrast & analysis settings.
• Goal was to understand binning.
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LIGO-T1000126-v1Rand Dannenberg
3
LMA Micromap Sample – Binning: the result can be made nearly independent of the bin size by dividing by the bin size. Below, the results are NOT normalized to a bin size.
All 20x Objective, bin size varies
0
100
200
300
400
500
600
700
0 5 10 15 20 25 30 35
Equidiameter (um)
De
fec
t D
en
sit
y (
co
un
t/m
m2 )
20X - 2 um bins
20X - 0.5 um bins
20X - 0.1 um bins
All 20x Objective, bin size varies
0.01
0.1
1
10
100
1000
0 5 10 15 20 25 30 35
Equidiameter (um)
De
fec
t D
en
sit
y (
co
un
t/m
m2
)
20X - 2 um bins
20X - 0.5 um bins
20X - 0.1 um bins
scannedtotalA
bEcountsbEDensity
_
),(),(
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LIGO-T1000126-v1Rand Dannenberg
4
LMA Micromap Sample – Binning: By dividing by the bin size (in microns) the defect density is normalized to a bin size of 1 micron. Larger bin sizes then serve to integrate the data and reduce noise.
All 20x Objective, bin size varies
0
200
400
600
800
1000
1200
1400
1600
1800
2000
0 5 10 15 20 25 30 35
Equidiameter (um)
De
fec
t D
en
sit
y (
co
un
t/m
m2 )
No
rma
lize
d t
o 1
um
bin
20X - 2 um bins / bin size
20X - 0.5 um bins / bin size
20X - 0.1 um bins / bin size
All 20x Objective, bin size varies
0.01
0.1
1
10
100
1000
10000
0 5 10 15 20 25 30 35
Equidiameter (um)
De
fec
t D
en
sit
y (
co
un
t/m
m2 )
No
rma
lize
d t
o 1
um
bin
20X - 2 um bins / bin size
20X - 0.5 um bins / bin size
20X - 0.1 um bins / bin size
bA
bEcountsbENormDensity
scannedtotal
1),(),(_
_
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LIGO-T1000126-v1Rand Dannenberg
5
LMA Micromap Sample – Conversion of the bin-normalized defect density to a fraction of area covered is done by multiplying by the average defect size S in a bin range at each equidiameter E. The b is the bin size. This produces a peak at the most important equidiameter. Note the peak position is slightly dependent on the bin size. The micromap
sample has mostly small defects 1.1 um < E < 1.5 um, discernable with the smaller bin sizes. Bin sizes that are too big give higher peak values (the 2 um bin has a peak near 3.5 um equidiameter).
),(1),(
),(
2
)(
2
1),(
_
2
bESbA
bEcountsbEFC
bEEbES
scannedtotal
All 20x Objective, bin size varies
0
0.0001
0.0002
0.0003
0.0004
0.0005
0.0006
0.0007
0.0008
0 5 10 15 20 25 30 35
Equidiameter (um)
Fra
ctio
n C
ove
rag
e N
orm
aliz
ed t
o 1
um
bin
Fraction Coverage Norm to 1 um bin (2 um bin)
Fraction Coverage Norm to 1 um bin (0.5 umbin)
Fraction Coverage Norm to 1 um bin (0.1 umbin)
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LIGO-T1000126-v1Rand Dannenberg
6
LMA Micromap Sample – Integrating over equidiameter then gives the cumulative coverage fraction.
Very weakly bin size dependent.
EE
bSbDensitybFCbbEFCCumulative
00
),(),(),(),(_
0
0.0005
0.001
0.0015
0.002
0.0025
0.003
0 5 10 15 20 25 30 35
Equidiameter (um)
Cu
mu
lati
ve
Co
ve
rag
e F
rac
tio
n
Cumulative Coverage Fraction - 2 um bin
Cumulative Coverage Fraction - 0.5 um bin
Cumulative Coverage Fraction - 0.1 um bin
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LIGO-T1000126-v1Rand Dannenberg
7
Tinsley Scatter Master Sample
• 1” x 3” microscope slide.
• 20X objective, 99 frames analyzed - 26.8 mm2 total area.
• 5X objective, 24 frames analyzed – 102 mm2 total area.
• Histogram bin size fixed at 0.5 um.
• Contrast (exposure time) must change on changing magnification,Contrast (exposure time) must change on changing magnification,
• Analysis settings (threshold + restrictions) must also change.Analysis settings (threshold + restrictions) must also change.
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LIGO-T1000126-v1Rand Dannenberg
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Tinsley Scatter Sample – Defect density normalized to 1 micron bin.
Objective Lens varies, bin size fixed
0
50
100
150
200
250
0 5 10 15 20 25 30 35
Equidiameter (um)
Def
ect
Den
sity
(co
un
t/m
m2)
No
rmal
ized
to
1 u
m b
in
5X Obj (count/mm^2)/(bin size)
20X Obj (count/mm^2)/(bin size)
Objective Lens varies, bin size fixed
0.01
0.1
1
10
100
1000
0 5 10 15 20 25 30 35
Equidiameter (um)
Def
ect
Den
sity
(co
un
t/m
m2)
No
rmal
ized
to
1 u
m b
in
5X Obj (count/mm^2)/(bin size)
20X Obj (count/mm^2)/(bin size)
Note that the 5X objective is more sensitive tolarger defects, the 20X objective is moresensitive to smaller ones, while in the mid-rangethey are in closer agreement.
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LIGO-T1000126-v1Rand Dannenberg
9
Tinsley Scatter Sample – Coverage Fraction normalized to 1 micron bin.
Objective Lens varies, bin size fixed
0
0.0002
0.0004
0.0006
0.0008
0.001
0.0012
0.0014
0 5 10 15 20 25 30 35
Equidiameter (um)
Fra
cti
on
Co
ve
rag
e N
orm
aliz
ed
to
1 u
m b
in
Fraction Coverage Norm to 1 um bin (0.5 um bin)- 20x
Fraction Coverage Norm to 1 um bin (0.5 um bin)- 5x
The peak range varies with the magnification. 5X is 13-16 um while at 20X the peak range is 7 – 11 um.
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LIGO-T1000126-v1Rand Dannenberg
10
Tinsley Scatter Master Sample – Integrating over equidiameter then gives the cumulative coverage fraction.
Strongly magnification dependent.
0
0.002
0.004
0.006
0.008
0.01
0.012
0.014
0 5 10 15 20 25 30 35
Equidiamter (um)
Cu
mu
lati
ve C
ove
rag
e F
ract
ion
Cumulative Coverage Fraction - 5X Obj
Cumulative Coverage Fraction - 20X Obj
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LIGO-T1000126-v1Rand Dannenberg
11
Conclusions
• The results thus far seem to be more strongly magnification dependent, and less strongly bin size dependent.
• For a sample type, the bin size and magnification should be standardized before comparing with a scatter measurement.
• How to standardize will come with experience in analyzing real samples that are routinely generated.