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Nanotech 2011: Technical Proceedings of the 2011
Nanotechnology Conference and Expo
A Novel Method for Measuring the Sizes and Concentrations
of 5-500 nm Particles in Colloidal Suspensions
H. Gary Van Schooneveld, Mark R. Litchy and Donald C. Grant
CT Associates, Inc., 7121 Shady Oak Road, Eden Prairie, MN 55344, U.S.A.,
gary@ctassociatesinc.com, mark@ctassociatesinc.com, don@ctassociatesinc.com
ABSTRACT
Measurement of the sizes and concentration of particles
in colloidal suspensions has been a challenge particularly
for suspensions with particles smaller than 100 nanometers.
A new measurement technique has been developed that
allows for measurement of particles as small as 5
nanometers in these suspensions. This new approach,
uniquely combining proven techniques used for counting
and sizing aerosol particle size distributions (PSDs) with
nebulizer technology, has been developed to measure both
particle size and number concentration in concentrated
liquid suspensions. The technique has demonstrated the
ability to provide unique and useful PSD data for chemical
/mechanical planarization (CMP) slurries used extensively
in the micro-electronics industry. In addition, the ability to
measure filter retention of particles as small as 10
namometers has been demonstrated.
Keywords: nebulizer, SMPS, slurry, filtration,
nanoparticles
1 LIQUID NANOPARTICLE SIZING
(LNS) SYSTEM DESCRIPTION
The LNS (Figure 1) consists of an ultrafine nebulizer
and a scanning mobility particle sizer (SMPS). A colloidal
suspension is diluted on-line in ultrapure water (UPW) and
injected into the nebulizer. The nebulizer generates a
droplet distribution in filtered air. The resultant droplet
distribution is diluted and dried with additional filtered air
to form an aerosol laden with the particles originally in the
colloidal suspension. The aerosol PSD is then measured
using a commercially available SMPS system that is
capable of measuring particles as small as 3 nm in size. A
TSI Model 3936 SMPS was used to generate the data
provided in this paper.
The key to this measurement approach is the nebulizer.
Dissolved non-volatile residue in the suspension will form
particles when the droplets from the nebulizer are dried.
These residue particles can interfere with the particle
analysis.
Figure 1. Schematic of the liquid nanoparticle sizing (LNS) system
Dynamic Mobility
Analyzer (DMA)
Condensation Particle
Counter (CPC)CDA
UPW
Ultrafine
Nebulizer
Scanning Mobility Particle Sizer (SMPS)Particle
Aerosol
Nanoparticle
supension
Pressure
regulator
Drain
Neutralizer DMA CPC
monodispersed
aerosol
Nanotech 2011: Technical Proceedings of the 2011
Nanotechnology Conference and Expo
The nebulizer used in this system minimizes this effect
by producing droplets that are sufficiently small and
uniformly sized that particles formed from dissolved
materials in the droplets are small enough as to not
interfere with the particle size measurement. In addition,
the particle suspension is sufficiently dilute that no more
than one particle is present in each droplet. Also,
measuring under different operating conditions, the
instrument is capable of determining whether particles
measured are from initially dissolved or particle residue.
The LNS technique of measuring colloidal PSDs offers
many interesting capabilities. This technique measures
number concentrations, not relative particle concentrations
(that is, one size relative to another) and makes no
assumption regarding the shape of the PSD. The number-
weighted PSD measured may easily be converted to
alternative weightings such diameter (D), surface area
(D2
), or volume (D3
) weighted distributions. Since this
technique measures individual particles, it is highly
sensitive to measuring rather small changes in these
suspensions and is not affected by the optical properties
and density of the particles. Finally, the SMPS used to
size and count the particles is a well establish instrument
for measuring aerosols [1] and is even used to size NIST
particle standards [2].
2 SIZING ACCURACY
An example of the sizing accuracy of the LNS system
is shown in Figure 2. In this evaluation, particles of three
gold colloids (BBI Research, Madison, WI) were
measured individually. As seen in Table 1, the sizing
measurements correlate well with the manufacturer’s
sizing claims. Measurements of polystyrene latex (PSL)
and silica particles have also shown good agreement with
manufacturer’s claims [3].
Particle diameter (nm)
5 6 7 8 9 15 20 25 30 35 4010
Relativedifferentialconcentration
d(#/mL)/dlog(DP)
10 nm
20 nm
30 nm
Figure 2. Measurement of BBI gold nanoparticles
Mean (nm) CV (%) Mean (nm) CV (%)
10 9.3 < 15 8.4 13
20 20.3 < 8 20.8 7.4
30 30.3 < 8 30.5 7.3
Manufacturer measured
size
LNS measured
size
Nominal Size
(nm)
Table 1. Sizing comparison between BBI certificate of
analysis and LNS measurments
3 MEASUREMENT OF POLISHING
SLURRIES
The PSD of a tri-modal polishing slurry measured by
the LNS is presented in Figure 3. As discussed previously,
the LNS directly measures the sizes and numbers of
individual particles in the colloidal suspension. As such,
variations in concentration of specific size particles
amongst samples can readily be detected. Variations in
particle concentration can effect process efficacy (e.g.
effect material removal rates during polishing). In
comparison, Figure 4 presents the data from a DLS
instrument used to measure the the same polishing slurry.
The DLS is an ensemble measurement technique that
measures the properties of many particles simultaneously
and then fits the data to an assumed lognormal PSD. In
addition, only relative particle concentrations are provided.
Scanning electron microscopy (SEM) of the slurry
confirms the tri-modal PSD (Figure 5).
Particle diameter (nm)
20 30 40 50 60 70 80 9010 100
Differentialvolumeconcentration
d(nm3
/mL)/dlog(DP
)
0
2e+15
4e+15
6e+15
8e+15
1e+16
1e+16
1e+16
2e+16
2e+16
2e+16
Figure 3. Measurement of a tri-modal polishing slurry by
the LNS system
Nanotech 2011: Technical Proceedings of the 2011
Nanotechnology Conference and Expo
Particle diameter (nm)
20 30 40 50 60 70 80 9010 100
Relativeconcentration
0.00
0.25
0.50
0.75
1.00
Figure 4. Measurement of a tri-modal polishing slurry
by a DLS system
Figure 5. Measurement of a tri-modal polishing slurry
by an SEM
It has been well established that handling slurry (i.e.
circulating through a distribution system) can result in
changes in the particle size distribution and agglomeration
of slurry particles [4]. The ability to measure the change
in the “working particle size distribution” is benefical to
the CMP engineer seeking tighter process control and
improved removal efficacy. Figure 6 shows the
cumulative effect of circulating a batch of slurry
containing colloidal silica particles. As the number of
turn-overs (passes through the pumping system) increased,
the concentration of small particles decreased (top graph)
and the number of large particles increased (bottom
graph). This suggests that this slurry is susceptible to
handling damage with small particle agglomerating to
form larger particles.
Number-weighted concentrations
Particle diameter (nm)
20 30 40 50 60 70 80 90 150 200 300 400100
Differentialnumberconcentration
d(#/ml)/dlog(DP
)
0
2e+10
4e+10
6e+10
8e+10
0
10
20
50
100
197
508
1013
3217
Number of passes
through the pump
Volume-weighted concentrations
Particle diameter (nm)
20 30 40 50 60 70 80 90 150 200 300 400100
Differentialvolumeconcentration
d(nm3
/ml)/dlog(DP
)
0.0
2.0e+16
4.0e+16
6.0e+16
8.0e+16
1.0e+17
1.2e+17
0
10
20
50
100
197
508
1013
3217
Number of passes
through the pump
Figure 6. Example of PSD changes during circulation
of a colloidal silica slurry.
4 MEASUREMENT OF FILTER
RETENTION BELOW 50
NANOMETERS
The removal of particles from liquids by filters used in
semiconductor processes has traditionally been performed
using optical particle counters. Improvements in these
instruments now allow for measurement of particles as
small as 40 nm. However, critical feature size for current
state-of-the-art devices are currently at 40 nm resulting in
a critical particle size of 20 nm. The LNS system has the
ability to measure filter retention efficiency well below the
critical particle size. In addition, since the sizing accuracy
of the LNS is independent of the optical properties of the
particle, multiple types of particles can be used as a filter
challenge. Historically, most retention testing has been
conducted using PSL, particles which have a high
refractive index relative to water. In addition, most optical
particle counters are calibrated using PSL. PSL is not
typically found in high purity water and chemical systems
so the ability to use more realistic and relevant particles
such as silica is a benefit.
An experiment was performed to assess the
capabililites of the LNS to measure retention of silica
Nanotech 2011: Technical Proceedings of the 2011
Nanotechnology Conference and Expo
Cin - Cout
Cin
particles by four different filters. The filters were
challenged with mono-dispersed silica particles having a
median diameter of 28 nm. Prior to the particle challenge
the filters were flushed with UPW to eliminate particle
shedding. Four challenge particle concentrations were
used ranging from 3x107
/mL to 1x109
/mL (0.7 to 23 ppb).
Particle concentrations upstream and downstream of the
filter were measured using the LNS. Filter particle
retention was measured as a function of loading (Figure 7).
Total challenge (monolayers)
0.01 0.1 1 10
Retention(%)
0
10
20
30
40
50
60
70
80
90
100
Filter E
Filter F
Filter G
Filter H
Figure 7. Retention of 28 nm silica by four filters
The vertical axis in Figure 7 is % retention defined as:
% Retention = ----------- x 100
where Cin = particle concentration pre-filter
Cout= particle concentration post-filter
The horizontal axis represents the cumulative particle
challenge plotted in monolayers. One monolayer equals
the number of particles theoretically require to cover the
entire area of the filter based on the particle’s circular
cross-section. The vertical dashed lines indicate the
change to a new challenge concentration.
While Figure 7 indicates significant differences
between the retention capabilities the four filters tested.
Filter H retention dropped quickly with loading to the
point where it was passing almost 100% of the challenge
particles near the end of the test. Filter E retained almost
100% of the challenge particles throughout the entire test.
Filter F had close to 100% retention until challenged at the
highest concentration.
SUMMARY
A liquid nanoparticle sizing (LNS) system capable of
measuring the sizes and concentrations of particles in
colloidal suspension has been developed. The method
directly measures particle concentrations and can detect
particle sizes down to 5 nm. The system allows
measurement of small differences in particle size
distributions in colloidal suspensions and measurment of
filter retention of particles as small as 10 nm.
REFERENCES
[1] Wang SC and RC Flagan, “Scanning Electrical
Mobility Spectrometer,” Division of Engineering
and Applied Science, California Institute of
Technology, Pasadena, CA 91125, pp. 138-178,
1989.
[2] Donnelly, MK and Mulholland, “Particle size
Measurement for Spheres with Diameters of 50 to
400 nm”, National Institute of Standards and
Technology, Report # NISTIR 6935, 2003.
[3] Grant, DC, “Measurement of 28 nm particle
removal from liquids by high purity filters”, North
American Membrane Society 2010 Conference,
Washington, DC, 2010.
[4] Litchy MR and DC Grant. “Effect of Pump Type
on the health of various CMP slurries”,
Semiconductor Fabtech, 33rd
edition, pp 53-59,
2007.
3E7/mL 1E8/mL 3E8/mL 1E9/mL

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A Novel Method for Measuring the Sizes and Concentrations

  • 1. Nanotech 2011: Technical Proceedings of the 2011 Nanotechnology Conference and Expo A Novel Method for Measuring the Sizes and Concentrations of 5-500 nm Particles in Colloidal Suspensions H. Gary Van Schooneveld, Mark R. Litchy and Donald C. Grant CT Associates, Inc., 7121 Shady Oak Road, Eden Prairie, MN 55344, U.S.A., gary@ctassociatesinc.com, mark@ctassociatesinc.com, don@ctassociatesinc.com ABSTRACT Measurement of the sizes and concentration of particles in colloidal suspensions has been a challenge particularly for suspensions with particles smaller than 100 nanometers. A new measurement technique has been developed that allows for measurement of particles as small as 5 nanometers in these suspensions. This new approach, uniquely combining proven techniques used for counting and sizing aerosol particle size distributions (PSDs) with nebulizer technology, has been developed to measure both particle size and number concentration in concentrated liquid suspensions. The technique has demonstrated the ability to provide unique and useful PSD data for chemical /mechanical planarization (CMP) slurries used extensively in the micro-electronics industry. In addition, the ability to measure filter retention of particles as small as 10 namometers has been demonstrated. Keywords: nebulizer, SMPS, slurry, filtration, nanoparticles 1 LIQUID NANOPARTICLE SIZING (LNS) SYSTEM DESCRIPTION The LNS (Figure 1) consists of an ultrafine nebulizer and a scanning mobility particle sizer (SMPS). A colloidal suspension is diluted on-line in ultrapure water (UPW) and injected into the nebulizer. The nebulizer generates a droplet distribution in filtered air. The resultant droplet distribution is diluted and dried with additional filtered air to form an aerosol laden with the particles originally in the colloidal suspension. The aerosol PSD is then measured using a commercially available SMPS system that is capable of measuring particles as small as 3 nm in size. A TSI Model 3936 SMPS was used to generate the data provided in this paper. The key to this measurement approach is the nebulizer. Dissolved non-volatile residue in the suspension will form particles when the droplets from the nebulizer are dried. These residue particles can interfere with the particle analysis. Figure 1. Schematic of the liquid nanoparticle sizing (LNS) system Dynamic Mobility Analyzer (DMA) Condensation Particle Counter (CPC)CDA UPW Ultrafine Nebulizer Scanning Mobility Particle Sizer (SMPS)Particle Aerosol Nanoparticle supension Pressure regulator Drain Neutralizer DMA CPC monodispersed aerosol
  • 2. Nanotech 2011: Technical Proceedings of the 2011 Nanotechnology Conference and Expo The nebulizer used in this system minimizes this effect by producing droplets that are sufficiently small and uniformly sized that particles formed from dissolved materials in the droplets are small enough as to not interfere with the particle size measurement. In addition, the particle suspension is sufficiently dilute that no more than one particle is present in each droplet. Also, measuring under different operating conditions, the instrument is capable of determining whether particles measured are from initially dissolved or particle residue. The LNS technique of measuring colloidal PSDs offers many interesting capabilities. This technique measures number concentrations, not relative particle concentrations (that is, one size relative to another) and makes no assumption regarding the shape of the PSD. The number- weighted PSD measured may easily be converted to alternative weightings such diameter (D), surface area (D2 ), or volume (D3 ) weighted distributions. Since this technique measures individual particles, it is highly sensitive to measuring rather small changes in these suspensions and is not affected by the optical properties and density of the particles. Finally, the SMPS used to size and count the particles is a well establish instrument for measuring aerosols [1] and is even used to size NIST particle standards [2]. 2 SIZING ACCURACY An example of the sizing accuracy of the LNS system is shown in Figure 2. In this evaluation, particles of three gold colloids (BBI Research, Madison, WI) were measured individually. As seen in Table 1, the sizing measurements correlate well with the manufacturer’s sizing claims. Measurements of polystyrene latex (PSL) and silica particles have also shown good agreement with manufacturer’s claims [3]. Particle diameter (nm) 5 6 7 8 9 15 20 25 30 35 4010 Relativedifferentialconcentration d(#/mL)/dlog(DP) 10 nm 20 nm 30 nm Figure 2. Measurement of BBI gold nanoparticles Mean (nm) CV (%) Mean (nm) CV (%) 10 9.3 < 15 8.4 13 20 20.3 < 8 20.8 7.4 30 30.3 < 8 30.5 7.3 Manufacturer measured size LNS measured size Nominal Size (nm) Table 1. Sizing comparison between BBI certificate of analysis and LNS measurments 3 MEASUREMENT OF POLISHING SLURRIES The PSD of a tri-modal polishing slurry measured by the LNS is presented in Figure 3. As discussed previously, the LNS directly measures the sizes and numbers of individual particles in the colloidal suspension. As such, variations in concentration of specific size particles amongst samples can readily be detected. Variations in particle concentration can effect process efficacy (e.g. effect material removal rates during polishing). In comparison, Figure 4 presents the data from a DLS instrument used to measure the the same polishing slurry. The DLS is an ensemble measurement technique that measures the properties of many particles simultaneously and then fits the data to an assumed lognormal PSD. In addition, only relative particle concentrations are provided. Scanning electron microscopy (SEM) of the slurry confirms the tri-modal PSD (Figure 5). Particle diameter (nm) 20 30 40 50 60 70 80 9010 100 Differentialvolumeconcentration d(nm3 /mL)/dlog(DP ) 0 2e+15 4e+15 6e+15 8e+15 1e+16 1e+16 1e+16 2e+16 2e+16 2e+16 Figure 3. Measurement of a tri-modal polishing slurry by the LNS system
  • 3. Nanotech 2011: Technical Proceedings of the 2011 Nanotechnology Conference and Expo Particle diameter (nm) 20 30 40 50 60 70 80 9010 100 Relativeconcentration 0.00 0.25 0.50 0.75 1.00 Figure 4. Measurement of a tri-modal polishing slurry by a DLS system Figure 5. Measurement of a tri-modal polishing slurry by an SEM It has been well established that handling slurry (i.e. circulating through a distribution system) can result in changes in the particle size distribution and agglomeration of slurry particles [4]. The ability to measure the change in the “working particle size distribution” is benefical to the CMP engineer seeking tighter process control and improved removal efficacy. Figure 6 shows the cumulative effect of circulating a batch of slurry containing colloidal silica particles. As the number of turn-overs (passes through the pumping system) increased, the concentration of small particles decreased (top graph) and the number of large particles increased (bottom graph). This suggests that this slurry is susceptible to handling damage with small particle agglomerating to form larger particles. Number-weighted concentrations Particle diameter (nm) 20 30 40 50 60 70 80 90 150 200 300 400100 Differentialnumberconcentration d(#/ml)/dlog(DP ) 0 2e+10 4e+10 6e+10 8e+10 0 10 20 50 100 197 508 1013 3217 Number of passes through the pump Volume-weighted concentrations Particle diameter (nm) 20 30 40 50 60 70 80 90 150 200 300 400100 Differentialvolumeconcentration d(nm3 /ml)/dlog(DP ) 0.0 2.0e+16 4.0e+16 6.0e+16 8.0e+16 1.0e+17 1.2e+17 0 10 20 50 100 197 508 1013 3217 Number of passes through the pump Figure 6. Example of PSD changes during circulation of a colloidal silica slurry. 4 MEASUREMENT OF FILTER RETENTION BELOW 50 NANOMETERS The removal of particles from liquids by filters used in semiconductor processes has traditionally been performed using optical particle counters. Improvements in these instruments now allow for measurement of particles as small as 40 nm. However, critical feature size for current state-of-the-art devices are currently at 40 nm resulting in a critical particle size of 20 nm. The LNS system has the ability to measure filter retention efficiency well below the critical particle size. In addition, since the sizing accuracy of the LNS is independent of the optical properties of the particle, multiple types of particles can be used as a filter challenge. Historically, most retention testing has been conducted using PSL, particles which have a high refractive index relative to water. In addition, most optical particle counters are calibrated using PSL. PSL is not typically found in high purity water and chemical systems so the ability to use more realistic and relevant particles such as silica is a benefit. An experiment was performed to assess the capabililites of the LNS to measure retention of silica
  • 4. Nanotech 2011: Technical Proceedings of the 2011 Nanotechnology Conference and Expo Cin - Cout Cin particles by four different filters. The filters were challenged with mono-dispersed silica particles having a median diameter of 28 nm. Prior to the particle challenge the filters were flushed with UPW to eliminate particle shedding. Four challenge particle concentrations were used ranging from 3x107 /mL to 1x109 /mL (0.7 to 23 ppb). Particle concentrations upstream and downstream of the filter were measured using the LNS. Filter particle retention was measured as a function of loading (Figure 7). Total challenge (monolayers) 0.01 0.1 1 10 Retention(%) 0 10 20 30 40 50 60 70 80 90 100 Filter E Filter F Filter G Filter H Figure 7. Retention of 28 nm silica by four filters The vertical axis in Figure 7 is % retention defined as: % Retention = ----------- x 100 where Cin = particle concentration pre-filter Cout= particle concentration post-filter The horizontal axis represents the cumulative particle challenge plotted in monolayers. One monolayer equals the number of particles theoretically require to cover the entire area of the filter based on the particle’s circular cross-section. The vertical dashed lines indicate the change to a new challenge concentration. While Figure 7 indicates significant differences between the retention capabilities the four filters tested. Filter H retention dropped quickly with loading to the point where it was passing almost 100% of the challenge particles near the end of the test. Filter E retained almost 100% of the challenge particles throughout the entire test. Filter F had close to 100% retention until challenged at the highest concentration. SUMMARY A liquid nanoparticle sizing (LNS) system capable of measuring the sizes and concentrations of particles in colloidal suspension has been developed. The method directly measures particle concentrations and can detect particle sizes down to 5 nm. The system allows measurement of small differences in particle size distributions in colloidal suspensions and measurment of filter retention of particles as small as 10 nm. REFERENCES [1] Wang SC and RC Flagan, “Scanning Electrical Mobility Spectrometer,” Division of Engineering and Applied Science, California Institute of Technology, Pasadena, CA 91125, pp. 138-178, 1989. [2] Donnelly, MK and Mulholland, “Particle size Measurement for Spheres with Diameters of 50 to 400 nm”, National Institute of Standards and Technology, Report # NISTIR 6935, 2003. [3] Grant, DC, “Measurement of 28 nm particle removal from liquids by high purity filters”, North American Membrane Society 2010 Conference, Washington, DC, 2010. [4] Litchy MR and DC Grant. “Effect of Pump Type on the health of various CMP slurries”, Semiconductor Fabtech, 33rd edition, pp 53-59, 2007. 3E7/mL 1E8/mL 3E8/mL 1E9/mL