nanomechanical characterization of cdse qd-polymer nanocomposites
TRANSCRIPT
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Eddie McCumiskeyMaster’s Thesis Presentation23 January 2008Virginia Commonwealth University
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1. Motivation2. Problem Statement3. Challenges4. Approach5. Experimental Details6. Results7. Conclusion8. Acknowledgements9. Questions
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Low-cost, light-weight, rollable solar cells
Low-power, high-resolution displays Flexible circuitry
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Sony’s 3-mm thick TVwww.sonystyle.com/oled
http://www.solardirect.com/pv/consumer-ready/power-film.htm#fea
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Nanostructure-polymers hybrids exhibit: Increased Efficiency Tunable Band Gap Tunable Electrical Properties
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http://www.nn-labs.com/CdSe-orderform.htm
Commercial CdSe Quantum Dots
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In order for QD-polymer hybrids to be commercially viable, their reliability
and durability must be known.
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Mechanical Characterization
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Polymer-Clay Nanocomposites invented by Toyota (1985)Greatly enhanced strength, elastic modulus
Large Interaction between NPs and filler material due to high interfacial area
CNT-polymer nanocomposites: Increased hardness, elasticmodulus
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Nanocomposite Mechanical Properties
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Theoretically, QDs should be stiffer than bulk Lattice contraction due to high surface energy
Nanoscale structures shown to impede dislocation formation
Nanoindentation of QD films reveals:* Polymeric behavior of QDs with ligands attached Granular behavior of QD films without ligands
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*D. Lee et al., Phys. Rev. Lett. 98.2 (2007)
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Large gap in research on mechanical properties of QD-polymer nanocomposite films
Challenges Mechanical characterization of thin films (<100 nm) Interference from the underlying substrate Obtaining uniform QD Dispersion
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glass substrate
Applied Load
QDs in a polymer matrix
Conceptual Design of ExperimentExample from the literature: organic solar cell made with blended CdSe nanoparticles and OC1C10-PPV*
*Figure from: B. Sun, E. Marx, and N. C. Greenham, “Photovoltaic Devices Using Blends of Branched CdSe Nanoparticles and Conjugated Polymers.” Nano Lett. 3.7 (2003), pp. 691-963.
blended nanoparticle-
polymer thin film
Nanoindenter tip
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Characterizing the Mechanical Properties of Nanocomposite Films
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I. Prepare QD-Polymer Solutions
II. Deposit Films onto Glass
III. Characterize Film Uniformity
IV. Mechanical Characterization
Nanoindentation
TEMAFM
Stirring Sonicating
Spin-coating
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CdSe QDs NN-Labs # CSE 620-100 Capped with ODA Ligand Dispersed in Toluene (5 mg/mL) Abs 620 nm; PL ~630 nm
CdSe
ODA Ligands
5.6 nm
CdSe QDs
Source: http://www.nn-labs.com/CdSe-orderform.htm
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MEH-PPV* Polymer American Dye Source # ADS200RE Abs 490 nm; PL ~585 nm
MEH-PPV Structure
Dry MEH-PPV
*poly[2-methoxy-5-2(2΄-ethylhexyloxy-phenylenevinylene)]
Source: http://www.adsdyes.com/products/pdf/homopolymers/ADS200RE_DATA.pdf
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Fabrication and Characterization
of QD-Polymer Films
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1. Dissolve MEH-PPV in TolueneA. Weigh MEH-PPVB. Add toluene (5 mg MEH-PPV / mL toluene)C. Stir ~12 hrs at 300 RPM at room temp.
2. Mix MEH-PPV & QD SolutionsA. Add equal volume of QD solution to make 50
wt% QDs in MEH-PPV
B. Stir ~12 hrs at 300 RPM at room temp.
+
MEH-PPV in toluene
QDs in toluene
MEH-PPV + QDs in toluene
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A. Ultrasonicate Combined Solutions for 30 minsB. Filter through a 1.0-µm PTFE filter (optional) C. Spin-Coat @ 1,000-2,000 RPM, 30 secondsD. Anneal on hot plate @ 120 °C, 10 mins
A. SonicateC. Deposit via Spin-
Coating
D. Anneal
Filtering
B.
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Unfiltered Filtered
Aggregation
Aggregation observed at the micrometer scale
Filtering removes manylarge aggregates
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20 μm
200 μm200 μm
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Dispersion is a common problem through the literature
Ligands may lead to aggregationLigands also unfavorable for
devices*
* N. C. Greenham, X. Peng, and A. P. Alivisatos, “Charge Transport in Conjugated-Polymer/ Semiconductor-Nanocrystal Composites Studied by Photoluminescence Quenching and Photoconductivity.” Phys Rev. B 54.24 (1996), pp. 17628-17637.
ligand
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Ligand is an insulator
Removing ligands: enhances charge
separation & transport;
quenches PL more realistic for
commercial applications
QDs w/ Ligands
QDs w/o Ligands
LIGAND
Need to remove the ligands
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QDs precipitated in pyridine 1 mL QD solution 1 mL pyridine ~10 mL hexanes
Retrieved via centrifugation 9,000+ RPM 30 mins
Change to binary solvent: 8% pyridine, 92% choloroform**** Modified method of Sun et al. ** suggested by Dr. David Goorskey
** B. Sun, E. Marx, and N. C. Greenham, “Photovoltaic Devices Using Blends of Branched CdSe Nanoparticles and Conjugated Polymers.” Nano Lett. 3.7 (2003), pp. 691-963.*** W. U. Huynh, J. J. Dittmer, W. C. Libby, G. L. Whitting, and P. Alivisatos, “Controlling the Morphology of Nanocrystal-Polymer Composites for Solar Cells.” Adv. Funct. Mater. 13.1 (2003), pp. 73-79.
2X
Centrifuge
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Lig
and
re
mo
ved
Lig
and
atta
che
d
Unfiltered Filtered
Improved dispersion after ligand-removal process Preliminary film preparation is complete All solutions & films henceforth made w/ ligand-removal procedures
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6 Films to characterize:
wt% QDs
vol% QDs*
0% 0%
50% 15.0%
75% 34.6%
90% 61.4%
95% 77.0%
100%
100%
* Vol% estimated using densities of 1 g/cm3 for MEH-PPV* (Mirzov 2004) and 5.664 g/cm3 for CdSe.** O.Mirzov et al. “Direct Exciton Quenching in Single Molecules of MEH-PPV at 77 K.” Chem. Phys. Lett. 386.4-6 (2004), pp. 286-290.*** S. Adachi, Handbook on Physical Properties of Semiconductors. Volume 3: “II-VI Compounds.” Springer-Verlag (2004).
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Tapping-mode AFM Resonant Freq ~260 kHz
Veeco Multimode AFM
LASER alignment
Piezo tubescanner
sample
10µm
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wt% QDs:
100%
0%
50%
75%
90%
95%
5 μm 5 μm
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Ra = 3.4
Ra = 20.3
Ra = 21.0
Ra = 5.7
Ra = 11.7
Ra = 2.4Ra Average Roughness (nm)
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Drop-cast dilute (1 mg/mL) solutionsonto Cu mesh, thin-carbon film TEM grids 50 wt% QDs in MEH-PPV 90 wt% QDs in MEH-PPV
Drop-cast Original QD solution as well Dry in N2 dry box ~ 24 hrs
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Jeol 2010F TEMTEM grid
Drop-casting
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QDs in toluene (as-received)
90 wt% QDs in MEH-PPV
50 wt% QDs in MEH-PPV
20 nm 20 nm 20 nm
5 nm 5 nm 5 nm
3-D Architecture
No QDs
Noise from amorphous
polymer
~5-6 nm25
QD
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MECHANICALCHARACTERIZATION
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Load
, P
Displacement, h
dPS
dh
ch
hold segment
loading segmen
tunloadin
g segmen
t
fh maxh
maxPhf hmaxhc
aspecimen
Play
h
indenter tip
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hc
cP
HA h
2r c
dPS E A h
dh
hardnessstiffness
elastic modulus (reduced)
cross-sectional area
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Isolating Film Properties
Indenter Tip Bluntness
Viscoelasticity
Surface Roughness
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For thin films, substrate properties may interfere w/ measurements
Analogous to two springs in series Minimize with shallow Indentations
(<10 % film thickness)
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*A. C. Fischer-Cripps, Nanoindentaion. Springer Mechanical Engineering Series. New York (2002).
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Time-Dependence on Deformation Leads to erroneous values of E, hc
Minimizing Creep Error: Long Hold* Rapid Unload**
Correcting throughComputation L
oad
, P
Displacement, h
“Nose”
dh
dP
ch
long hold
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*Briscoe 1998**Yang 2004
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hc
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Indenter Tip Geometry
-Images from: A. C. Fischer-Cripps, Nanoindentaion. Springer Mech. Engineering Series (2002).*Oliver, W. C. and G. M. Pharr. J. Mater. Res. 7.6 (1992), pp. 1564-1583.
θ = 65.3º2( ) 24.5c cA h h
Berkovich Indenter Tip
<Rounded tip>
Ideally:
In actuality: 2 1/ 2 1/ 4 1/8 1/160 1 2 3 4 5( ) ...c c c c c c cA h C h C h C h C h C h C h
Rounded at end
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100 Indentations on Fused Quartz: ~5-170 nm Calibrate using known values of
(Er,H) = (69.6 GPa, 9.25 GPa)
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2 1/2 1/424.5 1204.8 6858.3 7914.4c cc cA h h h h h
Overlapping Load-Displacement Curves
Determine Area Function from Measured Er’s
scattered under 20 nm
Check area function
Er = 69.72 ± 3.26 GPA
H = 8.52 ± 0.75 GPA
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Nanoindenter Setup: Hysitron Triboindenter
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Determining the Film Thickness Compare large (hundreds of nm-deep) indentations in film vs.
clean substrate
92 nm
224 nm
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Film Thicknesses
wt% QDs 0% 50% 75% 90% 95% 100%
Film Thickness (nm) 201.62 85.61 162.62 85.15 156.42 131.36
Standard Deviation (nm) 19.33 11.67 17.11 4.48 6.98 11.35
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Nanoindentation Parameters
Load-Control Test Cycle
5 indentations each at 8 maximum loads, 3 rates Load-control feedback Drift correction enabled Diamond Berkovich indenter with 50-nm tip radius
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Add film thickness, roughness
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75 wt% QDs
00.5
11.5
22.5
33.5
4
0 50 100 150Contact Depth (nm)
Hard
ness
(GPa
)
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Indentation Size Effect
0 wt% QDs
00.5
11.5
22.5
33.5
4
0 50 100 150Contact Depth (nm)
Hard
ness
(GPa
)
50 wt% QDs
00.5
11.5
22.5
33.5
4
0 50 100 150Contact Depth (nm)
Hard
ness
(GPa
)
90 wt% QDs
00.5
11.5
22.5
33.5
4
0 50 100 150Contact Depth (nm)
Har
dnes
s (G
Pa)
95 wt% QDs
00.5
11.5
22.5
33.5
4
0 50 100 150Contact Depth (nm)
Hard
ness
(GPa
)
100 wt% QDs
00.5
11.5
22.5
33.5
4
0 50 100 150
Contact Depth (nm)H
ardn
ess
(GPa
)
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Choose an appropriate range: > 10nm < ~10% thickness
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Red
uced
Mod
ulus
(G
Pa)
Contact Depth (nm)
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Modulus vs. QD Loading
Modulus increases by a factor of 3Linear when plotted vs. vol%
Red
uced
Mod
ulus
(G
Pa)
Wt% QDs in MEH-PPV Vol% QDs in MEH-PPV
4141
75 wt% QDs
00.5
11.5
22.5
33.5
4
0 50 100 150Contact Depth (nm)
Hard
ness
(GPa
)
Choose an appropriate range: > 50nm
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Hardness vs. QD Loading
Hardness increases by a factor of 6Linear when plotted vs. vol% QDs
Har
dnes
s (G
Pa)
Wt% QDs in MEH-PPV Vol% QDs in MEH-PPV
4343
Sample0 wt% QDs(pure MEH-PPV)
100 μN/s
10 μN/s
1 μN/s
1 μN/s
4444
100 µN/s
1 µN/s
Sample0 wt% QDs(pure MEH-PPV)
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Creep During the Hold Segment for Different Loading Rates0 wt% QDs
Time (s)
Cre
ep (
nm)
4646
0 wt%
50 wt%
75 wt%
95 wt%
100 wt%
90 wt%
Creep During the Hold Segment for Different QD Loading
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Incorporation of QDs: Increases elastic modulus (up to 3x) Increases hardness (up to 6x) Reduces viscoelasticity
Implications: Important for assessing the durability and
reliability of QD-polymer hybrid devices Less creep more stable structure over
time
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Special thanks to: Dr. Curtis Taylor (Committee Chair) Dr. Jim McLeskey (Committee Member) Dr. Samy El-Shall (Committee Member) Dr. N. Chandrasekhar VCU Nanomanufacturing Lab
▪ Dr. Tarek Trad, Yezuo Wang, Dongshan Yu, Jon Kodadek, Nikolai Eroshenko
IMRE Staff▪ Dr. Saravanan Shanmugavel, Shen Lu, Dr.
Dominik Janczewski, Luong Trung Dung, Kajen Rasanayagam
Dr. David Goorskey48
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Agilent PicoPlus System User’s Manual v1.2, “Aligning the Photodiode Detector.” pp. 1-18
Used with permission from http://barrett-group.mcgill.ca/yager/art.html
http://www.nanoscience.com/products/AFM_tips.html
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