from nano-particles to nano-polymers · gretchen a. devries alicia m. jackson a. amy yu (also at...
TRANSCRIPT
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The Supramolecular Nano‐Materials Group
From Nano-Particles to Nano-Polymers
Francesco StellacciDepartment of Materials Science
and Engineering, [email protected]
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S u N M a G
The Supramolecular NanoMaterials Group
Supramolecular Materials Science
Monolayer Protected Metal Nanoparticles
FunctionalizedCarbon Nanotubes
Nanowires
Supramolecular Lithography Supramolecular
Nano Stamping
Jackson, Myerson, Stellacci, Nat. Mat., 3, 330, 2004Akthakul, Stellacci, Mayes,. Adv. Mat., 17, 532, 2005Jackson, Silva, Hu, Stellacci, JACS., 128, 11135, 2006DeVries, Brunnbauer, Stellacci, Science 315, 358, 2007Centrone, Yu, Stellacci,Small, 3, 814, 2007
Barsotti, O’Connell, Stellacci, Langmuir, 20, 4795, 2004Barsotti, Stellacci, J. Mat. Chem., 16, 962, 2006
Halik, M. et al. Nature, 431, 963, 2004
Yu, Stellacci, Nano Letters, 5, 1061, 2005Yu, Stellacci, JACS, 127, 16774, 2005 Yu, Stellacci, J. Mat. Chem., 16, 2868, 2006
Wunsch, Stellacci, Prato, manuscript in prepLong, Wu, Wunsch, Marzari, Stellacci in prep..Liu, Yuan, Kong, Stellacci manuscript in prep.
NANO-MATERIALS
LITHOGRAPHY
20 μm
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S u N M a G
Metal Nanoparticles Synthesis
Metal Salt (AuHCl4) + HS
Reducing Agent (NaBH4)+HS
Ligand exchange reaction*
Direct mixed ligands reaction**
A. C. Templeton, M. P. Wuelfing and R. W. Murray, Accounts Chem. Res. 2000, 33, 27F. Stellacci, et al. Adv. Mat. 2002, 14, 194
HS
HS
HS
HS
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S u N M a G
Nanoparticle Absorption
12 2
1 2( 2 )m
εσε ε ε
=+ +
Mie theory describes the absorption, σ, of small metallic particles:
mεgoldε
εm is a volume-average of the dielectric constants (ε) of the ligand molecules and the solvent
4-Aminophenyldisulfide(APS)
Electron donor
4-Fluorobenzenethiol(FBT)
Electron acceptor
5,5’-Dithiobis(2-nitrobenzoic acid)(NBA)
Electron acceptor
Dimethyl (4,4’ dithiobiscinnamate)(CIN)
Electron acceptor
F
SH SH
NO2
OH
O
SH
OO
NH2
SH
Conjugated molecules:
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S u N M a G
Absorption by Functionalized Nanoparticles
• Trend in ε predicted by polarizability of molecules • Steric hindrance of NBA molecule causes porous ligand shell,
effectively lowering ε relative to expected value
By Mie theory:
CIN
FBT
APS
(NBA)
Increasing ε
522
530
510
541
0
0.05
0.1
0.15
0.2
0.25
0.3
0.35
0.4
300 400 500 600 700 800Wavelength (nm)
Abs
orpt
ion
AminophenyldisulfideFluorobenzenethiolNitrobenzoic acidCinnamate
Spectra taken in dichlorobenzene (DCB) F
SH
SH
NO2
OH
O
SH
OO
NH2
SH
Absorption spectra for fully conjugated nanoparticles
*
*
* Chromophore absorption from ligands; unrelated to plasmon resonance
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S u N M a G
Increasingly Conjugated Nanoparticles
518
518
522
522
528
0.1
0.2
0.3
0.4
0.5
0.6
250 350 450 550 650 750 850Wavelength (nm)
Abs
orpt
ion
hexanethiol1:21:12:1conjugated
Absorption spectra for increasingly conjugated FBT series nanoparticles
Nanoparticles with varying ratios of:
SH
F
SH
HT
FBT
(low ε)
and
(high ε)
Larger fractions of conjugated FBT make ligand shell more polarizable; ε demonstrates corresponding increase
Similar trends are observed in other molecule series as well
More FBTIncreasing ε
HT HT FBT FBTeff
ligands
V VV
ε εε +=
Spectra taken in dichlorobenzene (DCB)
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S u N M a G
Characterizing Metal Nanoparticles
2.7 nm
3 nm
TEM shows atoms in the core STM shows ligands in the shell
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S u N M a GS u N M a G
Diameter =7.422nmLigand length= 1.08 nm
1.9nm
Average S-S spacing <x>=0.409 nm
Octanethiol (C8) homoligand np
Average STM observed headgroup spacing <S> = 0.5
Diameter=7.418Ligand length=1.56 nmAverage STM observed headgroup spacing <S>= 0.6305
Average S-S spacing<x>=0.3646 nm
Dodecanethiol (C12) homoligand np
Based on Luedtke and Landman Faraday Discussions 2004, 125, 1-22
S = STM observed spacingx = ligand spacing at core surface (adjacent Sulfur-Sulfur distance)D = STM observed np dimater (core + ligand shell)d = diameter of np core
Sd/2
D/2
x
S/D = x/d
Assumptions:The nanoparticle can be approximated as a sphereLigand length (L) is constant around the shell i.e. (D/2) = Constant
For a fully extended ligand chain of length L, with n carbon atoms, Use L = 0.12 (n+1) nm
W. D. Luedtke and Uzi LandmanJ. Phys. Chem. B, 102 (34), 6566,, 1998
Homoligand particle’s ligand structure
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S u N M a G
Au (111)
STM Height Image of OT/MPA Mixed Monolayer on Au(111)
5 nm
Randomly distributed domains of OT form in a surrounding matrix of MPA
MPA
OT
R. Smith, S. Reed, P. Lewis, J. Monnell, R. Clegg, K. Kelly, L. Bumm, J. Huthison, P. Weiss. J. Phys. Chem. B 2001, 105, 1119-1122.
SHCOOH SH
Mixed SelfMixed Self--Assembled Assembled MonolayersMonolayers
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S u N M a G
2 nm
a b
5 nm
c
2 nm
a b
5 nm
c
SH
MPA
OT
SHCOOH
STM Images of ‘Rippled’ Nanoparticles
b
5 nm
2 nm2 nm
ab c
c d
Jackson, Myerson, Stellacci, Nat. Mat., 3, 330, 2004Jackson, Silva, Hu, Stellacci, JACS., 128, 11135, 2006
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S u N M a G
Hydrophobic/Hydrophilic Ripples
a
5 nm
a
5 nm
5 nm
2 nm2 nm
ab c
c d
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S u N M a G
STM height image of OT:MPA 2:1 gold nanoparticles on gold foil
5 nmAu foil
hemispheresImaging Speed (µm/s)
0
0.2
0.4
0.6
0.8
1
1.2
1.4
1.6
1.8
2
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 1.1 1.2
Ave
rage
Spa
cing
(nm
)
0
0.2
0.4
0.6
0.8
1
1.2
1.4
1.6
1.8
2
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 1.1 1.2
Ave
rage
Spa
cing
(nm
)
Imaging Speed (µm/s)
0
0.2
0.4
0.6
0.8
1
1.2
1.4
1.6
1.8
2
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 1.1 1.2
Ave
rage
Spa
cing
(nm
)
Imaging Speed (µm/s)
STM imaging of Nanoparticles
0
0.2
0.4
0.6
0.8
1
1.2
1.4
1.6
1.8
2
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 1.1 1.2
Ave
rage
Spa
cing
(nm
)A
vera
ge S
paci
ng (n
m)
Imaging Speed (µm/s)
OT:MPA 2:1
OT:MPA 1:1
OT:MPA 30:1
Noise
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S u N M a G
Noise and Ripples
ajs6_11_12
0.4
0.5
0.6
0.7
0.8
0.9
1
4 4.5 5 5.5 6 6.5 7 7.5 8 8.5 9 9.5 10
Diameter [nm]
Rip
ple
Spac
ing
[nm
] .007.007'.007''.005.005'.005''
0.5 1.0 1.5 2.0 2.50.0
0.2
0.4
0.6
0.8
1.0
1.2
1.4
1.6
1.8
rippl
e sp
acin
g [n
m]
speed [um/s]0.5 1.0 1.5 2.0 2.5
0.0
0.2
0.4
0.6
0.8
1.0
1.2
1.4
1.6
1.8
rippl
e sp
acin
g [n
m]
speed [um/s]0.5 1.0 1.5 2.0 2.5
0.0
0.2
0.4
0.6
0.8
1.0
1.2
1.4
1.6
1.8
nois
e sp
acin
g [n
m]
speed [um/s]
b c
5 nm5 nm1.496 μm/s 5 nm5 nm1.496 μm/s 5 nm5 nm1.841 μm/s 5 nm5 nm1.841 μm/s5 nm5 nm1.595μm/s 5 nm5 nm1.595μm/s
a005 image taken at0.57 μm/s
Shows average ripple spacing of 0.699 nm ±0.098 nm
007 image taken at0.814 μm/s
Shows average ripple spacing of 0.743 nm ±0.052 nm
Jackson, Silva, Hu, Stellacci, JACS., 128, 11135, 2006
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S u N M a G
Phase Separation on NanoparticlesPhase Separation on Nanoparticles
OT:MPA
OT:MUA
SH NH2SH NH2
Hexanethiol: p-Aminothiophenol
SH OH
O
SH
SH
Ag/-SH or /-NH2, Fe3O4 /-COOH, CaCO3/COOH
SH
OT:Mercaptohexanol
SHOH
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S u N M a G
Increasing Curvature
Flat Au (111) on Mica
OT:MPA Mixed Monolayers formed on surfaces of varying curvatures
Au on Si, with 20 nm hemispheres
Au film with Au crystals ~ 10 nm
Au film with Au crystals ~ 4 nm
10 nm 10 nm 5 nm 5 nm
Curvature EffectsCurvature Effects
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S u N M a G
The Hairy Ball Theorem and SAMs
Molecules in SAMs form a 2D crystal, that is a vectorial order.
Self-Assembled Monolayers The hairy ball theorem
The hairy ball theorem states that a vectorial order cannot propagate on a topological sphere unless the vector assumes a zero value in at least two points, called poles.
One Vector Two Vectors
*Poincarre, J. Math. Pure Appl. 1, 167, 1885; Nelson, Nano Lett., 2, 1125, 2002; DeVries, Science 315, 358, 2007; see also Zerbetto et al. Small, 2007
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S u N M a G
• Molecules in SAMs form a specific angle with the surface normal in order to maximize van derWaals interactions.
• One can define a vector (from the attachment point to the projection of the molecular head group) to describe the molecular position.
What is the VectorialOrder in SAMs?
What is a topological sphere?
Thermodynamic interpretation
dodecane solution
W. D. Luedtke and Uzi Landman J. Phys. Chem. B, 102 (34), 6566,, 1998
solution
HS
HS HS
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S u N M a G
Chemistry of chain formation
SH
OH
OSH
OH
O
SHHOOC
1. Pole functionalization with 11-Mercaptoundecanoic acid (MUA)
Short reaction times allow functionalization only at the polar singularities
2. Two-phase reaction: interface-controlled stoichiometry
NH2
NH2
1,6-Diaminohexanein water phase
Nanoparticles in toluene phase
“Nano-nylon”
Amide bonds
Precipitation at the toluene-water interface indicates the formation of insoluble material
Initial
PrecipitateFinal
SH SH
DeVries, Stellacci, Science 315, 358, 2007
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S u N M a G
Nano-Nylon Two-Phase TEM images
100 nm
Nanoparticles
Chains
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S u N M a G
Inter-Particle Distance
NH
O
NH
O
SHSH 5 5
NH
OO
O NH
O
SHSH 595
DAH theoretical length = 3.6 nm
EGDA theoretical length = 9.6 nm
Potential EGDA linker conformation
Measured interparticle
distance
Potential linker position
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S u N M a G
Chains of Big Particles
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S u N M a G
AcknowledgementsGraduate StudentsRobert J. Barsotti, Jr. (now at
Arkema. Senior Scientist)Gretchen A. DeVriesAlicia M. JacksonA. Amy Yu (also at MGH, post doc)Tan Mau WuBenjamin WunschOsman Bakr (Harvard)Suelin ChenJeffrey KunaSarah ThevenetOzge AkbulutJin Young KimHyewon KimJin-Mi Jung (KAIST)Ramona DallaPiccola (Trento)
Post-DocsMarkus Brunnbauer (now at
Infineon, Senior Scientist)Xiaogang “Bruno” Liu (now at NUS,
Assistant Professor)Brenda LongOktay UzunYing YuAndrea CentroneAyush VermaKazuya NakataCedric DuboisGeorg Heimel
NSF: NER DMI-0303821NIRT DMR-0086944NIRT SCP-0304019CAREER
NIH TPEN ProgramHewlett PackardDeshpande Center ACS-PRFReed Foundation at MIT CMSE-MRSEC DMR 02-13282Int. Copper AssociationMARCO3M Non Tenured Faculty Award3M Innovation AwardDuPont Young Professor AwardPackard Foundation AwardMineral Technologies
CollaboratorsDavid Nelson, HarvardLucia Pasquato, TriesteRalph Weissleder, Harvard, MGHMolly Stevens, Imperial C., UKHenry I. Smith, MITEnzo diFrabrizio, Catanzaro, ItalyAnthony Guiseppe-Elie, C. VirginiaMaurizio Prato, TriesteMarcus Halik, Erlangen U., GermanyAnne Mayes, MITSharon Glotzer, U. MichJoerg Lahan, U. Mich.Nicola Marzari, MITDarrell Irvine, MITKrystyn Van Vliet, MITRobert Cohen, MIT
UndergraduatesJacob M. Myerson ( now at MIT)Brian Netlner ( now at MIT)Angela TongNishi N. Rochelle (LSU, now at Purdue)Kathy Li (now at UT Austin)Peter Stone (now at Berkeley)Allon Houchbaum (now at Berkeley)Samantha Bennett (now at Cambridge UK)Tom Schilling (will join Berkeley)Paulo Silva (will join Northwestern)