nanoparticles and qunatum dots via solution based...
TRANSCRIPT
Nanoparticles and qunatum dots
via
solution based chemistry
Helmer Fjellvåg and Anja Olafsen Sjåstad
Lectures at CUTN spring 2016
Nanostructures
Nanostructure:
Structures so small that chemical and physical properties become
observably different from the “normal” properties of the material.
The dimension at which this transformation become apparent depends
on the phenomena investigated.
Normally in the rage of 1 - 100 nm
Finite size effect: electronic bands are gradiually converted to molecular
orbitals – electrons as ‘particle-in-box’
Surface and interface effects: relative fraction of atoms located on the
surface/interface are significant – affects
reactivity
(1 nm = 109 m)
Size alter electronic structure
Linear combination of n atomic orbitals (AO) to form n molecular orbitals (MO)
n energy bands are formed
LUMO
CdSe quantum dots
Semiconductors as NP
Size decides - let us look into CdSe
Radiated with light
Fluorescence:
Short wavelength (blue) – small particles
Long wavelength (red) – bigger particles
Quantum dots – bandgap increasing with
decrease in particle size
5
The energy gap between the valence band and the conduction band
(corresponding to the HOMO-LUMO gap in molecular compounds) widens as
the particle size decreases. The corresponding absorption band is blue-shifted
and becomes sharper. The size distribution must be very narrow in order to obtain
good optical properties.
The optical properties may also be influenced by
interaction with e.g. solvent molecules or ligands,
which may perturb the energy levels of the surface
atoms.
Semiconductor nanoparticles in a transparent
matrix exhibits photoluminescence and third order
non-linear optical behavior (refractive index
depends in the intensity of the incident light.
Size decides – CdS (text book)
Size decides - Appliction Quantum dots
Gold
Lycurgus cup, 4. century a.c.
Size matters for metallic particles
Why does the gold look red or blue?
Colour of Au NPs are conferred by the interaction of light
with electrons on the gold nanoparticle surface.
Electrons mean free path is 5-60 nm. When particle enter this size range, electrons are
scattered at the inner surface (Mie scattering) giving rise to surface plasmons.
At a specific wavelength (frequency) of light, collective oscillation of electrons on the
gold nanoparticle surface cause a phenomenon called surface plasmon resonance
resulting in strong absorption and scattering. Frequency is related to gold nanoparticle
size, shape, surface and agglomeration state.
9
Smaller particles;
the absorption is blue shifted,
i.e. towards higher energy.
Why does the gold look red or blue or…?
Why does the gold look reddish – brown to orange?
Quantum size effect corresonding to those we have in quantum dots
10
SIMIT: Size-induced metal-insulator transition, SIMIT effect
Transition from metallic to non-metallic behavior below a few nanometers.
The energy bands gradually change toward molecular orbitals. Bulk metals follow
Ohms law (collective movement). The corresponding NPs are insulators.
In nanosized (metal) particles the
electrostatic contribution must be included
(describing the energy associated with
adding or removing an electron), Eel =
e2/2C,
C is the effective capacitance.
Add or remove single electron into
nanoparticle = single electron transfer, SET
(Possible application: Quantum computers)
Size matters for metallic particles – SIMIT effect
11
Melting point: When the mean thermal displacement (d) of the atoms becomes
larger than some fraction of the interatomic distance, the material melts.
Surface atoms have lower coordination and a higher displacement compared to bulk.
When the surface/volume ratio increases, the mean d increase, i.e. the melting point
decreases. This is more pronounced for metals. (Why?)
The melting point is only constant as long as surface effect can be neglected!
Size decides – melting point
12
Ferromagnetic materials (Fe, Co, Ni, Gd, CrO2…) spin alignment below TC,
Magnetic domains are present, separated by Block walls.
When the size of the magnetic particle is in the same range as the domain size,
only one domain is present in one particle.
Critical sizes: Fe: 14 nm, Co: 70 nm, Ni: 15 nm; Fe3O4: 128 nm.
Size decides – cooperative magnetism
13
Size decides – cooperative magnetism
-60000 -40000 -20000 0 20000 40000 60000
-0.010
-0.005
0.000
0.005
0.010 Cat-A
M (
em
u)
H (Oe)
Ms
-2000 -1000 0 1000 2000
-1.0
-0.5
0.0
0.5
1.0 Cat-A
Cat-B
M/M
s
H(Oe)
Ferromagnetic
Size – surface – crystallographic planes
Can act as a catalyst and transform carbon monoxide (CO) to carbon dioxide (CO2),
catalyst used in the removal of odours and toxins or to clean automotive exhaust gases.
Size of gold particles is more than 10 nm.
The particles are almost spherical and the perimeter attached
to the support (active sites) is short. Inactive as a catalyst
Size of gold particles is less than 5 nm.
The particles are almost hemispherical and the perimeter
attached to the support (active sites) is long. Active as a
catalyst
Size of gold particles is less than 2 nm (no. of atoms < 300).
Catalytic activity is abruptly changed by the number of atoms
and steric structure of particles.
Catalytic selectivity is abruptly changed by the
crystallographic form of supports.
Gold catalysts
Silver catalysts
The shape of a catalyst may be as important as its size.
Shape Morphology
Size control Chemical composition
• Average composition
• “Phase” segregation
• Compositional gradients
(core shell vs. solid solution)
• Contaminations
Atomic arrangement
18
How to perform the synthesis?
Main ingrediensens: Metal precursor(s) – surfactant(s) – solvent
Hot injection – case studies Co NPs and CdSe NPs
Microwave assisted synthesis
Reversed micelles
Hot injection for burst nucleation
Case studies – Co NPs and CdSe NPs
19
Extra papers related to this topic:
- Zacharaki et al. 2016 (Co NPs)
- Murray et al. 1993 (CdSe NPs)
A nanoparticle of 5 nm core diameter with different hydrophobic ligand molecules.
Left to right: trioctylphosphine oxide (TOPO), triphenylphosphine (TPP), dodecanethiol
(DDT), tetraoctylammonium bromide (TOAB) and oleic acid (OA).
Some selected surfactants for NPs
R. A. Sperling, W. J. Parak (2010)
DOI: 10.1098/rsta.2009.0273
Burst nucleation via hot injection – case study Co NPs - I
Solvent : 1,2 dichlorobenzene
C6H4Cl2
Tb = 180.5 °C
Cobalt source: Dicobalt octacarbonyl
Co2(CO)8
Tdecomp: 52 oC
Burst nucleation refers to the formation of a large number of nuclei in a short
period of time, followed by growth without additional nucleation (La Mer theory).
Surfactant: Oleic acid (OA)
CH3(CH2)7CH=CH(CH2)7COOH
Tb = 360 oC
Reflux
Burst nucleation via hot injection Case study – Co NPs –II
Sun et al. 2012
Co2(CO)8 2Co(solv) + 8CO(g)
Burst nucleation via hot injection – case study – Co NPs –III; LaMer theory
How can we trig – alter supersaturation?
- Solubility increases normally with temperature – higher injection temperature smaller
supersaturation (and larger particles)
- Solubility may decrease with increasing temperature (retrograde solubility) – higher
injection tempertaure larger supersaturation (and smaller particles)
Characterization – stable suspensions and particles
2. Suspension stability (DLS)
- Hydrodynamic diameter 13 – 25 nm
- Polydispersivity index (PDI) 0.06 0.02
- Suspensions stable for more than 1 month
1. Yield synthesis (after 4 washing cycles): 75 %
3. Phase purity and atomic arrangement
- -Co (not fcc or hcp)
- Phase pure – occasionally some CoO
- Crystallite size
4. Particle size and morphology
- TEM
- SEM in STEM mode
12 16 20 24 28 32
Inte
nsity (
a.u
.)
2(o)
a = 6.0984 0.0004 Å
( = 0.50557 Å)
Co particle size control
1) Injection time
2) Reaction time
3) Injection temperature
4) [𝐶𝑜]
[𝑆𝑢𝑟𝑓𝑎𝑐𝑡𝑎𝑛𝑡]
5) Reactant concentrations
Co2(CO)8
Dichlorobenzene (DCB)
Oleic Acid (OA)
Co particle size control; Temperature
Variable temperature and constant [𝐶𝑜]
[𝑆𝑢𝑟𝑓𝑎𝑐𝑡𝑎𝑛𝑡] = 12.9
Particle size (nm)
168 oC 179 oC
174 oC 164 oC
Particle size (nm)
Co particle size control; Temperature
162 164 166 168 170 172 174 176 178 1800
2
4
6
8
10
12
Present study (TEM) (Ratio = 12.9; Reaction time = 30 min)
Iablokov et al. 2012 (TEM) (Ratio = 6.5; Reaction time = 20 min)
Avera
ge p
art
icle
siz
e (
nm
)
Injection temperature (oC)
Co particle size control
1) Injection time
2) Reaction time
3) Injection temperature
4) [𝐶𝑜]
[𝑆𝑢𝑟𝑓𝑎𝑐𝑡𝑎𝑛𝑡]
5) Reactant concentrations
Co2(CO)8
Dichlorobenzene (DCB)
Oleic Acid (OA)
Co particle size control; Variable [𝑪𝒐]
[𝑺𝒖𝒓𝒇𝒂𝒄𝒕𝒂𝒏𝒕]
0 2 4 6 8 10 12 14 16 18 200
2
4
6
8
10
12 Present study (XRD) (T = 168
oC); Reaction time = 30 min)
Ma et al. 2004 (TEM) (T = 190 oC; Reaction time = 10 min)
Avera
ge s
ize (
nm
)
[Co]/[OA]
Co particle size control
1) Injection time
2) Reaction time
3) Injection temperature
4) [𝐶𝑜]
[𝑆𝑢𝑟𝑓𝑎𝑐𝑡𝑎𝑛𝑡]
5) Reactant concentrations
Co2(CO)8
Dichlorobenzene (DCB)
Oleic Acid (OA)
31
Synthesis of CdSe nanoparticles – hot injection
•Se dissolved in TOP (Se2-)
•Cold solution is injected into
hot CdMe2 in TOPO (300ºC)
•Temperature drops to approx.
170ºC
•Increase of temperature to
higher temperature (below
300ºC) for a specified time
Kinetically controlled synthesis
•Nucleation
•Growth
•Shape
•Composition
TOPO: Tri-n-octylphosphine oxide
TOP: Tri-n-octylphosphine
32
Synthesis of CdSe nanoparticles – hot injection
Se2-
Cd2+
Ksp =[Se2-][Cd2+]
33
Synthesis of CdSe nanoparticles – hot injection
34
Particle growth mechanisms
Coalescence
Oswald Ripening
Side-note: Earthworms goes to work…….
CdSe quantum dots
Element distribution in bi-metallic NPs
36
Bi-metallic NPs – element distribution
Is alloying in form of a solid solution favoured by decreasing the particle size?
Yes, it can be shown from thermodynamic considerations and molecular dynamic
simulations that solid solutions are favored when particle size goes down
(see p. 2894 in You et al. 2013)
Note – kinetics may play a role and alter what thermodynamic calculations are
predicting (Pt-Rh Example, next slides)
Bi-metallic NPs – element distribution
When can you expect to form a solid solution between to elements A and B in
bulk metallic materials?
Hume-Rothery substitutional solubility rules
1. Crystal structure of each element of the pair is the same
2. Atomic sizes of the atoms do not differ more than 15%
3. The elements do not differ greatly in electronegativity
4. Elements should have same valence
Metals – overview structures (Extra slide)
ccp
A1
bcc
A2
hcp
A3
40
Solid solution – Rh100xPtx - bulk
Immiscibility dome
Solid solution – Rh100xPtx NPs
0 20 40 60 80 100
3.80
3.85
3.90
230oC
Nanoparticles - reaction temperature 220 oC
Linear fit - bulk
a-a
xis
(Å
)
x in Rh100-x
Ptx
190oC
Metallic radii: rPt
> rRh
Observe that a-axis become longer
when:
- Increasing reaction temperature
- Increasing reaction time
Pt Rh
Rh rich core
with a Pt rich shell
5 10 15 20 25 30
a = 6.2286 0.0004 Å
( = 0.31010 Å)
Inte
nsity (
a.u
.)
2(o)
Co-Re nanoparticles taking the -Mn type structure
12 16 20 24 28 32
Inte
nsity (
a.u
.)
2(o)
a = 6.0984 0.0004 Å
( = 0.50557 Å)
1 0 0 n m1 0 0 n m
EDS: 10.5 2.4 at. % Re
ICP-AES:
13.9 at. % Re
Co Co85Re15
0 20 40 60 80 100
6.00
6.25
6.50
6.75
7.00 Dinega et al., 1999
Vavilova et al. 1991
This study
a-a
xis
(Å
)
x in Co100-xRex
43
Particle morphology – faceting – I
For pristine single crystals and nanoparticles surface energy plays the most important
role on the growth of the crystals.
Thermodynamics surface energies come into play
Often low-index facets {111}, {110}, {100} lowest surface energy
Construct/predict shape of NPs with basis in knowlegde on the low index factes
surface energy and Wulff-constructions (ref. Barmparis et al., 2015)
Wulff construction for Au NPs
in vacuum and 28 nm (left);
in CO(g) and 27 nm (right)
44
Particle morphology – faceting – II
Synthesis conditions affects morphology – relative rearrangment of most stable facets
and possible kinetic effects.
- Ratio between metal salt and capping agent
- Nature of solvent and surfactant/capping agent (and possible other addidatives)
octopod-cube cube truncated-cube spherical
PVP/PtCl42 = 0.007 PVP/PtCl4
2 = 0.07 PVP/PtCl42 = 0.14 PVP/PtCl4
2 = 0.28
Kalyva et al.; Submitted April 2016
45
Particle morphology – faceting – III
You et al. 2013; (See also Tables 1 and 2 same ref)
Silver catalysts
The shape of a catalyst may be as important as its size.
0 2 4 6 8 10 12 140
10
20
306.7 ± 1.0 nm
Part
icle
Popula
tion
dtotal
(nm)
Ni /Al2O3 catalysts for methanation
Pt at.60% Rh at.40%
Pt at.70% Rh at.30%
13 nm
0 2 4 6 8 10 12 140
20
40
5.5 ± 1.0 nmRSD: 18 %
Part
icle
Popula
tion
Particle Size (nm)
NiO deposited on Al2O3 NiO/Al2O3 300 oC 1% O2
0 2 4 6 8 10 12 140
10
20
30
40
50 5.1 ± 1.0 nmRSD: 20 %
Part
icle
Popula
tion
Particle Size (nm)
Ni/Al2O3 400 oC 4% H2
Microwave assisted synthesis
48
Microwave Irradiation Synthesis of NPs
Several attributes of microwave heating contribute to greener
nanosynthesis, including shorter reaction times, reduced energy
consumption, and better product yields.
dipolar polarization
ionic conduction
The heating mechanism Involves two main processes:
The dielectric
properties
of the solvents are
critical parameters for
the MWI synthesis.
Synthesis by microwave dielectric heating, is based, on the ability of a specific
material (e.g. solvent and/or reagents) to absorb microwave energy and to convert it
into heat.
Rh(acac)3, PtCl4 @100 ⁰ C
Mixture of Rh(acac)3, PtCl4 @100 ⁰ C
After MIW @ 900 W for 10 min
Pt-Rh NPs - Color of the starting materials at 100 ⁰ C
Metallic precurcors: Rh(acac)3 (97%, rhodium(III) acetylacetonate), PtCl4 (99.9+%, platinum(IV) chloride)
Liganding solvents:
OAm (tech. 70%, oleylamine) & PVP10
Polyvinylpyrrolidone average mol wt 10,000 and
(DMF, (99.8%, N,N-dimethylformamide) Dielectric constant: 36.71
51
52
Particle morphology – faceting – II
Synthesis conditions affects morphology – relative rearrangment of most stable facets
and possible kinetic effects.
- Ratio between metal salt and capping agent
- Nature of solvent and surfactant/capping agent (and possible other addidatives)
octopod-cube cube truncated-cube spherical
PVP/PtCl42 = 0.007 PVP/PtCl4
2 = 0.07 PVP/PtCl42 = 0.14 PVP/PtCl4
2 = 0.28
Kalyva et al.; Submitted April 2016
Reversed micelles
53
Nanoparticles using microemulsions as confined
reaction media - principles
Nanoreactor range 2-50 nm
Oil in Water
Water in Oil
Lecture notes KJM-5500 spring 2012, F. K. Hansen, UiO.
M. Sanchez-Dominguez et al., “New Trends on the Synthesis of Inorganic Nanoparticles Using Microemulsions as Confined Reaction Media”, 2010.
CTAB
PtRh nanoparticles in W/O microemulsions-II
Nanoreactor range 2-50 nm
M. Sanchez-Dominguez et al., “New Trends on the Synthesis of Inorganic Nanoparticles Using Microemulsions as Confined Reaction Media”, 2010.
PtRh nanoparticles in W/O microemulsions-I
Water phase: Rh(NO3)3 + H2PtCl6
Oil: n-heptane
Surfactant: polyethyleneglycol-dodecylether
F.J. Vidal-Iglesias et al. ; Journal of Power Sources 171 (2007) 448–456.
Water phase: NaBH4 or N2H4 (reducing agent)
Oil: n-heptane
Surfactant: polyethyleneglycol-dodecylether
M. Sanchez-Dominguez et al., “New Trends on the Synthesis of Inorganic Nanoparticles Using Microemulsions as Confined Reaction Media”, 2010.
Pt25Rh75
Size (TEM): D = 3.8 ± 0.9 nm
XPS: 19.9/80.1 (PtRh)
EDX: 25/75 (PtRh)
PtRh nanoparticles – how to break the microemulsion?
Pt25Rh75
58
May be produced by precipitation or by reaction in confined space.
Synthesis in confined spaces. Nanosized reactors, “Ship-in-a-bottle”. May be
pores or channels in solids or liquid droplets.
Reversed micelle (water in oil microemulsions).
Formed by adding a small amounts
of water to a surfactant in a
hydrocarbon solvent.
E.g. precipitation of CdS by adding
sulfide to a solution of a cadmium
salt.
The size is determined by the size
of the droplet (controlled by the
water/surfactant ratio).
Reversed Micelles – text book
Extra – from text book
59
60
Formation of nanoparticles from vapor.
Aerosol route – advantage: Particle size may be
controlled by droplet size, concentration etc.
Gas condensation method:
Ultra high vacuum (filled with ca. 100
Pa He).
Liquid nitrogen cold finger, a scraper,
and in-situ compactor.
Evaporation of a solid (mostly
metals) by heating.
Clusters are formed, which grow by
cluster-cluster condensation.
Convective transport towards cold
finger.
Gram quantities may be produced.
Synthesis of nanoparticles: Condensation from gas phase
61
Mechanical attrition. (abrasion, grinding)
High energy ball milling may reduce particle size to 2-20 nm. (may also
be used for synthesis or alloying)
Top – bottom synthesis
62
Thermolysis of e.g. transition metal carbonyls under an inert atmosphere may
produce metal colloids.
e.g. thermolysis of Fe(CO)5 Fe + 5CO in an organic surfactant produces
“ferrofluids” of metallic iron nanoparticles (8.5 nm).
Ni, Co, Fe and Cu nanoparticles have been prepared from the formiates:
M(OOCH)x M + xCO2 + x/2 H2 (or M + x/2 CO + x/2 CO2 + x/2 H2O)
Or from the oxalates
Photolysis, e.g. photochemical decomposition of silver halide nanocrystals.
Synthesis of nanoparticles: Thermolysis
Variant of Co NPs as discussed earlier.
Delamination Layered structures may be used to
construct new nanomaterials by
restructuring them. Typical starting
material may be layered silicates
such as clay. However, many
transition metals also form layered
structures.
These may also be curled to form
nanoscrolls.
Synthesis of nanoparticles: Delamination
Ceria/zirconia nanoparticles with
excellent thermal stability. Such
materials are used in automotive exhaust
gas treatment.
Two-nozzle flame synthesis of
Pt/Ba/Al2O3 catalysts
Flame made Pt/TiO2. Pt
particles d<3nm are indicated
by arrows.
Nanocatalyst materials can be made by spray pyrolysis. By crossing two such sprays, it
is possible to produce nanoparticles of one material on another material.
Synthesis of nanoparticles: Spray pyrolysis
Nanoparticles can be made by laser ablation of a material. They are typically collected
on a cooled substrate and most often form films. But the particles may also be used as
is in the gas phase.
Synthesis of nanoparticles: Laser ablation