lecture 6: individual nanoparticles, nanocrystals and ...€¦ · nanoscience ii spring 2009 3...
TRANSCRIPT
Nanoscience II spring 20091
Lecture 6: Individual nanoparticles, nanocrystals and quantum dots
Definition of nanoparticle:
Size definition arbitrary
More interesting: definition based on changein physical properties.
Size smaller than some critical length thatcharacterize physical phenomena
Examples: Electron mean free path, thermaldiffusion length
Nanoscience II spring 20092
Metal nanoparticles
Structure:
Common metals have close-packed crystal structure: fcc or hcp (somebcc)
Smallest fcc ”crystal”: one unit cell, 13 atoms
Nanoscience II spring 20093
Another atom layer outside: 13 + 42 = 55 atoms
More layers: 13, 55, 147, 309, 561 atoms
Structural magic numbers
N =1310n3 15n2 +11n 3( )
n = number of layers
Surface atoms:
Nsurf =10n2 20n+12
Nanoscience II spring 20094
Geometric structure, general comments:
Nanoparticle structure generally similar to bulk
Small particles (< 5 nm) may have different structures
Example Al13: theory predicts icosahedral structure
Also size-dependent deviations from the ideal structure
Indium nanoparticles, tetragonal c/aratio
TheoreticalAl13 clusters
Nanoscience II spring 20095
Electronic magic numbers
Simple model: Clusters as”superatoms”, with electronicshell structure
Jellium model: ”free” valenceelectrons in a homogeneouspositive background
Potential:
U r( ) =U0
exp r r0( ) +1[ ]
r0 : cluster effective radiusU0 : potential constant : steepness parameter
Electronic magic numbers: 2, 18, 20, 40 …. corresponding to filled shells
Compare to single atoms: 2, 10, 18, 36 (He, Ne, Ar, Kr)
Nanoscience II spring 20096
Electronic structure, general
• Solve the Schrödinger equation for an exact atomicmodel, using realistic potentials
• Density-functional theory and molecular dynamicsmost commonly used
• Find minimum-energy structure (depends onelectronic energy levels)
• Typical solution has discrete energy levels,depending on cluster size (compare ”particle in a box”)- big difference to bulk metal.
• Quantum size effects when cluster size is comparableto Fermi level wavelength. Much larger size forsemiconductors (μm compared to nm)
Nanoscience II spring 20097
Experimental studies of nanoparticle energy levels
• Optical spectroscopy (absorption, fluorescence)
• UV photoemission
• STM/STS
Example: combined STM/STS and photoemission studyof gold clusters
Nanoscience II spring 20098
Photoemission:
Gold nanoparticles gold surface
Gold nanoparticles on HOPG
STMSTS, current images
Nanoscience II spring 20099
Reactivity - catalysis
Depends on size and structure
• most (all) atoms on the surface
• closed shell most stable (compare noble gasatoms)
• strong variations with size
Production of nanoparticles - largecommercial activities
Example: Nanostellar Inc., a Silicon Valleystartup company(www.nanostellar.com)
Nanoscience II spring 200910
Fluctuations
Small nanoparticles, many surface atoms with lessmovement restrictions structure changes (fluctuations)
Nanoscience II spring 200911
Semiconducting nanoparticles
Strong variation in optical properties compared to bulk - blue shift
Nanoparticles:
• weak confinement: particle radius larger thanexciton radius blue shift
• strong confinement: particle radius smaller thanexciton radius no exciton, electron and holeindependent. blue shift + new set of energylevels
En = 13.6m* m0
r( )2n2
eV
Bulk: excitons are important for the opticalproperties
4.19 Optical absorption in Cu2O
Nanoscience II spring 200912
Light absorption in colloidal solution
Figure 7.2. Solutions of quantum dots of varying
size. Note the variation in color of each solution
illustrating the particle size dependence of the
optical absorption for each sample. Note that the
smaller particles are in the red solution (absorbs
blue), and that the larger ones are in the blue
(absorbs red).
Nanoscience II spring 200913
4.20 Optical absorption spectrum of CdSe nanoparticles withsizes 20 and 40 Å
Nanoscience II spring 200914
Karlstad: ZnO nanocrystals on surfaces
SEM images: STM images:
a) 250 x 250 nmb) 50 x 50 nmc) 28 x 28 nm
Nanoscience II spring 200915
Other nanoparticles
• Inert-gas clusters - weak van der Waals forces
• Magnetic nanoparticles… very hot research area (chapter 7)
• Superfluid clusters - Bose-Einstein condensates
• Molecular clusters - example: water, hydrogen-bondedclusters
Nanoscience II spring 200916
Synthesis of nanoparticles
Laser evaporation methods:
Nanoscience II spring 200917
Aerosol techniques, Lund Univ.Metal nanoparticles
Semiconductor nanoparticles
Nanoscience II spring 200918
Differential mobility analyzer - analysis and size selection
Nanoscience II spring 200919
Chemical methods - colloidal growth- nanoparticles grown in solution with surfactant layer
- most promising for volume production, good scalability (ExampleNanostellar)
- monodispersive growth possible (similar size of particles)
- control over composition, size, shape, structure, surface properties
Figure 7.3. La Mer model for the growth
stages of nanocrystals.
Kinetic size control
Nanoscience II spring 200920
Colloidal growth
Kinetic size control:
Monodisperse colloidalnanocrystals synthesized underkinetic size control. a,Transmission electron microscopy(TEM) image of CdSenanocrystals. b, TEM image ofcobalt nanocrystals. c, TEMmicrograph of an AB13superlattice of _-Fe2O3 and PbSenanocrystals. The precise controlon the size distributions of bothnanocrystals allows theirselfassembly into ordered three-dimensional superlattices. Scalebars, 50 nm.
Nanoscience II spring 200921
Colloidal growth - shape control
Shape control of colloidal nanocrystals. a, Kinetic shape control at high growth rate. The high-energy facets grow morequickly than low energy facets in a kinetic regime. b, Kinetic shape control through selective adhesion. The introduction ofan organic molecule that selectively adheres to a particular crystal facet can be used to slow the growth of that side relativeto others, leading to the formation of rod- or disk-shaped nanocrystals. c, More intricate shapes result from sequentialelimination of a high-energy facet. The persistent growth of an intermediate-energy facet eventually eliminates the initialhigh-energy facet, forming complex structures such as an arrow- or zigzag-shaped nanocrystals. d, Controlled branchingof nanocrystals. The existence of two or more crystal structures in different domains of the same crystal, coupled with themanipulation of surface energy at the nanoscale, can be exploited to produce branched inorganic nanostructures such astetrapods. Inorganic dendrimers can be further prepared by creating subsequent branch points at the defined locations onthe existing nanostructures. The red and green dots in a and b represent metal coordinating groups with different affinitiesto nanocrystal facets.
Nanoscience II spring 200922
Other synthesis techniques
• Radiofrequency plasma methods
• Epitaxial growth - self-assembled quantum dots (lecture 3)
• Ion implantation
• Thermolysis - high-temperature decomposition
• Mechanical milling
• Cavitation, sonochemistry, detonation
After treatments
• Passivation of cluster surfaces
• Powder consolidation
• Nanoparticle coatings