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Upplägg och planering för NanoIntro’15; Lars Samuelson ([email protected]):
Måndag 31/8: Presentationer av deltagarna8-10 Sal F Generellt om kursen/utbildningen. Exempel på “nanofenomen” runt oss
Torsdag 3/9: Viktiga grunder: energistruktur, atomer-molekyler-kristaller10-12 Sal F Metaller-halvledare-isolatorer. Bandgap hos halvledare (& isolatorer)
Måndag 7/9: Nanofysik: kvantfysik & unika fenomen på nanoskalan8-10 Sal F Partikel-våg dualitet, “konstgjorda atomer”, tunnlingsfenomen
Torsdag 10/9: Materialvetenskap/teknik – syntes på nanoskalan, funktionella material 10-12 Sal F Epitaxi, nanomaterial, sveptunnel- och atomkraftmikroskop mm mm
Måndag 28/9: Nanoelektronik och -optik, Nano-energi 8-10 Sal F Transistorer, lysdioder, solceller mm
Onsdag 2/10: Övning & Frågestund10-12 Sal H421
Micro/Nanoelectronics och technology for the fabrication of integrated circuits and advanced heterostructure devices
EpitaxyEpitaxy allows layer-by-layer deposition of mono-crystalline materials. Basis for fabrication of low-dimensional structures: quantum wells (QWs), quantum wires (QWRs)& quantum dots (QDs).Extremely good (ML) control of thicknesses
Types of epitaxy:•liquid phase epitaxy (LPE)•vapor phase epitaxy (VPE, MOVPE)•molecular beam epitaxy (MBE, also CBE)
The MOVPE, MBE and CBE methods are used widely for nanostructure/low-dimensional structure growth.
Example of MOVPE process (T≈600 °C):
TMGa + AsH3 ----> GaAs +by-productsTMIn + PH3 ----> InP +by-products
MBE: frequently used for III-V materials1- RHEED screen2-effusion oven shutters3-effusion cells for several elements4-cryo shrouds5-RHEED electron gun6-main shutter7-substrate
0
0,5
1
1,5
2
2,5
3
3,5
4
4 4,5 5 5,5 6 6,5 7Lattice parameter (Å)
GaN
SiCBP
Si
GaPAlP
GaAs
Ge
ZnSe
AlAsCdS
InP
PbS
CdSe
InAs
GaSb
ZnTe
PbSe
AlSb
SnTe
HgTeInSb
CdTe
400
500
600700
1000
2000
10000∞
IR
UV
© 1999
InN
AlN (6.2 eV)
Band gaps of different semiconductors
IVIII V
För lysdioder (LEDs) i UV - blått - grönt dominerar idag AlGaInN
B-A-B
A-B-A
A-B-A-B-A
Growingcrystalsurface
First layerof AlGaAsgrown on a substrateof GaAs
Desorption ofexcess molecules
Supplied sourceatoms/molecules
So - how do you do epitaxial growth and how do you form heterostructures?
Growingcrystalsurface
Thin layerof GaAs
First layerof AlGaAsgrown on a substrateof GaAs
Desorption ofexcess molecules
Supplied sourceatoms/molecules
So - how do you do epitaxial growth and how do you form heterostructures?
Growingcrystalsurface
First layerof AlGaAsgrown on a substrateof GaAs
Desorption ofexcess molecules
Supplied sourceatoms/molecules
So - how do you do epitaxial growth and how do you form heterostructures?
Thin layerof GaAs
Growingcrystalsurface
Thin QWof GaAs
First layerof AlGaAsgrown on a substrateof GaAs
Desorption ofexcess molecules
Supplied sourceatoms/molecules
Top layerof AlGaAs
So - how do you do epitaxial growth and how do you form heterostructures?
Growingcrystalsurface
Thin QWof GaAs
First layerof AlGaAsgrown on a substrateof GaAs
Desorption ofexcess molecules
Supplied sourceatoms/molecules
Top layerof AlGaAs
So - how do you do epitaxial growth and how do you form heterostructures?
Thin QWof GaAs
First layerof AlGaAsgrown on a substrateof GaAs
Top layerof AlGaAs
So - how do you do epitaxial growth and how do you form heterostructures?
Thin QW
of GaAsFirst layer
of AlGaAs
grown on a
substrate
of GaAs
Top layer
of AlGaAs
So - how do you do epitaxial growth and how do you form heterostructures?
Quantizedenergy levels
Growth direction
Ener
gy
Conduction band(for electrons)
Valence band(for holes)
So - how do you do epitaxial growth and how do you form heterostructures?
Quantizedenergy levels
Growth direction
Ener
gy
Conduction band(for electrons)
Valence band(for holes)
Heterostructures to confine carriers in quantum wells, wires and dots
Conduction band(for electrons)
Valence band(for holes)
Quantizedenergy levels
Growth direction
Ener
gy
Heterostructures to confine carriers in quantum wells, wires and dots
Conduction band(for electrons)
Valence band(for holes)
Quantizedenergy levels
Growth direction
Ener
gy
Growth direction
Ener
gyConduction band(for electrons)
Valence band(for holes)
IN CLASSICAL PHYSICS:The electron approaches whatacts like a barrier which stops(blocks) the transport
Heterostructures to create tunnel barriers
Growth direction
Ener
gy
IN QUANTUM PHYSICS:If the barrier is ”thin” the wave-function can appear on the other side: the electron passes throughby a quantum mechanical process, called TUNNELING
Conduction band(for electrons)
Valence band(for holes)
Heterostructures to create tunnel barriers
Kvantprick
~ 0,3 eV
Väteatom
13,6 eV elektronenstillåtnaenerginivåer ljus
ljus
protonproton
Jämförelse mellan
en ”riktig” atom och en ”artificiell” atom
What’s a Quantum Dot Like?
10nm
10nm
[110]
[110]
AFM
Contains ~10000 atoms
InP dots grown on GaInP/GaAs
K. Georgsson et al., Appl. Phys. Lett. 67, 2981 (1995).
Aerosol particles of III-V semiconductors
Formation ofultrafine group-III aerosol particles
Size selection Adding group-V precursor
Formation of III-V semiconductor
nanocrystals
K. Deppert et al., J. Aerosol Sci. 29 (1998) 737Deppert and Samuelson, Appl. Phys. Lett. 68 (1996) 1409
10 nm
InP
10 nm
GaAs
Semiconductor nanoparticles
K. Deppert et al., J. Aerosol Sci. 29 (1998) 737
A top-down approach to making one-dimensional quantumdevices. like resonant tunneling via quantum dots. Method pioneered by Randall and Reed at Texas instruments in the late 1980s. However, rather unsatisfactory device properties due to fabrication induced damage and poor lateral control.
TOP-DOWN fabrication of 1D devices
Alternative No. 2: BOTTOM-UP fabricationPlant a seed and control bottom-up growthof a perfectly functioning Bonsai tree.
Alternative No. 1: TOP-DOWN fabricationStart with a block of wood and carve a small wooden mini-tree with trunk and branches.
Comparison between top-down & bottom-up fabrication of complex structures
A forest of nanotrees with multiply seeded trunks, branches and leaves, with the entire tree being single-crys-talline and monolithic.
Each level of branches is seeded by Au aerosol nanoparticles, allowingcontrol of: – diameter – length – compositionincluding formation ofheterostructures insidebranches or at branch-leaf interfaces.
Kimberly Dick et al.
Top view
Side view
Au aerosol particlesdeposited on <111>B- oriented nanowires(low density)
Kimberly Dick et al.
AEROTAXY growth w/o substrate Would it be possible (a thought exp!)to initiate NW growth directly froma catalytic gold-particle, which wesomehow hold in a nano-tweezer?
If so, new possibilities could emerge for production of semiconductors w/o the need for expensive substrates, for areas like solar cells, LEDs, Batteries etc..
New initiative for substrate-free NW-growth
AEROTAXY: a revolutionary new way to grow NWs
TraditionalNW growth
Generally accepted notion:NWs grow guided by the substrate on top of which the NW nucleates.
The crystalline structure & orientation then governs the structure & orientation of the resulting NWs!
(111)
50nm Au seedsTg = 525°C
- The growth rate is extremely high, >1µm/s, which is up to 1000 times faster than for normal epitaxial growth!
From HRTEM+FFT we can say:- The NWs are perfect ZB, and virtually defect free- Growth direction is <111>B.
New initiative for substrate-free NW-growth
AEROTAXY: a revolutionary new way to grow NWs
Heurlin et al., “Continuous gas-phase synthesis of nanowires with tunable properties”, NATURE 492, 90, 6th Dec. 2012
Aerotaxy - Present status
1"µm" 0.5"µm"
In our presently operated Gen 3.0 we produce perfectly straight and untapered GaAs nanowires of length 2-4µm
Lund Nano Lab
Second floor
• Cleanroom class ISO 7 “class 10,000”• Semiconductor growth• Connected with Berzelius Laboratory
First floor
• Cleanroom class ISO 5 “class 100”• Semiconductor processing• 3 individual anti-vibration platforms
Lithography: from Greek “writing on stone”
Lithography: pattern transfer into recording media (resist) and its subsequent
transfer to a desired device structure (metallization, etching, ion implantation).
Different types:
1. Optical lithography: contact, proximity and projection printing
2. X-ray lithography
3. Electron beam lithography
4. Ion beam lithography
5. Imprint lithography
Lithographic techniques
EBL exposure strategy
Dedicated EBL system or modified SEM
Exposure: sequential writing, pixel-by-
pixel (exceptions: shaped beam, cell
projection lithography, SCALPEL
systems)
What is needed:
1. Source of e-beam
2. Pattern generator
3. Alignment system
Pattern transfer after lithography: lift-
e-
(a) (b) (c)
ResistSubstrate
Exposure Developed
backward leaning profile in resist (key requirement!)
evaporation of metal dissolution of resist (acetone)
metalmetal etching
contactsion impl.etc
Nanoimprint lithography (NIL)
New lithographic technique, S. Chou et al (1995)
NIL processing:
1. Deposition of a polymer onto substrate.
2. Physical contact between stamp and substrate. Application of pressure (50-80 bar) and heating above Tg of the polymer.
3. Cooling and release of stamp from the substrate.
4. Oxygen plasma ashing to remove resist residues on substrate.
CONFERENCES
+ EXPO
Site control & morphology of NW growth induced by Au patterns• Many applications require a high degree of control over site and morphology…• Site control - how ideal can we make it?• We can determine the growth site by controlling the site of the seed particle.
Metallization, 1-50 nm Au
Transferred to growth system, Au particles alloy with the substrate
Lift-off defines gold nanoparticle seeds
NW growth begins when precursors are introduced
Bare waferEBL opens up apertures in the resist
For details of EBL- and NIL-defined nanowire arrays, see for instance:T. Mårtensson et al., “Fabrication of individually seeded nanowire arrays by VLS growth”, Nanotechnology 14, 1255 (2003) T. Mårtensson et al., “Nanowire arrays defined by nanoimprint lithography”, Nano Letters 4, 699 (2004)
InP NW array grownby Thomas Mårtenssonusing MOVPE