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1. Length scales and low dimensionality
Nerea Zabala
Fall 2007
1
LOW DIMENSIONAL SYSTEMS AND NANOSTRUCTURES
•Contents:
• Introduction: Nanoscience and Mesoscopic Physics.
• Dimensionality definitions.
• Relevant length scales.
• Examples of low dimensional systems.
• Fabrication and exploring tools.
• New phenomena and new applications.
LOW DIMENSIONAL SYSTEMS AND NANOSTRUCTURES
1. Length scales and low dimensionality
2
• Introduction: Nanoscience and Mesoscopic Physics.
• MESO- In between an atom and bulk solids. Size below which a solid does no longer behave bulk-like.
• Mesoscopic Physics...Physics of small condensed objects (a collection of atoms)
• Often in the nanometer-size regime ! discipline of “Nanoscience”
3
• Introduction: Nanoscience and Mesoscopic Physics.
Nanoscience and Nanotechnology
Why increasing interest for the nanoscale?
1 nm = 0,000000001 m
•(Motivation in previous course : Nanoscience: a historical perspective)
4
• Introduction: Nanoscience and Mesoscopic Physics.
ADN
Diameter of human hair
Diameter of red blood cell
Visible light wavelengths
Intel’s newest transistor
Diameter of DNA, nanotubes
Bohr diameter
5
httpp://www.owlnet.rice.edu
• Dimensionality definitions
I: Bond percolation (Microscopic scheme)
(Bottom-up)
•Based on the bonding.
•Strong covalent bond within regions of structure define the dimensionality unit and weak (e.g. Van der Waals) between units to produce the 3D structure overall.
6
• Dimensionality definitions
0D: Molecular P4Se3 1D: crystalline SiSe2
2D: crystalline Ge4Se3 3D: amorphous SiO27
• Dimensionality definitions
I: Bond percolation (Microscopic scheme)
(Bottom-up)
•Start by considering electrons in single atoms and small molecules.
•Theories to treat electrons in nanostructures:Huckel theory “Tight-binding” Localized orbitals
•Chemistry.
•This point of view will be explored in the last chapter (C nanostructures) and in course
“Soft matter and nanostructured materials (polymers, gels, colloids,...)
8
• Dimensionality definitions
II: Length scales (More macroscopic scheme)
(Top-down)
•Based on size dependence of a physical property, e.g. transport (electrons and also phonons involved).
•Reduced dimension if the dimension of the sample is lower than a characteristic length (e.g. mean free path for transport, Fermi wave-length for quantization or exciton Bohr radius in semiconductors).
9
• Dimensionality definitions
0D: quantum dot
L0 = ! , characteristic length
1D: quantum wire2D: quantum well
L0 > Li, i = 1, n ! (3" n)D system
Lx, Ly, Lz < L0
Lx, Ly < L0 Lx < L0
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• Dimensionality definitions
II: Length scales (More macroscopic scheme)
(Top-down)
•Start from solid state physics.
•Physics/electrical engineering.
•Shows qualitative features. Not bad for many metals and doped semiconductors.
•Approximations to treat electrons in nanostructures:
• “Free electrons”-no external potential-
• Independent electron approximation- ignores interactions.
• Many-particle system can be modeled by starting from single particle case
• Starting point: single particle states and energies (next chapter).
11
• Relevant length scales
•A few relevant scale lengths:
12S. Datta, “Electronic transport in mesoscopic systems”,1995
proccess transistor
(Texas Instruments).
• Relevant length scales
•Some characteristic lengths:
•De Broglie wave length, Fermi wavelength:!, !F
•Mean free path:Lm
Related to kinetic energy of electrons
Initial momentum of electrons is destroyed
! =2"!p
=2"
k
Fermi gas: characteristic momentum kF ! !F =2
kF
One single filled band in 2DEG: ! =!
2"/ns , ns : sheet density
Boltzamann gas: p =!
2mkT
Length between collisions with impurities or phonons
Lm = v!t
typical
velocity
transport
relaxation time
13
• Relevant length scales
•Phase-relaxation length : L!
•Thermal dephasing length : LT
Initial phase of electrons is destroyed
•Some characteristic lengths:
14
Quantun mechanical: phase of the electron wave function
L! =!
D!!
difusion
constant
typical
time of
elastic
collisions
D = (1/d)vLm
dimensionality of
electron gas
Characteristic length of coherent propagation for two electrons
If the energy difference between two electrons is ~kT, they travel almost coherently during time !/kT
LT =!
!D/kT
•For example: Transport through a constriction, 3 different regimes:
• Relevant length scales
•Wire dimensions: W,L
•Mean free path: LmLmLm << W,L
Lm >> W,L
W < Lm < L
15
• Relevant length scales
•For example:conductance quantization in a quantum point contact
T. Heinzal, “Mesoscopic electronics in solid state nanostructures”, WileyAFM surface topography of
Ga AS microchip.
A small wire length 140nm,
width 80 nm connects
source and drain. Planar gate
30 nm below its surface.
By applying voltages to
t h e p l a n a r g a t e
electrode, the width of
the wire is tuned.
At low T conductance is
quantized in units of
2e2h.
Ballistic regime
• Relevant length scales
•For example:mesoscopic ring used to study Abraronov-Bohm effect
17
From a 38 nm film of polycrystalline
gold. Diameter 820 nm. Thickness of
wires 40 nm
S. Washburn and R. A. Webb, Adv. Phys. 35, 375 (1986).
G. Fraser, “The New Physics for the 21th century”, Y. Imry, ch. 12
L! ! 100µm
(low T)
A significant fraction of
electrons traverse the
ring phase coherently
•Summary of conditions required for a mesoscopic device
T. Heinzal, “Mesoscopic electronics in solid state nanostructures”, Wiley
• Relevant length scales
• Relevant length scales
•For example:Kondo mirage
D. Eigler et al., IBM Almaden
http://www.almaden.ibm.com/almaden/media/image_mirage.html
Unusual phenomena
due to the wave nature
of electrons and their
correlations around
impurities.
Images of elliptical arrangements of
atoms on a metallic surface, prepared
and visualized with STM microscope.
Placing a magnetic impurity at
a focal point the ellipse created a
shadow in the other focus
(“Kondo mirage”)
(This and more beatiful images)
• Examples of low dimensional systems
•Some quasi-two-dimensional systems:
G. Lehmann, P. Ziesche, “Electronic properties of metals, Esevier, 1990
E. Sheer et al., Phys. rev. Lett. 78, 3535 (1997)
• Examples of low dimensional systems
•Peroskite-like high temperature superconductors
G. Lehmann, P. Ziesche, “Electronic properties of metals, Esevier, 1990
Superconductivity related to 2D character due lo weakly connected 2D sheets of Cu and O
• Examples of low dimensional systems
•Some quasi-one-dimensional materials:
G. Lehmann, P. Ziesche, “Electronic properties of metals, Esevier, 1990
(More in lecture 4)
(More in lecture 3)
MCBJ technique to produce metallic nanowires
• Examples of low dimensional systems
• Examples of low dimensional systems
CovalentCovalent
C-C bonds withinC-C bonds within
'molecule''molecule'
Variable spVariable sp
hybridisationhybridisation
spsp22
spsp22
pure sppure sp22
pure sppure sp33
!!"" ++
--
Carbon in all dimensions
24
• Examples of low dimensional systems
•Semiconductor nanostructures starting from GaAs-AlGaAs heterostructures
•Diminishing dimensions...
•2D electron gas
25
E. Corcoran, TRENDS IN MATERIALS: DIMINISHING DIMENSIONS; November, 1990
• Examples of low dimensional systems
•Semiconductor nanostructures starting from GaAs-AlGaAs heterostrcutures
QUANTUM
WIRE
•Squeezing 2D electron gas...
26
• Examples of low dimensional systems
27
• Examples of low dimensional systems
•Also with Si (MOSFET)
Si technology
• Examples of low dimensional systems
•Why GaAs?
29
C.W.J. Beenakker, H. van Houten, "Quantum Transport in Semiconductor Nanostructures", Solid State Physics 44, 1, 1991.http://arxiv.org/abs/cond-mat/0412664
• Examples of low dimensional systems
•OD systems, quantum dots or “artificial atoms”
30
•Synthetic nanocrystals :CdS, CdSe in glassy matrix, CuCl in
NaCl crystals, Si, Ge...
•Self-assembled QD’s
•QD’s produced from heterostructures and lithographic etching. applications in nanoelectronics and optoelectronics
•Clusters of metallic atoms grown from vapour-phase condensation in
creasing size
•Fullerenes
, Size control (~1nm-> ~200nm)
• Synthetic nanoparticles interesting because of optical properties.
• Reducing the size the gap changes, Higher fusion temperatures,
estructural changes... e.g. the gap of CdSe can be tuned from red
(1.7eV) to green (2.4 eV) when the particle diameter is reduced from
200 nm to 2 nm
•Aplications: lasers, LEDS, biosensors....
• Examples of low dimensional systems
•OD systems, quantum dots or “artificial atoms”
• Fabrication and exploring tools
•Nanolithography
•Atomic force microscopy
•Scanning tunneling microscopy
•Molecular beam epitaxy and other techniques for atomic-scale layer deposition of material.
•Chemical sysntesis with different methods....
32
(Described in previous course “Nanoscience: a historical perspective” ?
Also later in :”Fundamentals of nanoscale characterization”, “Experimental techniques”)
• New phenomena and new applications
•Laboratory for quantum phenomena:•quantum coherence, quantum confinement, tunel effect, electron-electron interactions....
•When we go dowm in dimension properties are not scalable:
•new functional relations among magnitudes, oscillations of the physical magnitudes....
•quantum Hall effect, Coulomb blockade, breakdown of Ohm’s law, quantum size effects...
•New phenomena
•New operating principles and applications: one electron devices, molecular electronics, spintronics, nanophotonics. optoelectronic devices, quantum computing, bio-nano devices for aplications in biomedicine....
33
• New phenomena and new applications
•Scalability regimes:
Simulations of breaking of Na
nanowires
Eduardo Ogando, Thesis 2004
• New phenomena and new applications
•Fermi surface topology for 3D (sphere), 2D (cylinder) and 1D (planes) electron gas
•General trends or signatures of low dimensionality
Fermi surface of a
quasi-one -dimensional
electron gas.
(More details in next lecture)
Wavy planes due to
weak coupling in real
systems or
• New phenomena and new applications
•General trends or signatures of low dimensionality
•Density of states
(More details in next lecture) Eduardo Ogando, Thesis 2004
• New phenomena and new applications• New phenomena and new applications
•General trends or signatures of low dimensionality
•Response function, susceptibility
Wave vector dependent response
function for 1”, 2D, and 3D electron gas
at T=0 K
The response function of a 1D free
electron gas at various temperature (Heeger, 1979)
• New phenomena and new applications
•Response to magnetic fields (quantum Hall effect)
Shubnikov-de Haas oscillations and
the quantum Hall effect.
Measure the longitudinal (Rxx) and Hall
resistance (Rxy) of a 2D electron gas as a
function of the perpendicular magnetic
field.
T=100mK
von Klitzing et al. 1982
G. Fraser, “The New Physics for the 21th century”, Y. Imry, ch. 12
• Summary
Write it yourself and send it to me
(just to fill one slide)
39
• Take home exercises
•Bibliographic search: Peculiarities or surprises found for other low dimensional
systems. Give paper reference where it is found, describe briefly the system
(composition, size, tempertaure...) and the property studied.
•Why interest in GaAs? Compare properties of GaAs vs. Si
(Be very concise)
40
•Find examples of systems behaving as 0D