nanoelectronic transport basicsnanotr16/notes/bmuralidharan-intro.pdf · 2016-02-23 ·...
TRANSCRIPT
Nanoelectronic Transport Basics
Bhaskaran Muralidharan Department of EE, IITB
22/02/2016
School on electronic transport and magnetism
HRI Allahabad
The Building block of digital age
S D
Nanoelectronics
How far can we scale transistors?
New physics emerges at these lengthscales
CHARGE Spin
Energy
Emerging Electronics Landscape
Charge is only the beginning!
Outline of this workshopPart I: Nanoscale charge transport and low dimensional systems Theory: B. Muralidharan - basics A Ghosh -basics S Datta- overview of lessons on nanoelectronics !Modeling and simulation: A Ghosh – predictive modeling S Mahapatra – predictive modeling A Sengupta – predictive modeling + demo !Experiments: T. Kalarikkad – low dimensional conductance K Dasgupta – 2 D systems and quantum Hall effect S Lodha – 2 D Systems K Majumdar – 2 D systems !Part II: Nanomagnetism and Spintronics P Majumdar - Magnetism P Sen – Magnetism K Raman – Spin devices and molecular spintronics A Tulapurkar- Spin devices and spin transport S Bandyopadhyay – Frontiers of spintronics !Part III: Nano-energy S. D. Mahanti – Thermoelectric energy conversion B. Muralidharan – Thermoelectric energy conversion !Part IV: Frontier topics B. Muralidharan – Information viewpoint of transport S. Ganguly – Bio memetics
!
Modeling device electronics
Bulk Solid (“macro”) (Classical Drift-Diffusion)
~ 1023 atoms
Bottom Gate
Source
Channel
Drain
Clusters (“meso”) (Semiclassical Boltzmann Transport)
80s ~ 106 atoms
Molecules (“nano”) (Quantum Transport)
Today ~ 10-100 atoms
(“Traditional Engg”)
(“Nano Engg”)
Nanoelectronics: New Paradigms and Possibilities
8
Part 1: Key concepts: !•Elastic resistor model, basic concepts of current flow, role of contacts, ballistic transport basics !
•Bottom up view point, Landauer approach, connection with diffusive transport, Concepts regarding conductivity !
•Role of electrostatics, case of nano transistor, drift-diffusion, Boltzmann transport formalism
Bottom up view point of transport
Drift Diffusion
Quantum theory
Quasi-Ballistic/Ballistic
( )∫∞
∞−
−Ξ= )()()( EfEfEdEI DS
“Top Down” … (EE 620/normal way of thinking)
Vd20 µm
Vd
2 nm
Solid State Electronics/ Mesoscopic Physics
Molecular Electronics
“Bottom Up” ... (EE 724)
Vd20 µm
Vd
2 nm
Solid State Electronics/ Mesoscopic Physics
Molecular Electronics
Bottom Up fabrication
Build pyramidal quantum dots from InAs atoms (Gerhard Klimeck, Purdue)
Bottom up architecture Chepren Pyramid, Giza (2530 BC)
Full quantum theory of nanodevices !• Carbon nanotubes, Graphene • Atomic wires, nanowires, • Point contacts, quantum dots, • thermoelectrics, • molecular electronics • Single electron Transistors (SETs) • Spintronics
Bottom up view point of transport
Diffusive
Quantum theory
0.1 mm !10 µm !1 µ m !0.1 µm !10 nm !1 nm !0.1 nm
Macroscopic dimensions
Atomic dimensions
��
€
γ /h
qVD(E)
€
µ2,T2
€
µ1,T1
�2/)()()( EEDE γ→Ξ
hEMLEvEDE /)(2/)()()( ≡→Ξ
22 /)()()()( LEEvEDE τ→Ξ
Anatomy of Nano-Devices: Point to Point
0µ1µ 2µ
Contacts/Leads Source/Drain electrodes
Channel
e-e-
Dynamics+ Dissipation
A possible evolution path?
Strained Si, SiGe (µ ~ 270cm2/Vs)
Bottom Gate
Source DrainTop Gate
Channel
15 nm
CNTs (µ ~ 10,000cm2/Vs) Hard to align into a circuit!
VG VD
INSULATOR
DRAIN
SOURCE
I
< 10 nm
Silicon Nanowires (Low µ < 100 cm2/Vs)
5 nmOrganic Molecules ?
(Reproducibility/ Gateability)
2 nm
Quantum transport: •Schoedinger equation, Hamiltonian, density of states, basic semiconductor physics from quantum mechanical viewpoint !•Examples of equilibrium calculations: concept of band structure, quantum wells, nanowires, carbon nanotubes, graphene, electrostatics, quantum capacitance !•Non-equilibrium transport: elastic resistor model re-visited from quantum transport perspective, introducing “contacts” to the Schroedinger equation, Green’s functions, self-energy, Non-equilibrium Green’s function (NEGF) formalism !•Application of the NEGF formalism to concrete examples: a) molecular electronics, b) nanowire transport, c) resonant tunnelling diodes
Nanoscale Devices: DOS determines everything!
( )∫∞
∞−
−Ξ= )()()( EfEfEdEI DS
�/γ
qVD(E)
€
µ2,T2
€
µ1,T1
Transport Function
Driving Force
DSDSqV µµ −=
I
V
Quantum Transport: DOS is the main thing!
��
€
γ /h
qVD(E)
€
µ2,T2
€
µ1,T1
S D S D
Effective mass + Poisson Equation
Tight Binding + Poisson Equation
Semi-empirical /Ab initio
The material ‘zoo’ !!
Strained Si, SiGe (µ ~ 270cm2/Vs)
Bottom Gate
Source DrainTop Gate
Channel
15 nm
CNTs (µ ~ 10,000cm2/Vs) Hard to align into a circuit!
VG VD
INSULATOR
DRAIN
SOURCE
I
< 10 nm
Silicon Nanowires (Low µ < 100 cm2/Vs)
5 nmOrganic Molecules ?
(Reproducibility/ Gateability)
2 nm
24
Molecular ElectronicsAviram-Ratner Diode: an acceptor-bridge-donor molecule Chem.Phys.Lett. (1974) 29, 277.
1. Electrode charge-injection to donor 2. Donor-Acceptor ET 3. Acceptor-electrode charge-injection
A molecular rectifier
Quantum Transport
��
€
γ /h
qVD(E)
€
µ2,T2
€
µ1,T1
S D S D
Effective mass + Poisson Equation
Tight Binding + Poisson Equation
Semi-empirical /Ab initio
CHARGE Spin
Energy
Part III: Charge Spintronics
Charge + SPIN degree of freedom
SPINTRONICS
Spintronics
Brief History
SV/MTJ DW NLSV QD
BUILDING BLOCKS
ULTRAFAST MAGNETIZATION DYNAMICS
SPINTRONIC INTERONNECTS
LOGIC MEMORY
BUILDING BLOCKS
Nanomagnetic logic
• Energy-efficient • Non-volatile • Fast • Radiation resistant
GMR technology
MRAM: Reading/writing process
Spin transfer torque (STT)
Future MRAM Improvements
Spin Torque Transfer !• No applied magnetic field
• Utilizes heavily spin polarized current • The magnetization of nano-elements is flipped back and forth • Still has challenges in basic physics and materials to overcome
MTJ DW NLSV QD
BUILDING BLOCKS
ULTRAFAST MAGNETIZATION DYNAMICS
SPINTRONIC INTERONNECTS
LOGIC MEMORY
CHARGE Spin
Energy
Part IV: Charge + Energy
Energy transport: •Introduction to nanoscale energy conversion devices, basics of thermoelectrics and photovoltaics !•Thermoelectric transport, energy conversion efficiency, low dimensional thermoelectrics !•Energy, entropy and heat currents, connection with second law
Nanocaloritronics Energy Conversion at nanoscale!
Electronic Maxwell’s demon
Batteries, Fuel cells and Nano-heat engines
Battery Operation Schematic
1µ 2µ
0µ
Active Region
Electrodes
fuel!cell
H2OO2H2
heat
work
Battery Operation Basics
Electrolysis (Chemistry)
fuel!cell
H2OO2
H2
heat
work
The familiar process of electrolysis requires work to proceed, if the process is put in reverse, it should be able to do work for us spontaneously. !The most basic “black box” representation of a fuel cell in action is shown below:
Figure 2
Battery Operation Basics
Electrolysis (Chemistry)
Figure 3
Battery Operation Basics
Fuel cells: Putting all together!
Figure 3
Battery Operation Basics
Some types!
What is the connection with nanoelectronic devices?
RECALL: Anatomy of Nano-Devices
0µ1µ 2µ
Contacts/Leads Source/Drain electrodes
Channel
e-e-
I
V
0=ΔT I
V
0>ΔT
Sapp VV =
Nanoscale Devices/Heat Engines?
00
≤Δ−Δ=Δ
≥Δ
STEFStot
1µ 2µ
MsappQ
nnn
JT
JVT
JT
S
JFS
TSEFHMNpVTSE
µ
µ
Δ−−Δ=
=
−=
++−=
∑11)1(�
�
21
2211 0NNNN
−=
≥+ µµ
12
2
2
1
1
NNT
ET
E
−=
−≥
− µµOnsager-Callen theory
1µ 2µ
T1 T2
50
POWER GENERATION: USING SEEBECK EFFECT REFRIGERATION:
USING PELTIER EFFECT
• Discovered in early 1800s –Seebeck and Peltier !
• Theory by Onsager-Callen -1930s !• Practical energy conversion ideas after 1950s—Ioffe !• Nanoscale energy conversion –after 2000s!
Thermoelectric energy conversion
Thermoelectric applications
T_H T_CV
TE
MacroscopicSeebeck effect
C H
I
TE
Peltier effect
T_H T_C
Ef
Seebeck effectMicroscopic
D(E)
C H
Peltier effect
Electron Engineering: Microscopic viewpoint
• Asymmetry in DOS results in a better TE material • Barriers create better TE cooling systems
What nano-world does?
• Distort ing the smooth DOS- DOS engineering !• Superlattices – Electron filtering
Engineering the Nanoscale-Basics
• Hicks and Dresselhaus: Sharp features in DOS (quantum wells, wires) would enhance zT due to energy filtering
• Sofo and Mahan: Delta-like DOS best for reaching Carnot efficiency
Hot Contact Cold Contact Channel
54
• Hicks and Dresselhaus: Sharp features in DOS (quantum wells, wires) would enhance zT due to energy filtering
• Sofo and Mahan: Delta-like DOS best for reaching Carnot efficiency
Hot Contact Cold Contact Channel
55
Engineering the DOS-Basics
• Hicks and Dresselhaus: Sharp features in DOS (quantum wells, wires) would enhance zT due to energy filtering
• Sofo and Mahan: Delta-like DOS best for reaching Carnot efficiency
Hot Contact Cold Contact Channel
56
Engineering the DOS-Basics
Modeling device electronics
Bulk Solid (“macro”) (Classical Drift-Diffusion)
~ 1023 atoms
Bottom Gate
Source
Channel
Drain
Clusters (“meso”) (Semiclassical Boltzmann Transport)
80s ~ 106 atoms
Molecules (“nano”) (Quantum Transport)
Today ~ 10-100 atoms
EE 620 (“Traditional Engg”)
ECE 724 (“Nano Engg”)
Bottom up view point of transport
Diffusive
Quantum theory
0.1 mm !10 µm !1 µ m !0.1 µm !10 nm !1 nm !0.1 nm
Macroscopic dimensions
Atomic dimensions
��
€
γ /h
qVD(E)
€
µ2,T2
€
µ1,T1
�2/)()()( EEDE γ→Ξ
hEMLEvEDE /)(2/)()()( ≡→Ξ
22 /)()()()( LEEvEDE τ→Ξ