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The Applications of Nano Materials

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Title: The Applications of Nano Materials


1
The Applications of Nano Materials
  • Department of Chemical and Materials Engineering
  • San Jose State University

Zhen Guo, Ph. D.
2
How to study Nanomaterials
Part I -- Done
Basic Materials Science Principles
Microstructure
Properties
Materials
Applications
Processing
Part II Done
Part III This one
3
The Applications of Nano Materials
Electronics
Magnetic Device
Structure
Nano Materials Applications
Optics
Daily Life consumable
Renewable Energy
MEMS
Bio Device
4
Applications of Nano Materials
5
Session X Nano Electric Materials
-- Single Electron Transistor -- Other Novel
Transistor -- Nano Crystal Memory -- Phase
Change Memory
6
MOSFET Principles
  • Review MOSFET principles accumulations,
    depletion, and inversion. Vt, Vg, Ids, Idsat,
    etc.
  • Just remember that Electrons are like water,
    source / drain like two bottles, channel is a
    pipe in between and gate is like a valve to open
    / close the pipe...

7
Single Electron Box
  • Single Electron Box
  • One Quantum Dot
  • Two Electrodes
  • Tunneling Junction
  • Control Gate Capacitor
  • Electrons are injected/ejected into / from
    quantum dots thru tunneling junctions.
  • Extra electrons injected into quantum dots will
    lead to excessive charging energy

Courtesy from Rainer Waser Nano-electronics and
Information technology PP427-445
8
Coulomb Blockade
  • Coulomb Blockade is caused by excessive charging
    energy Wc which increase as the size of quantum
    dot decrease

With adding extra electron into QD
r? gt Csp? gt Wc?
Wce2/2Csp
When Wc gtgt kT, thermal energy is no longer
sufficient to overcome excessive charging energy
gt Coulomb Blockade
  • Quantum Effect of Coulomb Blockade Quantum
    confinement cause energy level split gt next
    electrons may need to occupy higher energy level

Wc e2/2Csp DE (n)
http//www.plus2physics.com/capacitors/study_mater
ial.asp
9
Bias Condition for Coulomb Blockade
  • When gate voltage is zero, the charge at quantum
    dot is zero.
  • As gate voltage increases to a certain value,
    electrons are attracted to quantum dot, making 1e
    net charge of dot
  • Further increase gate voltage will increase
    electron number.

10
Bias Condition for Coulomb Blockade
  • To maintain the electron number in quantum dots,
    we have
  • To substitute the equations in previous slide, we
    obtained

When Consider both sides, we have
or
Courtesy from Rainer Waser Nano-electronics and
Information technology
11
Single Electron Transistor (SET)
  • SET three terminal switching device that can
    transfer electron one by one from source to drain

-- can be considered as two independent tunneling
junctions -- Each will have to satisfy Coulomb
Blockade conditions
Courtesy from Rainer Waser Nano-electronics and
Information technology
12
Single Electron Transistor (SET)
Cond Two Equations can be reduced to
Source Blue Line
Drain Red Line
  • In grey area, both source and drain satisfy
    coulomb blockade condition for same n
    valuegtFixed electrons.
  • In green area, source and drain satisfy
    different value.
  • -- In Area A, for source junction, it satisfy n1
    so one electron will tunnel from source to QD
  • -- Once electron at QD, it found that drain
    junction is favor n0 so this electron will
    further tunnel to drain
  • -- Current Flow from source to drain
  • -- Giving a small Vds, Ids will vary with Vg
    periodically
  • -- Vg can behave as a switch. Vg0, need Vds
    greater than threshold, Vge/2Cg, linear Ids
    verse Vds

13
Fabrication of SET (I)
  • PADOX Pattern Dependent Oxidization
  • -- 1-D Si Nano Wire connected with 2-D Si layers
    at both ends
  • -- Oxidization process forms tunneling barriers
    at both ends.
  • -- Can be either width or thickness modulated.
  • -- For Vertical PADOX, it is possible to form 2
    tiny islands

14
Fabrication of SET (II)
  • Surface-Treated SOI Channel
  • -- 1-D SOI channel intentionally undulated with
    alkaline based solutions
  • -- The nano scaled undulation results in
    potential fluctuation due to the difference of
    quantum confinement effect from one part to
    another.
  • -- The channel effectively splits into several
    quantum dots.
  • -- Process is completely compatible with current
    CMOS fabrications

15
Advantage and Disadvantages
  • Advantages
  • Lower power assumption
  • Good scalability
  • Disadvantages
  • Operated usually at low temperature
  • High output impedance due to tunneling
  • Vds has to be less than Vg to have gate fully
    control the switch.

16
Other Novel Logic Transistor
  • Ferro-Electric Field Effect Transistor (FeFET)

-- On state for positive gate voltage, the
polarization vector P is directed towards
Channel. -- Cohesive voltage Vc keep remanent
polarization Pr large enough to invert channel
and keep current flow even when Vg0
(non-volatile operation) -- Off State negative
gate voltage will bring Pr direct opposite to
channel and charge are accumulated in the
channel region. Channel resistance is high and no
current flow
Courtesy from Rainer Waser Nano-electronics and
Information technology
17
Other Novel Logic Transistor
  • Spintronic transistor based on the effect of
    spin orientation on electrons transportation
    properties

-- Source and drain are both ferro-magnetic
materials with identical magnetization
direction -- Channel is a hetero-junction of
semiconductor compound with a highly mobile 2-D
electron gas. -- Source will inject a
spin-polarized current into channel. Without gate
voltage, spin will remain unchanged so electron
travel to drain on a very high velocity (1 of
speed of light) -- When applied gate voltage,
spin direction will be rotated by magnetic field
so the spin is no longer aligned with drain side
gt More scattering, higher resistance, lower
velocity.
18
Other Novel Logic Transistor
  • Molecular transistor Single Molecular acting
    as electronic switch and storage elements

19
Nano Crystal Memory
  • Introduction
  • Why Nano Crystal Memory
  • New Development on Nano Crystal Memory

20
(No Transcript)
21
Recent Trend in Non-volatile Memory
  • Current flash memory is continuing to follow
    Moores Law at 90 / 65 / 45nm Nodes
  • -- 18 years for 9 generations
  • ETOX and NAND will still be the mainstream flash
    memory in next 5 years.
  • There is no clear roadmap to continuously scale
    flash memory beyond 32nm node.

22
ITRS Roadmap for Emerging Memory Device (2003)
63
23
Nano-crystal Memory for Technology Gap
S. J. Baik et al, IDEM, 2003
24
Principle of Nano Crystal Memory
Improvement of Data Retention and SILT.
25
Nano Crystal as Storing Bit
  • Nano Crystal Technology has been studied
    extensively to replace traditional floating gate
    as charge storage media.
  • Advantages
  • Scalability with Channel Tunneling and Erase
  • Compatible with Traditional CMOS Platform
  • Improved Charge Retention and Endurance
  • Potential Multi Bit usage
  • Challenges
  • Strictly control the size and distribution of
    nano crystals
  • Still Litho node limited
  • Much work to be done for a integrated reliable
    and high yield process

26
Silicon Nano Crystal as Storing Media
  • Reduce SILC and thus improve data retention and
    endurance
  • Decrease gate coupling and thus improve leakage
    and erase saturation
  • Possible multi-bit storage as particle size goes
    down to discrete energy state of electrons

R. Muralidhar et al. IDEM, 2003
27
Metal Dots as Storage Media
C. Lee, et al, IDEM, 2003
  • Metal dots can be Co, W or Au
  • Suppose to be better than Si as work function is
    higher (more attractive to electrons)
  • Multilayer can improve retention and endurance

M. Takata, et al, IDEM, 2003
28
Silicon Nano Crystals Produced by CVD Methods (I)
  • A Si-rich SiOx thin film is deposited on Si
    surface by PECVD method. The non-stoichemetry are
    controlled by gas flow ratios.
  • An furnace annealing were performed on this film
    at 1000C in N2 atmosphere to precipitate Si Nano
    crystals out of supersaturated film.

-- U.S. Pattern Pending
29
Si SiO2 Binary Phase Diagram -- Si has no
solubility in SiO2 at equilibrium state
30
Silicon Nano Crystals Produced by CVD Methods (II)
  • Thermal Decomposition of SiH4 precursor on
    Silicon surface for Si Nano crystals .
  • No Anneal Step is required.
  • Most compatible with current CMOS technology.
  • Challenge is how to control location and size
    distribution.

-- U.S. Pattern Pending
31
Other Ideas of Synthesis Nano Crystals
  • Controllable Nucleation and Growth
  • Volmer-Weber Growth (3-D Island Growth) on Thin
    Film
  • In-Situ Phase Segregation (Spinodal
    Decomposition)
  • Pre-patterned Growth (Polymer Precursor
    Self-assembly)

32
Summary
  • Nano storing bit can and must meet Si technology
    in 5 years.
  • Nano crystal memory is the most promising one to
    be compatible with CMOS platform
  • Many challenges still exist ranging from
    manufacturing nano particles to integration into
    traditional process flow
  • Materials scientist can definitely help!

33
Phase Transformation Memory
  • Same principle as DVD
  • Using transformation between amorphous and
    crystalline phase based on cooling speed.
  • Different phases has different optical and
    electrical properties.
  • Easy to be integrated and scalable.

34
Stephen Lai, Intel, December 2003.
35
Basic Architecture of Nano Crystal Memory
S. Tiwari et al. Appl, Phy lett, 1996
R. Muralidhar et al. IDEM, 2003
Floating nano crystals can be -- Silicon nano
crystals (multiple or single) -- Silicon nano
wires -- Metal nano dots (single or Multi
layers)
36
Nucleation and Growth Control
  • Nano particles need strong nucleation and slow
    growth
  • Low temperature (high DT) promote nucleation and
    slow down growth
  • The distance among nucleation sites has to be
    bigger than diffusion length
  • Nucleus size should be controlled around
    critical radius

37
Volmer-Weber Growth
  • 3-D island growth
  • Neither complete wetting nor complete
    non-wetting surface
  • Island size and distribution controlled by
    heterogeneous nucleation sites

38
Spinodal Decomposition
  • Spontaneous transformation due to instability
  • No nucleation barriers-only require local
    compositional fluctuations
  • Wave length (or particle size) is a function of
    undercooling
  • Misfit strain will also play a key role in
    particle size (barriers for growth)

39
Self-Assembly Patterning
K. W. Guarini et. al. IDEM, 2003
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