PRESENTED BY:
JUSTIN GEORGE
University of Antwerpen
1
Allotropic forms of carbon
2
why carbon naotubes are so special?
 Electrical properties depend on geometry of nanotube
 Tremendous current carrying capacity
1 billion Amps/cm2
 Excellent heat conductor
twice as good as diamond
 High strength
much higher than high-strength steel
 Young Modulus ~ 1 TPa (SWNT) and 1.25 TPa (MWNT) (Steel: 230 Gpa)
 High Aspect Ratio: 1000 – 10,000
 Density: 1.3 – 1.4 g/cm3
 Maximum Tensile Strength: 30 GPa
 Thermal Conductivity: 2000 W/m.K (Copper has 400 W/m.K)
3
What is carbon nanotubes?
 Carbon nanotubes are a hexagonal shaped
arrangement of carbon atoms that has been rolled into
tubes.
Composites Science and Technology 61
(2001) 1899–1912
4
Carbon naotube family
5
Classification of carbon nanotubes
 Single walled carbon nanotubes (SWNT) (0.4 -2 nm)
 Multiwalled carbon nanotubes (MWNT) (2-100 nm)
 Metallic (n =m or n-m =3i, i is an interger)
 Semiconductor (all other cases)
Depends on the geometry
6
Diameter of the tube and chiral vector.
 The diameter d of the carbon nanubes are given by
Where is the nearest carbon-carbon bond
length and C is the chiral vector or roll-up vector.
where the chiral angle
7
Carbon nanotube synthesis
 Arc discharge
 Laser ablation
 CVD (chemical vapour deposition)
8
Arc discharge method
 cathode gets
consumed, CNTs in
cathodic soot
 structure of CNTs
depends on: current
I, voltage V, He gas
pressure, anode
material, distance
between the
electrodes
9
Arc discharge method
10
Laser vaporization
 Laser vaporizes the graphite target at high
temperature in an inert atmosphere
 nanotubes formed at the cooler surface of the
chamber as the vaporized carbon condenses.
11
Catalytic method
 Hydrocarbon in contact with hot metal nano particles
and decompose into hydrogen and carbon
 If the interaction with catalytic substrate is weak the
carbon diffuses down and push the nano particle up
“tip-growth model”
12
Characterization of CNT’s
 STM (Scanning tunneling
microscopy )
 AFM (Atomic force
microscopy)
 TEM (transmission
electron microscopy)
 SEM (scanning electron
microscopy)
 Raman spectroscopy
13
Quantum Effect
 Conductance appears to be ballistic over micron scales,
even at room temperature.
 Ballistic = no dissipation in the tube itself = very high
current densities are possible.
 Conductance increase with more CNTs are in contact with
liquid metal.
 Frank et al., Science 280, 1744 (1998).
14
Energy
Rayleigh
Scattering
(elastic)
The Raman effect comprises a very small fraction,
about 1 in 107 of the incident photons.
Stokes
Scattering
Anti-Stokes
Scattering
h 0
h 0
h 0
h 0 h 0 h m
h 0+h m
E0
E0+h m
Raman
(inelastic)
Virtual State
Raman scattering of CNT
16
Raman signals in SWNT’s
 Radial breathing mode (observed
up to 3 nm in SWNTs and
MWNTs )
 D-band (1350 ) –Resonant
nature.
 G-band (1530 -1620 )
 G’ band (depends on diameter of
CNTs)
 Other weak features.
 Resonance is diameter selective.
17
Significance of Raman signals
 RBM is useful to identify the presence of SWNT’s in
the carbon material and to determine the diameter of
SWNT’s.
 G-mode corresponds to planar vibrations of carbon
naotubes and is present in graphite like material
( carbon materials )
 D-mode generate from the structural defects of
graphite like carbon.
 G/D ratio is used to find quality of carbon nanotubes
(higher ratio, higher quality)
18
Radial-Breathing Mode
Diameter of the carbon
nanotube
Breathing mode : 100 – 350
The growth
temperature,
Diameter of nanotube increases with
increase in growth temperature
19
RBM as a function of diameter
 A particular diameter
is excited at a given
laser frequency
(Resonance Raman
effect)
 In a range of laser
frequency the RBM
frequency –diameter
plot can be made
which agree well with
the theory.
20
Temperature dependence of G-band
 Intensity of G-band
decreases exponentially with
temperature.
 The intensity is independent
of surface morphology and
preparation method.
 This can be used to measure
the temperature of the
sample.
 A shift in the G+ peak can
also be observed as the
temperature increases.
21
Distinction of SWNTs, DWNTs and
MWNTs using Raman spectroscopy
 Can distinguish
SWNT, DWNT
and MWNT from
a mixture of sample .
 G/D ratio show
MWNTs are low
quality.
22
Identify metallic and semiconductor
SWNT using Raman spectra.
 Frequency is independent of diameter but
depends on diameter and metallic and semiconductor
nature of SWNT .
 The frequency downshift of metallic SWNT is more
than semiconductor SWNT.
23
Characterization of water filled CNT using
Raman spectroscopy
 Resonance Raman
spectra of SWNT (a) S1
raw sample (c) air
oxidized and acid
treated sample (used to
open the SWNT).
 (b) and (d) are S1 and S2
respectively with empty
(0) and filled
nanotubes.

24
Nanotube elecronics
25
CNT gas sensors
 Chemical doping induces
a strong change in the
conductance.
 Detect small
concentration gas with
high sensitivity at room
temperature.
 Can detect NO2, NH3 etc.
with fast response time.
(Shu Peng and Kyeongjae Cho,
Department of Mechanical
Engineering, Stanford University)
26
AFM (atomic force microscopy )
 1. Laser
 2. Mirror
 3. Photodetector
 4. Amplifier
 5. Register
 6. Sample
 7. Probe
 8. Cantilever
 Uses van der Waals force
between the tip and the
surface
27
Nanotube as AFM tip
 Exceptional mechanical strength and large aspect ratio
 Survive tip crash due to accidental contact with
observation surface
 Slender and well defined tip, so higher resolution.
28
CNT mechanical sensors
 Conductance decreases as
the AFM tip pushes the
nanotube down, but recovers
as the tip retracts.
 Full reversibility of
conductance, so can be used
as a mechanical sensor.
29
CNT Nanothermometer
•Continuous, uni-dimensional column of Gallium in CNT
•Gallium has greatest liquid range (30 – 2,403 °C) and low vapour
pressure at high temperature.
• Height of liquid gallium varies linearly and reversibly with
temperature
• Expansion coefficient same as macroscopic gallium.
• Gallium meniscus perpendicular to inner surface of CNT
• Easy to read and suitable for microenvironment.
Gao and Bando, Nature (2002)
30
CNT nanobalance
 Nanobalance can measure a mass
small as 22 fg (femtogram)
 Time dependent voltage applied
cause time dependent force and
dynamic deflection, by adjusting the
frequency resonance excitation can
be achieved
 E, modulaus , L -length, t -
thickness, desnsity , effective mass
Most sensitive and smallest balance in the
world
Poncharal et al., Science (1999) 31
CNT infrared detector
 SWNT based IR
detectors have excellent
sensitivity, response
time, dark current
characteristics.
32
Applications of carbon nanotubes
33
Blacker than black
34
Electron field emission of CNT
 Electric field lines
concentrated on sharp
regions, since CNT have
sharp tip the geometry is
favorable for field
emission.
 Electron emission can
be observed with about
100 V on single CNT.
 Application in field
emission display.
35
Novel hard disk
 A novel data storage system
capable of 1015 bytes/cm2 is
being explored.
In this system, H atoms
would be designated as 0
and F atoms as 1.
A tip that can distinguish
between 0 and 1 rapidly and
unambiguously
is being investigated.
 http://www.ipt.arc.nasa.go
v/datastorage.html
36
Other applications
 Gas storage – as CNT has very large surface area gases
like Hydrogen can be absorbed and stored
 Super capacitor- can store large amount of energy and
can deliver very high peak power (CNT supercapacitor
have 7 times more energy density than commercial
activated carbon based supercapacitor)
 Nanomachines- CNT based nanogear with benzene
molecule bonded as teeth.
37
Thank you
38

Carbon nano materials

  • 1.
  • 2.
  • 3.
    why carbon naotubesare so special?  Electrical properties depend on geometry of nanotube  Tremendous current carrying capacity 1 billion Amps/cm2  Excellent heat conductor twice as good as diamond  High strength much higher than high-strength steel  Young Modulus ~ 1 TPa (SWNT) and 1.25 TPa (MWNT) (Steel: 230 Gpa)  High Aspect Ratio: 1000 – 10,000  Density: 1.3 – 1.4 g/cm3  Maximum Tensile Strength: 30 GPa  Thermal Conductivity: 2000 W/m.K (Copper has 400 W/m.K) 3
  • 4.
    What is carbonnanotubes?  Carbon nanotubes are a hexagonal shaped arrangement of carbon atoms that has been rolled into tubes. Composites Science and Technology 61 (2001) 1899–1912 4
  • 5.
  • 6.
    Classification of carbonnanotubes  Single walled carbon nanotubes (SWNT) (0.4 -2 nm)  Multiwalled carbon nanotubes (MWNT) (2-100 nm)  Metallic (n =m or n-m =3i, i is an interger)  Semiconductor (all other cases) Depends on the geometry 6
  • 7.
    Diameter of thetube and chiral vector.  The diameter d of the carbon nanubes are given by Where is the nearest carbon-carbon bond length and C is the chiral vector or roll-up vector. where the chiral angle 7
  • 8.
    Carbon nanotube synthesis Arc discharge  Laser ablation  CVD (chemical vapour deposition) 8
  • 9.
    Arc discharge method cathode gets consumed, CNTs in cathodic soot  structure of CNTs depends on: current I, voltage V, He gas pressure, anode material, distance between the electrodes 9
  • 10.
  • 11.
    Laser vaporization  Laservaporizes the graphite target at high temperature in an inert atmosphere  nanotubes formed at the cooler surface of the chamber as the vaporized carbon condenses. 11
  • 12.
    Catalytic method  Hydrocarbonin contact with hot metal nano particles and decompose into hydrogen and carbon  If the interaction with catalytic substrate is weak the carbon diffuses down and push the nano particle up “tip-growth model” 12
  • 13.
    Characterization of CNT’s STM (Scanning tunneling microscopy )  AFM (Atomic force microscopy)  TEM (transmission electron microscopy)  SEM (scanning electron microscopy)  Raman spectroscopy 13
  • 14.
    Quantum Effect  Conductanceappears to be ballistic over micron scales, even at room temperature.  Ballistic = no dissipation in the tube itself = very high current densities are possible.  Conductance increase with more CNTs are in contact with liquid metal.  Frank et al., Science 280, 1744 (1998). 14
  • 15.
    Energy Rayleigh Scattering (elastic) The Raman effectcomprises a very small fraction, about 1 in 107 of the incident photons. Stokes Scattering Anti-Stokes Scattering h 0 h 0 h 0 h 0 h 0 h m h 0+h m E0 E0+h m Raman (inelastic) Virtual State
  • 16.
  • 17.
    Raman signals inSWNT’s  Radial breathing mode (observed up to 3 nm in SWNTs and MWNTs )  D-band (1350 ) –Resonant nature.  G-band (1530 -1620 )  G’ band (depends on diameter of CNTs)  Other weak features.  Resonance is diameter selective. 17
  • 18.
    Significance of Ramansignals  RBM is useful to identify the presence of SWNT’s in the carbon material and to determine the diameter of SWNT’s.  G-mode corresponds to planar vibrations of carbon naotubes and is present in graphite like material ( carbon materials )  D-mode generate from the structural defects of graphite like carbon.  G/D ratio is used to find quality of carbon nanotubes (higher ratio, higher quality) 18
  • 19.
    Radial-Breathing Mode Diameter ofthe carbon nanotube Breathing mode : 100 – 350 The growth temperature, Diameter of nanotube increases with increase in growth temperature 19
  • 20.
    RBM as afunction of diameter  A particular diameter is excited at a given laser frequency (Resonance Raman effect)  In a range of laser frequency the RBM frequency –diameter plot can be made which agree well with the theory. 20
  • 21.
    Temperature dependence ofG-band  Intensity of G-band decreases exponentially with temperature.  The intensity is independent of surface morphology and preparation method.  This can be used to measure the temperature of the sample.  A shift in the G+ peak can also be observed as the temperature increases. 21
  • 22.
    Distinction of SWNTs,DWNTs and MWNTs using Raman spectroscopy  Can distinguish SWNT, DWNT and MWNT from a mixture of sample .  G/D ratio show MWNTs are low quality. 22
  • 23.
    Identify metallic andsemiconductor SWNT using Raman spectra.  Frequency is independent of diameter but depends on diameter and metallic and semiconductor nature of SWNT .  The frequency downshift of metallic SWNT is more than semiconductor SWNT. 23
  • 24.
    Characterization of waterfilled CNT using Raman spectroscopy  Resonance Raman spectra of SWNT (a) S1 raw sample (c) air oxidized and acid treated sample (used to open the SWNT).  (b) and (d) are S1 and S2 respectively with empty (0) and filled nanotubes.  24
  • 25.
  • 26.
    CNT gas sensors Chemical doping induces a strong change in the conductance.  Detect small concentration gas with high sensitivity at room temperature.  Can detect NO2, NH3 etc. with fast response time. (Shu Peng and Kyeongjae Cho, Department of Mechanical Engineering, Stanford University) 26
  • 27.
    AFM (atomic forcemicroscopy )  1. Laser  2. Mirror  3. Photodetector  4. Amplifier  5. Register  6. Sample  7. Probe  8. Cantilever  Uses van der Waals force between the tip and the surface 27
  • 28.
    Nanotube as AFMtip  Exceptional mechanical strength and large aspect ratio  Survive tip crash due to accidental contact with observation surface  Slender and well defined tip, so higher resolution. 28
  • 29.
    CNT mechanical sensors Conductance decreases as the AFM tip pushes the nanotube down, but recovers as the tip retracts.  Full reversibility of conductance, so can be used as a mechanical sensor. 29
  • 30.
    CNT Nanothermometer •Continuous, uni-dimensionalcolumn of Gallium in CNT •Gallium has greatest liquid range (30 – 2,403 °C) and low vapour pressure at high temperature. • Height of liquid gallium varies linearly and reversibly with temperature • Expansion coefficient same as macroscopic gallium. • Gallium meniscus perpendicular to inner surface of CNT • Easy to read and suitable for microenvironment. Gao and Bando, Nature (2002) 30
  • 31.
    CNT nanobalance  Nanobalancecan measure a mass small as 22 fg (femtogram)  Time dependent voltage applied cause time dependent force and dynamic deflection, by adjusting the frequency resonance excitation can be achieved  E, modulaus , L -length, t - thickness, desnsity , effective mass Most sensitive and smallest balance in the world Poncharal et al., Science (1999) 31
  • 32.
    CNT infrared detector SWNT based IR detectors have excellent sensitivity, response time, dark current characteristics. 32
  • 33.
  • 34.
  • 35.
    Electron field emissionof CNT  Electric field lines concentrated on sharp regions, since CNT have sharp tip the geometry is favorable for field emission.  Electron emission can be observed with about 100 V on single CNT.  Application in field emission display. 35
  • 36.
    Novel hard disk A novel data storage system capable of 1015 bytes/cm2 is being explored. In this system, H atoms would be designated as 0 and F atoms as 1. A tip that can distinguish between 0 and 1 rapidly and unambiguously is being investigated.  http://www.ipt.arc.nasa.go v/datastorage.html 36
  • 37.
    Other applications  Gasstorage – as CNT has very large surface area gases like Hydrogen can be absorbed and stored  Super capacitor- can store large amount of energy and can deliver very high peak power (CNT supercapacitor have 7 times more energy density than commercial activated carbon based supercapacitor)  Nanomachines- CNT based nanogear with benzene molecule bonded as teeth. 37
  • 38.