Title: Metallic-Enriched Single-Walled Carbon Nanotubes for Electronics Applications
1Metallic-Enriched Single-Walled Carbon Nanotubes
for Electronics Applications
- Erik H. Hároz
- NASA-Rice Nanotechnology Forum
- May 18, 2010
2Single-Walled Carbon Nanotubes
Chiral vector
Ch na1 ma2
n m 3M q
3Metallic Carbon Nanotubes
- Metallic SWNTs can be divided into two
subclasses, identifiable by their chiral indices
(n,m) - True metallic or armchair nanotubes where
(n-m)0 such as the (7,7) - Narrow-gap semiconducting nanotubes where (n-m)
integer multiple of 3 such as the (12,6) - Are ballistic conductors with electrical
conductivity 100x greater than copper and
electron mobility 70x that of silicon.
Current-carrying capacity 109 A/cm2. - Ideal materials for low-loss, high-capacity,
power transmission cables and nanometer-sized
electronics.
Tans et al., Nature, 386, (1997), 474
- Problems studying metallic SWNTs
- In bulk material, theoretically, 1/3 of all
possible chiralities are metallics.
Outnumbered by semiconductors. - In HiPco SWNTs, E22 semiconducting transitions
overlap with E11 metallic transitions. - Radial breathing mode of armchair SWNTs is very
weak in Raman spectra as compared to other
chiralities because the electron-phonon coupling
being weakest for armchair SWNTs.
Solution Make samples consisting of all
metallic SWNTs.
4Density Gradient Ultracentrifugation
HiPco HPR 188.1 SWNTs suspended in 1 sodium
deoxycholate (1mg/mL starting conc.) Sonicated
for about 30 min in bath sonicator, 20 hr in tip
sonicator, Decant prepared using 1hr
centrifugation _at_ 200,000g Run in a 40-20
iodixanol gradient in 1.5 sodium dodecyl
sulfate, 1.5 sodium cholate
Centrifugated for 18 hrs _at_ 200,000g
- Arnold et al., Nature Nanotechnology, 1, (2006),
60 - -Optical Absoprtion Characterization and sheet
conductance measurements - Yanagi et al., Applied Physics Express, 1,
(2008), 034003 - -Optical Absorption Single-line Excitation
Raman characterization - Iijima, et al., Nano Letters, 8, (2008), 3151
- - E-beam diffraction TEM chirality assignment of
Kataura sample
5Absorption Spectroscopy
- Sharp, narrow, well-defined peaks with large
absorbance in E11M region. - Flat, featureless section in E22S E11S regions.
- Overlap between E11M E22S regions eliminated.
- Absorption features have enhanced peak-to-valley
ratios. - Decrease in baseline of spectrum indicates
increase in degree of individuality. - Based on absorption peak areas, sample is 98
metallic.
- Peaks correspond to absorption of light at
energies corresponding to excitonic transitions
of specific (n,m) species of SWNTs - Transitions are roughly proportional to inverse
diameter but also depend on chiral angle and mod
as well. - Absorption is most direct optical method to
measure (n,m) species populations. - Sharpness of features and slope of baseline
qualitatively indicate degree of individuality.
x 0.1
x 2
6Photoluminescence Excitation Spectroscopy
Starting SWNT material
Metallic-enriched SWNTs
- Only individualized, wide-gap semiconducting
SWNTs fluoresce in the - near-infrared via visible excitation.
- ?Individualized, narrow-gap semiconducting SWNTs,
armchair SWNTs, - and bundles of SWNTs containing metallics do
not fluoresce.
7Resonant Raman Spectroscopy
- Resonant Raman scattering with a tunable
excitation source is the only optical method able
to identify all chiralities present, including
the armchairs (n,n). - Using excitation sources including
- CW TiSapphire laser (695-850 nm)
- Kiton red laser dye (610-685 nm),
- Rhodamine 6GB laser dye (562-615 nm),
- Ar laser (514.5, 501.7, 496.5, 488, 476.5,
457.8 nm) - doubled CW TiSapphire (500-440 nm)
- 5 weeks and 230 spectra later.
8Raman (562-670 nm)
Metallic-enriched HiPco
As-produced HiPco
9Raman (440-500 nm)
Metallic-enriched HiPco
As-produced HiPco
10Enrichment of Armchair Nanotubes
- Probing further using Raman scattering, we find
not only did we enrich in metallic nanotubes but - Of those metallic species, a large majority
(50) are armchairs (n,n).
Results summarized in Hároz et al., ACS Nano 4,
1955 (2010).
11Heading Towards Single Armchair Species Samples
12Absorption of Films UV-vis-NIR
- 100 SWNT films produced by vacuum filtration
from DGU-enriched solutions. - Sharp, narrow, well-defined peaks with large
absorbance in E11M region. - Metallic features remain relatively unperturbed
in film form probably due to screening. - Broadened, redshifted peaks in E22S E11S
regions.
13RBM Raman of DGU Films
(7,7)
514 nm excitation
Very little iodixanol
- Enrichment results in suppression of (8,5),
(9,3) (8,2) leaves behind mostly (7,7). - Very little density gradient medium left.
(8,5)
(8,2)
(9,3)
14Absorption of Films Terahertz
- THz examines optical conductivity.
- Response thought to be due to concentration of
metallic SWNTs (i.e. THz absorbance proportional
to conductivity). - Although metallic films have lower overall
optical absorption, they possess greater more
metallic nanotubes.
15How can these materials be used in research?
- In the Kono group, we are using these enriched
materials to look at - Temp. dependent DC magneto-transport
- Optical spectroscopy
- Electron spin resonance
- Ultrafast spectroscopy
- Terahertz conductivity
- Pump-probe
- We are also looking at ways to scale separations
using column chromatography
16Armchair Quantum Wire Program
- More broadly at Rice, we are engaged in trying to
create macroscopic structures (films and wires)
comprised of armchair nanotubes. - Primary question to answer
- While individual armchair SWNTs are excellent
ballistic conductors, how about in
macrostructures? - What dominates, tunneling barriers (i.e. variable
range hopping)? Can this be overcome?
17Acknowledgements
- Prof. Junichiro Kono (Rice, advisor)
- Prof. R. Bruce Weisman (Rice)
- Dr. Stephen K. Doorn (LANL)
- Dr. Robert H. Hauge (Rice)
- Mr. William D. Rice (Rice)
- Mr. Saunab Ghosh (Rice)
- Mr. Benjamin Y. Lu (Rice)
- Mr. Budihpta Dan (Rice)
- Mr. Lei Ren (Rice)
- Funding provided by DOE, AFRL, NSF, LANL LDRD
program, and Welch Foundation.