Metallic-Enriched Single-Walled Carbon Nanotubes for Electronics Applications - PowerPoint PPT Presentation

1 / 17
About This Presentation
Title:

Metallic-Enriched Single-Walled Carbon Nanotubes for Electronics Applications

Description:

Photoluminescence Excitation Spectroscopy Starting SWNT material Metallic-enriched SWNTs Only individualized, wide-gap semiconducting SWNTs fluoresce in the near- ... – PowerPoint PPT presentation

Number of Views:203
Avg rating:3.0/5.0
Slides: 18
Provided by: Erik150
Category:

less

Transcript and Presenter's Notes

Title: Metallic-Enriched Single-Walled Carbon Nanotubes for Electronics Applications


1
Metallic-Enriched Single-Walled Carbon Nanotubes
for Electronics Applications
  • Erik H. Hároz
  • NASA-Rice Nanotechnology Forum
  • May 18, 2010

2
Single-Walled Carbon Nanotubes
Chiral vector
Ch na1 ma2
n m 3M q
3
Metallic 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.
4
Density 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

5
Absorption 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
6
Photoluminescence 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.

7
Resonant 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.

8
Raman (562-670 nm)
Metallic-enriched HiPco
As-produced HiPco
9
Raman (440-500 nm)
Metallic-enriched HiPco
As-produced HiPco
10
Enrichment 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).
11
Heading Towards Single Armchair Species Samples
12
Absorption 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.

13
RBM 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)
14
Absorption 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.

15
How 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

16
Armchair 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?

17
Acknowledgements
  • 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.
Write a Comment
User Comments (0)
About PowerShow.com