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E L L I O T Y O U N G – L Y D I N G G R O U P
U N I V E R S I T Y O F I L L I N O I S
O C T O B E R 2 0 T H , 2 0 1 5
Characterization of Low-Dimensional
Tantalum Trisulfide using Scanning
Tunneling Microscopy
1
Where I Work
2
Where I Work
3
Introduction
 Tantalum trisulfide (TaS3) and other transition metal trichalcogenides have
unique electronic properties
 Approach material limits as silicon-based devices continue to shrink – look to
alternative materials to continue improvement in integrated circuits industry
 Hard to use CNTs due to difficulties with CVD fabrication techniques,
especially size differences in the nanotubes
 TaS3 retains one-dimensional structure with same dimensions every time
Meerschaut et al. J. Less Common Met 1975
4
Background
 Orthorhombic TaS3 deposited via DCT on H-passivated p-type Si (100)
 Bulk crystal grown via physical vapor transport
 Planar arrangement of crystal chains thought to
resemble structure of ZrSe3
 Previous work gives lattice constants a = 36.804 Å,
b = 15.173 Å, and c = 3.340 Å (Bjerkelund et al. 1964)
 Metallic at room temp. in bulk and at nano scale
T.B. Kilpatrick thesisLyding et al. Phys. Rev. B 1989
5
b
a
Background
6
Roucau et al. Phys. status solidi 1980
a = 36.804 Å
b = 15.173 Å
c = 3.340 Å
b
a
c
Goals
 Measure step height, row spacing, and modulation
along row axis and compare with previously reported
lattice constants
 Investigate band gap for different flake sizes TaS3
 Obtain high-resolution images of two-dimensional
TaS3
7
Step Height
11.7 Å 12.5 Å
Histogram analysis shows a step height
of approximately 12 Å
8
Roucau et al. Phys. status solidi 1980
Image taken at 0.1 nA, -3.5 V
Row Spacing
Average row spacing: 15.5 Å
Local modulation: 4.48 Å
9
Lyding et al. Phys. Rev. B 1989
Image taken at 0.1 nA, -3.5 V
Row Spacing
Row spacing: 16.88 Å
Local modulation: 4.15 Å
Shows three secondary peaks instead of just two and
with peak spacing ~0.3 Å smaller
10
Images taken at 0.1 nA, -3.5 V
Row Spacing
11
Images taken at 0.1 nA, -3.5 V
Measuring Modulation Along Row Axis
Measured spacing between features along row axis ~ 12.1 Å
12
Meerschaut et al. J. Less Common Met 1975
Images taken at 0.1 nA, -2.5 V
Measuring Modulation Along Row Axis
13
Image taken at 0.1 nA, -2.5 V
Small Flake Analysis
14
Image taken at 0.1 nA, -3.5 V
Band Gap for Small Flake
15
Images taken at 0.1 nA, -2.5 V
Spectroscopy for Small Flake
16
Spectroscopy data shows band gap of 1.1 eV on silicon and no band gap (metallic)
on flake with modulation corresponding to the row spacing (~1.2 nm)
Image taken at 0.1 nA, -2.5 V
Spectroscopy for Small Flake
17
Spectroscopy for Small Flake
18
1.1 eV
TaS3 Row Intersection
19
Images taken at 0.1 nA, -3.5 V
TaS3 Flake
20
Images taken at 0.1 nA, -3.5 V
Future Goals
 Peel off rows from flake using tip (ideally single row)
 Further investigate variances in row structure
 Collect spectroscopy data on single layer flakes
smaller than 10 nm
 Develop definitive model for crystal structure of
orthorhombic TaS3
21
Conclusions
 Step height of approximately 12 Å, about 1/3 of the lattice constant (36.804 Å)
 Row spacing of approximately 15.5 Å, which is in agreement with the lattice
constant (15.173 Å)
 Modulation along the chain axis with spacing 12.1 Å, which is approximately 4x
the lattice constant (3.340 Å)
 Rows appear to have either two or three local peaks, which could be due to how
sharply zig-zagged the rows are or the orientation angle between rows
 Spectroscopy data shows metallic behavior for
all sizes and arrangements larger than 10 nm
22
Lyding et al. Phys. Rev. B 1989
Acknowledgments
23
 Professor Lyding
 Lyding Group

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Research Update 1

  • 1. E L L I O T Y O U N G – L Y D I N G G R O U P U N I V E R S I T Y O F I L L I N O I S O C T O B E R 2 0 T H , 2 0 1 5 Characterization of Low-Dimensional Tantalum Trisulfide using Scanning Tunneling Microscopy 1
  • 4. Introduction  Tantalum trisulfide (TaS3) and other transition metal trichalcogenides have unique electronic properties  Approach material limits as silicon-based devices continue to shrink – look to alternative materials to continue improvement in integrated circuits industry  Hard to use CNTs due to difficulties with CVD fabrication techniques, especially size differences in the nanotubes  TaS3 retains one-dimensional structure with same dimensions every time Meerschaut et al. J. Less Common Met 1975 4
  • 5. Background  Orthorhombic TaS3 deposited via DCT on H-passivated p-type Si (100)  Bulk crystal grown via physical vapor transport  Planar arrangement of crystal chains thought to resemble structure of ZrSe3  Previous work gives lattice constants a = 36.804 Å, b = 15.173 Å, and c = 3.340 Å (Bjerkelund et al. 1964)  Metallic at room temp. in bulk and at nano scale T.B. Kilpatrick thesisLyding et al. Phys. Rev. B 1989 5 b a
  • 6. Background 6 Roucau et al. Phys. status solidi 1980 a = 36.804 Å b = 15.173 Å c = 3.340 Å b a c
  • 7. Goals  Measure step height, row spacing, and modulation along row axis and compare with previously reported lattice constants  Investigate band gap for different flake sizes TaS3  Obtain high-resolution images of two-dimensional TaS3 7
  • 8. Step Height 11.7 Å 12.5 Å Histogram analysis shows a step height of approximately 12 Å 8 Roucau et al. Phys. status solidi 1980 Image taken at 0.1 nA, -3.5 V
  • 9. Row Spacing Average row spacing: 15.5 Å Local modulation: 4.48 Å 9 Lyding et al. Phys. Rev. B 1989 Image taken at 0.1 nA, -3.5 V
  • 10. Row Spacing Row spacing: 16.88 Å Local modulation: 4.15 Å Shows three secondary peaks instead of just two and with peak spacing ~0.3 Å smaller 10 Images taken at 0.1 nA, -3.5 V
  • 11. Row Spacing 11 Images taken at 0.1 nA, -3.5 V
  • 12. Measuring Modulation Along Row Axis Measured spacing between features along row axis ~ 12.1 Å 12 Meerschaut et al. J. Less Common Met 1975 Images taken at 0.1 nA, -2.5 V
  • 13. Measuring Modulation Along Row Axis 13 Image taken at 0.1 nA, -2.5 V
  • 14. Small Flake Analysis 14 Image taken at 0.1 nA, -3.5 V
  • 15. Band Gap for Small Flake 15 Images taken at 0.1 nA, -2.5 V
  • 16. Spectroscopy for Small Flake 16 Spectroscopy data shows band gap of 1.1 eV on silicon and no band gap (metallic) on flake with modulation corresponding to the row spacing (~1.2 nm) Image taken at 0.1 nA, -2.5 V
  • 18. Spectroscopy for Small Flake 18 1.1 eV
  • 19. TaS3 Row Intersection 19 Images taken at 0.1 nA, -3.5 V
  • 20. TaS3 Flake 20 Images taken at 0.1 nA, -3.5 V
  • 21. Future Goals  Peel off rows from flake using tip (ideally single row)  Further investigate variances in row structure  Collect spectroscopy data on single layer flakes smaller than 10 nm  Develop definitive model for crystal structure of orthorhombic TaS3 21
  • 22. Conclusions  Step height of approximately 12 Å, about 1/3 of the lattice constant (36.804 Å)  Row spacing of approximately 15.5 Å, which is in agreement with the lattice constant (15.173 Å)  Modulation along the chain axis with spacing 12.1 Å, which is approximately 4x the lattice constant (3.340 Å)  Rows appear to have either two or three local peaks, which could be due to how sharply zig-zagged the rows are or the orientation angle between rows  Spectroscopy data shows metallic behavior for all sizes and arrangements larger than 10 nm 22 Lyding et al. Phys. Rev. B 1989

Hinweis der Redaktion

  1. Unique properties such as ballistic transport of charge carriers, which is when electrons can move in a material with negligible scattering (very low resistivity). Figure shows model of individual NbSe3 (niobium triselenide) crystal chains showing triangular prism structure