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
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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
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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
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b
a
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
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8. Step Height
11.7 Å 12.5 Å
Histogram analysis shows a step height
of approximately 12 Å
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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
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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
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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
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Meerschaut et al. J. Less Common Met 1975
Images taken at 0.1 nA, -2.5 V
15. Band Gap for Small Flake
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Images taken at 0.1 nA, -2.5 V
16. Spectroscopy for Small Flake
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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
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
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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
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Lyding et al. Phys. Rev. B 1989
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