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Sub-bandgap Voltage Electroluminescence and Magneto-oscillations in a WSe2 Light-Emitting van der Waals Heterostructure.

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A threshold voltage for electroluminescence significantly lower than the corresponding single particle band gap of monolayer WSe2 is observed, interpreted by considering the Coulomb interaction and a tunneling process involving excitons, well beyond the picture of independent charge carriers.
Abstract
We report on experimental investigations of an electrically driven WSe2 based light-emitting van der Waals heterostructure. We observe a threshold voltage for electroluminescence significantly lower than the corresponding single particle band gap of monolayer WSe2. This observation can be interpreted by considering the Coulomb interaction and a tunneling process involving excitons, well beyond the picture of independent charge carriers. An applied magnetic field reveals pronounced magneto-oscillations in the electroluminescence of the free exciton emission intensity with a 1/B periodicity. This effect is ascribed to a modulation of the tunneling probability resulting from the Landau quantization in the graphene electrodes. A sharp feature in the differential conductance indicates that the Fermi level is pinned and allows for an estimation of the acceptor binding energy.

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The University of Manchester Research
Sub-bandgap voltage electroluminescence and magneto-
oscillations in a WSe2 light-emitting van der Waals
heterostructure
DOI:
10.1021/acs.nanolett.6b04374
Document Version
Accepted author manuscript
Link to publication record in Manchester Research Explorer
Citation for published version (APA):
Binder, J., Withers, F., Molas, M. R., Faugeras, C., Nogajewski, K., Watanabe, K., Taniguchi, T., Kozikov, A.,
Geim, A., Novoselov, K., & Potemski, M. (2017). Sub-bandgap voltage electroluminescence and magneto-
oscillations in a WSe2 light-emitting van der Waals heterostructure. Nano Letters.
https://doi.org/10.1021/acs.nanolett.6b04374
Published in:
Nano Letters
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Download date:26. Aug. 2022

❙✉❜✲❜❛♥❞❣❛♣ ✈♦❧t❛❣❡ ❡❧❡❝tr♦❧✉♠✐♥❡s❝❡♥❝❡ ❛♥❞
♠❛❣♥❡t♦✲♦s❝✐❧❧❛t✐♦♥s ✐♥ ❲❙❡
2
❧✐❣❤t✲❡♠✐tt✐♥❣
✈❛♥ ❞❡r ❛❛❧s ❤❡t❡r♦str✉❝t✉r❡
❏♦❤❛♥♥❡s ❇✐♥❞❡r✱
r❡❞❞✐❡ ❲✐t❤❡rs✱
§
▼❛❝✐❡❥ ❘✳ ▼♦❧❛s✱
❈❧❡♠❡♥t ❛✉❣❡r❛s✱
❑❛r♦❧ ◆♦❣❛❥❡✇s❦✐✱
❑❡♥❥✐ ❛t❛♥❛❜❡✱
k
❛❦❛s❤✐ ❛♥✐❣✉❝❤✐
k
❆❧❡❦s❡② ♦③✐❦♦✈✱
§
❆♥❞r❡ ❑✳ ●❡✐♠✱
§
st ❙✳ ◆♦✈♦s❡❧♦✈✱
§
❛♥❞ ▼❛r❡❦ P♦t❡♠s❦✐
❛❜♦r❛t♦✐r ◆❛t✐♦♥❛❧ ❞❡s ❈❤❛♠♣s ▼❛❣♥❡t✐q✉❡s ■♥t❡♥s❡s✱ ✲❯●❆✲❯P❙✲■◆❙❆✲❊▼❋▲
✷✺ ✉❡ ❞❡s ▼❛rt②rs✱ ✸✽✵✹✷ ●r❡♥♦❜❧❡✱ r❛♥❝
❛❝✉❧t② ♦❢ P❤②s✐❝s✱ ❯♥✐✈❡rs✐t② ♦❢ ❛rs❛✇✱ P❛st❡✉r ✺✱ ✵✷✲✵✾✸ ❛rs❛✇✱ P♦❧❛♥❞
❙❝❤♦♦❧ ♦❢ P❤②s✐❝s ❛♥❞ ❆str♦♥♦♠②✱ ❯♥✐✈❡rs✐t② ♦❢ ▼❛♥❝❤❡st❡r✱ ❖①❢♦r ❛❞✱ ▼❛♥❝❤❡st❡r
▼✶✸ ✾P▲✱ ❯❑
§
◆❛t✐♦♥❛❧ ●r❛♣❤❡♥❡ ■♥st✐t✉t❡✱ ❯♥✐✈❡rs✐t② ♦❢ ▼❛♥❝❤❡st❡r✱ ❖①❢♦r ❛❞✱ ▼❛♥❝❤❡st❡r✱ ▼✶✸
✾P▲✱ ❯❑
k
◆❛t✐♦♥❛❧ ■♥st✐t✉t❡ ❢♦r ▼❛t❡r✐❛❧s ❙❝✐❡♥❝❡✱ ✶✲✶ ◆❛♠✐❦✐✱ ❚s✉❦✉❜ ✵✺✲✵✵✹✹✱ ❏❛♣❛♥
▼❛♥❝❤❡st❡r ❈❡♥tr ❢♦r ▼❡s♦s❝✐❡♥❝ ❛♥❞ ◆❛♥♦t❡❝❤♥♦❧♦❣②✱ ❯♥✐✈❡rs✐t② ♦❢ ▼❛♥❝❤❡st❡r✱
❖①❢♦r ❛❞✱ ▼❛♥❝❤❡st❡r✱ ▼✶✸ ✾P▲✱ ❯❑
❊✲♠❛✐❧✿ ❥♦❤❛♥♥❡s✳❜✐♥❞❡r❅❢✉✇✳❡❞✉✳♣❧❀ ♠❛r❡❦✳♣♦t❡♠s❦✐❅❧♥❝♠✐✳❝♥rs✳❢r
P❤♦♥❡✿ ✰✹✽ ✷✷ ✺✺ ✸✷ ✼✾✷❀ ✰✸✸ ✹✼✻ ✽✽ ✼✽ ✼✻
❆❜str❛❝t
r❡♣♦rt ♦♥ ❡①♣❡r✐♠❡♥t❛❧ ✐♥❡st✐❣❛t✐♦♥s ♦❢ ❛♥ ❡❧❡❝tr✐❝❛❧❧② ❞r✐✈❡♥ ❲❙❡
2
❜❛s❡❞ ❧✐❣❤t✲
❡♠✐tt✐♥❣ ❛♥ ❞❡r ❛❛❧s ❤❡t❡r♦str✉❝t✉r❡✳ ♦❜s❡r✈ t❤r❡s❤♦❧❞ t❛❣❡ ❢♦r ❡❧❡❝tr♦❧✉✲

♠✐♥❡s❝❡♥❝❡ s✐❣♥✐✜❝❛♥t❧② ❧♦❡r t❤❛♥ t❤❡ ❝♦rr❡s♣♦♥❞✐♥❣ s✐♥❣❧❡ ♣❛rt✐❝❧❡ ❜❛♥❞ ❣❛♣ ♦❢ ♠♦♥♦✲
❧❛❡r ❲❙❡
2
❚❤✐s ♦❜s❡r✈❛t✐♦♥ ❝❛♥ ✐♥t❡r♣r❡t❡❞ ❝♦♥s✐❞❡r✐♥❣ t❤❡ ❈♦❧♦♠ ✐♥t❡r❛❝
t✐♦♥ ❛♥❞ t✉♥♥❡❧✐♥❣ ♣r♦❝❡ss ✐♥♦❧✈✐♥❣ ❡①❝✐t♦s✱ ❡❧❧ ❡②♦♥❞ t❤❡ ♣✐❝t✉r❡ ♦❢ ✐♥❞❡♣❡♥❞❡♥t
❤❛r❣❡ ❝❛rr✐❡rs✳ ❆♥ ❛♣♣❧✐❡❞ ♠❛❣♥❡t✐❝ ✜❡❧❞ r❡✈❡❛❧s ♣r♦♥♦✉♥❝❡❞ ♠❛❣♥❡t♦✲♦s❧❧❛t✐♦♥s ✐♥
t❤❡ ❡❧❡❝tr♦❧✉♠✐♥❡s❝❡♥❝❡ ♦❢ t❤❡ ❢r❡❡ ❡①❝✐t♦♥ ❡♠✐ss✐ ✐♥t❡♥s✐t ✇✐t❤ ✶✴❇✲♣❡r✐♦❞✐❝✐t
❚❤✐s ❡✛❡❝t ✐s ❛s❝r✐❜❡❞ t♦ ♠♦❞✉❧❛t✐♦♥ ♦❢ t❤❡ t✉♥♥❡❧✐♥❣ ♣r♦❜❛❜✐❧✐t r❡s✉❧t✐♥❣ ❢r♦♠ t❤
▲❛♥❞❛✉ q✉❛♥t✐③❛t✐♦♥ ✐♥ t❤❡ ❣r❛♣❤❡♥❡ ❡❧❡❝tr♦❞❡s✳ s❤❛r♣ ❢❡❛t✉r❡ ✐♥ t❤ ❞✐✛❡r❡♥t✐❛❧
❝♦♥❞✉❝t❛♥❝❡ ✐♥❞✐❝❛t❡s t❤❛t t❤❡ ❡r♠✐ ❧❡✈❡❧ ✐s ♣✐♥♥❡❞ ❛♥❞ ❛❧❧♦✇s ❢♦r ❛♥ ❡st✐♠❛t✐♦♥ ♦❢ t❤❡
❛❝❝❡♣t♦r ✐♥❞✐♥❣ ❡♥❡r❣②
❑❡②✇♦r❞s
❡❧❡❝tr♦❧✉♠✐♥❡s❝❡♥❝❡✱ ♠❛❣♥❡t♦✲♦s❝✐❧❧❛t✐♦♥s✱ ❛♥ ❞❡r ❛❛❧s ❤❡t❡r♦str✉❝t✉r❡s✱ t✉♥❣st❡♥ ❞✐s❡
❧❡♥✐❞❡✱ ❤❡①❛❣♦♥❛❧ ♦r♦♥ ♥✐tr✐❞❡✱ ❛❝❝❡♣t♦r
♥❡✇ st❡♣ ♦❢ ❝♦♠♣❧❡①✐t ❤❛s r❡❝❡♥t❧② ❡❡♥ ✉♥❞❡rt❛❦❡♥ ✐♥ t❤❡ ✜❡❧❞ ♦❢ t♦✲❞✐♠❡♥s✐♦♥❛❧
❝r②st❛❧s✱ ❞❡t❡r♠✐♥✐st✐❝❛❧❧② ♣❧❛❝✐♥❣ ❛t♦♠✐❝❛❧❧② t❤✐♥ ❧❛❡rs ♦❢ ❞✐✛❡r❡♥t ♠❛t❡r✐❛❧s ♦♥ t♦♣ ♦❢
❡❛❝ ♦t❤❡r✳ ❚❤❡ r❡s✉❧t✐♥❣ st❛❝❦s ❛r❡ r❡❢❡rr❡❞ t♦ ❛s ❛♥ ❞❡r ❛❛❧s ✭✈❞❲✮ ❤❡t❡r♦str✉❝t✉r❡s✳
✶✱✷
❇❛s❡❞ ♦♥ t❤✐s ✐❞❡❛✱ ❢❡✇ ♣r♦t♦t②♣ ❞❡✈✐❝❡s✱ s✉❝ ❛s t✉♥♥❡❧✐♥❣ tr❛♥s✐st♦rs
✸✕✶✶
❛♥❞✴♦r ❧✐❣❤t✲
❡♠✐tt✐♥❣ t✉♥♥❡❧✐♥❣ ❞✐♦❞❡s✱
✶✷✕✶✻
❤❛ ❡❡♥ ❢❛❜r✐❝❛t❡❞ ❛♥❞ s✉❝❝❡ss❢✉❧❧② t❡st❡❞✳ ❍♦❡✈❡r✱ ❢✉r✲
t❤❡r ♦r❦ ✐s ♥❡❝❡ss❛r② ✐♥ ♦r❞❡r t♦ ❡tt❡r ❤❛r❛❝t❡r✐③❡ s✉❝ str✉❝t✉r❡s✱ t♦ ❧❡❛r♥ ♠♦r❡ ❛❜♦✉t
t❤❡✐r ❡❧❡❝tr♦♥✐❝ ❛♥❞ ♦♣t✐❝❛❧ ♣r❡rt✐❡s✱ ✇✐t❤ t❤❡ ❛✐♠ t♦ ♣r♦♣❡r❧② ❞❡s✐❣♥ ❞❡✈✐❝❡ ♦♣❡r❛t✐♦♥✳
❍❡r❡✱ ✉♥❡✐ ♥❡✇ ❢❛❝❡ts ♦❢ ❧✐❣❤t ❡♠✐tt✐♥❣ ✈❞❲ ❤❡t❡r♦str✉❝t✉r❡s✱ ✇✐t❤ r❡❢❡r❡♥❝❡ t♦ t❤❡
✐ss✉❡ ♦❢ t❤❡ ❛❧✐❣♥♠❡♥t ♦❢ ❡❧❡❝tr♦♥✐❝ ❜❛♥❞s✱ ❡✛❡❝ts ♦❢ ❈♦✉❧♦♠ ✐♥t❡r❛❝t✐♦♥ ❛♥❞ s✉❜t❧❡ ❜✉t
st✐❧❧ ❛❝t✐✈ r♦❧❡ ♦❢ t❤❡ ❣r❛♣❤❡♥❡ ❡❧❡❝tr♦❞❡s ✐♥ t❤❡s❡ ❞❡✈✐❝❡s✳ r❡♣♦rt ♦♥ ♦♣t♦❡❧❡❝tr♦♥✐❝
♠❡❛s✉r❡♠❡♥ts ❡r❢♦r♠❡❞ ♦♥ ❲❙❡
2
✲❜❛s❡❞ t✉♥♥❡❧✐♥❣ ❧✐❣❤t✲❡♠✐tt✐♥❣ ❞✐♦❞❡✳ ❚❤❡ ❞✐✛❡r❡♥t✐❛❧
t✉♥♥❡❧✐♥❣ ♦♥❞✉❝t❛♥❝❡ ♦❢ ♦✉r str✉❝t✉r❡ s❤♦✇s ❧❛r❣❡ ③❡r♦ ❜✐❛s ❛♥♦♠❛❧② ✭♣❛❦✮✱ ✇❤✐❝
❛s❝r✐❜ t♦ ♣✐♥♥✐♥❣ ♦❢ t❤❡ ❡r♠✐ ❡♥❡r❣② ❛t t❤❡ ❲❙❡
2
✐♠♣✉r✐t②✴❛❝❝❡♣t♦r ❧❡❡❧✳ ❝♦♥❝❡✐✈❛❜❧❡
s❝❡♥❛r✐♦ ❢♦r t❤❡ ❡✈♦❧✉t✐♦♥ ♦❢ t❤❡ ❜❛♥❞ ❛❧✐❣♥♠❡♥t ❛s ❢✉♥❝t✐♦ ♦❢ t❤❡ ❜✐❛s ♦❧t❛❣❡ ✐s ♣r♦♣♦s❡❞✳

❙tr✐❦✐♥❣❧② t❤❡ ❜✐❛s✲♣♦t❡♥t✐❛❧ ♦♥s❡t ❢♦r t❤❡ ❡❧❡❝tr♦❧✉♠✐♥❡s❝❡♥❝❡ ✐s ❢♦✉♥❞ t♦ ❝♦✐♥❝✐❞❡ ✇✐t❤ t❤❡
❡♥❡r❣② ♦❢ t❤❡ ❢r❡❡ ❡①❝✐t♦♥ ♦❢ t❤❡ ❲❙❡
2
♠♦♥♦❧❛❡r ✭❛♥❞ ♥♦t t❤ t❤❡ ❡♥❡r❣② ♦❢ s✐♥❣❧❡✲♣❛rt✐❝❧❡
❜❛♥❞❣❛♣✮✳ ❚❤✐s ❢❛❝t ♦✐♥ts ♦✉t t❤❡ r❡❧❡✈❛♥t r♦❧❡ ♦❢ ❈♦✉❧♦♠ ✐♥t❡r❛❝t✐♦♥s ❡t❡❡♥ ❡❧❡❝tr✐❝❛❧❧②
✐♥❥❡❝t❡❞ ❝❛rr✐❡rs ♦♥ t❤❡ t✉♥♥❡❧✐♥❣ ♣r♦❝❡ss❡s ✐♥ ♦✉r ❞❡✈✐❝❡ ✉rt❤❡r♠♦r❡✱ ♣r♦♥♦✉♥❝❡❞ ♠❛❣♥❡t♦✲
♦s❝✐❧❧❛t✐♦♥s ❛r❡ ♦❜s❡r✈❡❞ ✐♥ t❤❡ ❡❧❡❝tr♦❧✉♠✐♥❡s❝❡♥❝❡ ❡♠✐ss✐♦♥ ✐♥t❡♥s✐t ♠❡❛s✉r❡❞ ❛s ❢✉♥❝t✐♦♥
♦❢ ♠❛❣♥❡t✐❝ ✜❡❧❞ ❛♣♣❧✐❡❞ ❡r♣❡♥❞✐❝✉❧❛r❧② t♦ t❤❡ ❧❛❡r ♣❧❛♥❡s✳ ❚❤❡s❡ ♦s❝✐❧❧❛t✐♦♥s✱ ❡r✐♦❞✐❝ ✇✐t❤
t❤❡ ✐♥❡rs❡ ♦❢ t❤❡ ♠❛❣♥❡t✐❝ ✜❡❧❞✱ r❡✢❡❝t t❤❡ ♠♦❞✉❧❛t✐♦♥ ♦❢ t❤❡ ❡✣❝✐❡♥❝② ♦❢ ❝❛rr✐❡r t✉♥♥❡❧✐♥❣
❛♥❞ ❛r❡ ❝❛✉s❡❞ t❤❡ ▲❛♥❞❛✉ q✉❛♥t✐③❛t✐♦♥ ♦❢ t❤❡ t♦✲❞✐♠❡♥s✐♦♥❛❧ ❣r❛♣❤❡♥❡ ❡❧❡❝tr♦❞❡s✳
st✉❞✐❡❞ ❧✐❣❤t✲❡♠✐tt✐♥❣ ❞✐♦❞❡ str✉❝t✉r❡
✶✷✱✶✸
t❤❛t ✐s ❜❛s❡❞ ♦♥ ❲❙❡
2
♠♦♥♦❧❛❡r ❛s
t❤❡ ❛❝t✐✈ ♣❛rt✳ ❚❤❡ ❧❛❡r s❡q✉❡♥❝❡ ❢♦r t❤✐s ❞❡✈✐❝❡ ❛s ❙✐ ❙✐❖
2
❤❇◆ ❣r❛♣❤❡♥❡ ❤❇◆
❲❙❡
2
❤❇◆ ❣r❛♣❤❡♥❡✳ ❚❤❡ ❡♠✐ss✐♦♥ ❛r❡❛ ♦❢ t❤❡ str✉❝t✉r❡ ✐s ♣r❡s❡♥t❡❞ ♦♥ t❤❡ ♠✐❝r♦s❝♦♣
✐♠❛❣❡ ✐♥ ❋✐❣✉r❡ ✭❛✮✳ ❋✐❣✉r❡ ✭❜✮ ❞❡♣✐❝ts s❝❤❡♠❛t✐❝ ❞r❛✇✐♥❣ ♦❢ t❤❡ ❡r❡❞ str✉❝t✉r❡✳
❚❤❡ t ❤❇◆ s♣❛❝❡rs t❤❛t s❡♣❛r❛t❡ t❤❡ ❲❙❡
2
♠♦♥♦❧❛❡r ❢r♦♠ t❤❡ ❣r❛♣❤❡♥❡ ❡❧❡❝tr♦❞❡s ❛r❡
t ❧❛❡rs t❤✐❝❦✳ ❞❡t❛✐❧❡❞ ❞❡s❝r✐♣t✐♦♥ ♦❢ t❤❡ ❢❛❜r✐❝❛t✐♦♥ ♣r♦❝❡ss ❛♥ ❢♦✉♥❞ ✐♥ ❢✳ ✶✷❪✳
❚❤❡ ♦♣t♦❡❧❡❝tr♦♥✐❝ ❤❛r❛❝t❡r✐st✐❝s ♦❢ t❤❡ s❛♠♣❧❡ ❡r❡ st✉❞✐❡❞ r❡❝♦r❞✐♥❣ t❤❡ ❡❧❡❝tr♦✲
❧✉♠✐♥❡s❝❡♥❝❡ ✭❊▲✮ s✐❣♥❛❧ ❛s ❢✉♥❝t✐♦♥ ♦❢ ❜✐❛s ♦❧t❛❣ ❛♥❞ ✐♥ ♠❛❣♥❡t✐❝ ✜❡❧❞s ✉♣ t♦ ✶✹ ❚✳
❈✉rr❡♥t✲✈♦❧t❛❣❡ ❝✉r✈❡s ❡r❡ ♠❡❛s✉r❡❞ t♦ st✉❞② t❤❡ t✉♥♥❡❧✐♥❣ ♣r♦❝❡ss❡s ❛♥❞ ♣❤♦t♦❧✉♠✐♥❡s✲
❝❡♥❝❡ ✭P▲✮ ♠❛♣♣✐♥❣ ♦❢ t❤❡ s❛♠♣❧❡ ❛s ❡r❢♦r♠❡❞ t♦ ❛❞❞✐t✐♦♥❛❧❧② ❤❛r❛❝t❡r✐③❡ t❤❡ str✉❝t✉r❡✳
❆❧❧ ♠❡❛s✉r❡♠❡♥ts ❡r❡ ❡r❢♦r♠❡❞ ✇✐t❤ ❛♥ ♦♣t✐❝❛❧✲✜❜r✲❜s ✐♥s❡rt ♣❧❛❝❡❞ ✐♥ s✉♣❡r❝♦♥✲
❞✉❝t✐♥❣ ❝♦✐❧✳ ❚❤ ✐♥❡st✐❣❛t❡❞ s❛♠♣❧❡ ❛s ❧♦❝❛t❡❞ ♦♥ t♦♣ ♦❢ ❛♥ ①✲②✲③ ♣✐❡③♦✲st❛❣❡ ❡♣t ✐♥
❤❡❧✐✉♠ ❣❛s ❛t
T = 4.2
❑✳ ❚❤❡ ❧❛s❡r ❧✐❣❤t ❢r♦♠ ♦♥t✐♥✉♦✉s ❆r✰ ❧❛s❡r
λ = 514.5
♥♠✮
❛s ❝♦✉♣❧❡❞ t♦ ❛♥ ❡①❝✐t❛t✐♦♥ ✜❜❡r ♦❢
5 µ
❞✐❛♠❡t❡r✱ ❢♦❝✉s❡❞ ♦♥ t❤❡ s❛♠♣❧❡ ❛♥ ❛s♣❤❡r✐❝
❧❡♥s✳ ❚❤❡ s✐❣♥❛❧ ❛s ❞❡t❡❝t❡❞ ✇✐t❤
50 µ
❝♦r❡ ✜❜❡r ♦❧❧❡❝t✐♦♥ s♣♦t ❞✐❛♠❡t❡r ♦❢
10 µ
♠✮
0.5
❧♦♥❣ ♠♦♥♦❤r♦♠❛t♦r ❡q✉✐♣♣❡❞ ✇✐t❤ ❤❛r❣❡✲❝♦✉♣❧❡✲❞❡✈✐❝❡ ✭❈❈❉✮ ❝❛♠❡r❛✳ ❊❧❡❝✲
tr✐❝❛❧ ♠❡❛s✉r❡♠❡ts ❡r❡ ❡r❢♦r♠❡❞ ✉s✐♥❣ ❑❡✐t❤❧❡② ✷✹✵✵ s♦✉r❝❡✲♠❡❛s✉r❡ ✉♥✐t✳
❡rt✐❝❛❧ ❝✉rr❡♥t ❛s ♦❜s❡r✈ ♦♥ t❤❡ ❛♣♣❧✐❝❛t✐♦♥ ♦❢ ❜✐❛s ♦❧t❛❣❡ ✭❱
b
❡t❡❡♥ t❤❡
t ❣r❛♣❤❡♥❡ ❡❧❡❝tr♦❞❡s✳ ❙✉❝ ❤❛r❣❡ tr❛♥s❢❡r ❢r♦♠ ♦♥❡ ❣r❛♣❤❡♥❡ ❧❛❡r t♦ t❤❡ ♦t❤❡r ❝❛♥

❋✐❣✉r❡ ✶✿ ❉❡✈✐❝❡ str✉❝t✉r❡ ❛♥❞ tr❛♥s♣♦rt ❤❛r❛❝t❡r✐st✐❝s✳ ✭❛✮ ▼✐❝r♦s❝♦♣ ✐♠❛❣❡ ♦❢ t❤❡ ❛❝t✐✈
♣❛rt ♦❢ t❤ s❛♠♣❧❡✳ ❚❤❡ ❜r♦✇♥ ❛r❡❛ ✐♥❞✐❝❛t❡s t❤❡ ♦s✐t✐♦♥ ♦❢ t❤❡ ❲❙❡
2
✢❛❦❡✳ ✭❜✮ ❙❝❤❡♠❛t✐❝
✐❧❧✉str❛t✐♦♥ ♦❢ t❤ ❤❡t❡r♦str✉❝t✉r❡ s❤♦✇♥ ✭❛✮✳ ❚❤ ❧❛❡r s❡q✉❡♥❝❡ ❢r♦♠ ♦tt♦♠ t♦ t♦♣ ✐s
❤❇◆✴❣r❛♣❤❡♥❡✴❤❇◆✴❲❙❡
2
✴❤❇◆✴❣r❛♣❤❡♥❡✳ ✭❝✮ ❉✐✛❡r❡♥t✐❛❧ ❝♦♥❞✉❝t❛♥❝❡
G = dI/dV
b
❚❤❡
❝♦❧♦r❡❞ r❡❣✐♦♥s ❝♦rr❡s♣♦♥❞ t♦ t❤❡ s✐t✉❛t✐♦♥ s❤♦✇♥ ✐♥ ✭❢ ❛♥❞ ✭❣✮✳ ✭❞✮ ■♥t❡❣r❛t❡ ❊▲ s✐❣♥❛❧ ✐♥
s♣❡❝tr r❛♥❣❡ ❢r♦♠
1.48
t♦
1.85
❛s ❢✉♥❝t✐♦♥ ♦❢ t❤❡ ❜✐❛s ♦❧t❛❣❡✳ ✭❡✮ ❙❝❤❡♠❛t✐❝ ❜❛♥❞
❞✐❛❣r❛♠ ❢♦r ③❡r♦ ❜✐❛s✳ ❚❤❡ r❡❞ ♣❛r❛❜♦❧✐ ❜❛♥❞s ♦rrs♣♦♥❞ t♦ t❤❡ ❑✲♣♦✐♥t ♦❢ t❤❡ ❇r✐❧❧♦✉✐♥
③♦♥❡ ✐♥ ❲❙❡
2
❚❤❡ ❤♦r✐③♦♥t❛❧ ❣r❡❡♥ ❧✐♥❡s ❞❡♣✐❝t ❞♦♥♦r✴❛❝❝❡♣t♦r✲❧✐❦ ❜❛♥❞s✳ ✭❢ ❙❝❤❡♠❛t✐❝
❜❛♥❞ ❞✐❛❣r❛♠ ❢♦r t❤❡ ❝❛s❡ ♦❢ ✐♥t❡r♠❡❞✐❛t❡ ❜✐❛s✳ ❍❡r❡ ❤♦❧❡s ❝❛♥ t✉♥♥❡❧ t❤r♦✉❣❤ t❤❡ ❤❇◆
❜❛rr✐❡r ✐♥t♦ ❙❡
2
❜✉t ❡❧❡❝tr♦♥s ❝❛♥ ♥♦t✳
h
❝♦rr❡s♣♦♥❞s t♦ t❤❡ ♦❧t❛❣❡ r❡q✉r❡❞ t♦ ✐♥❥❡❝t
❤♦❧❡s✳ ✭❣✮ ❇❛♥❞ ❞✐❛❣r❛♠ ♦r ❧❛r❣❡ ❜✐❛s✳ ■♥ t❤✐s ❝❛s❡✱ ♦t❤ ❤♦❧❡s ❛♥❞ ❡❧❡❝tr♦♥s ❝❛♥ t✉♥♥❡❧✳
e
st❛♥❞s ❢♦r t❤❡ ♦❧t❛❣❡ t❤r❡s❤♦❧❞ ♦r t❤❡ t✉♥♥❡❧✐♥❣ ♦❢ ❡❧❡❝tr♦♥s ✐♥t♦ ❡①❝✐t♦♥✐❝ st❛t❡s ♦❢
❲❙❡
2
❚❤❡ ❡①❝✐t♦♥ ✐s ❞❡♣✐❝t❡❞ s❝❤❡♠❛t✐❝❛❧❧② ■♥ t❤✐s r❡❣✐♠❡ ❧✐❣❤t ❡♠✐ss✐♦♥ ✐s ♦❜s❡r✈ ❞✉❡
t♦ ❡①❝✐t♦♥ r❡❝♦♠❜✐♥❛t✐♦♥ ✐♥ t❤❡ ❲❙❡
2
♠♦♥♦❧❛❡r✳
osc
✐♥❞✐❝❛t❡s t❤❡ ♦✛s❡t ❡①tr❛❝t❡❞ ❢r♦♠
❊q♥✳ ✷✳

Citations
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Journal ArticleDOI

2D Layered Material-Based van der Waals Heterostructures for Optoelectronics

TL;DR: In this article, the authors reviewed the state-of-the-art research activities that focus on the 2D van der Waals heterostructures and their optoelectronic applications.
Journal ArticleDOI

Flexible Molybdenum Disulfide (MoS2) Atomic Layers for Wearable Electronics and Optoelectronics

TL;DR: The overall recent progress made in developing MoS2 based flexible FETs, OLED displays, nonvolatile memory (NVM) devices, piezoelectric nanogenerators (PNGs), and sensors for wearable electronic and optoelectronic devices is discussed.
Journal ArticleDOI

The optical response of monolayer, few-layer and bulk tungsten disulfide

TL;DR: In this paper, a comprehensive optical study of thin flakes of tungsten disulfide (WS2) with thickness ranging from mono-to octalayer and in the bulk limit is presented, where the optical band-gap absorption of monolayer WS2 is governed by competing resonances arising from one neutral and two distinct negatively charged excitons whose contributions to the overall absorption of light vary as a function of temperature and carrier concentration.
Journal ArticleDOI

Van der Waals heterostructures for optoelectronics: Progress and prospects

TL;DR: In this article, van der Waals (vdW) heterostructures have offered considerable freedom to integrate various two dimensional (2D) layered materials and proved themselves extremely versatile with unprecedented characteristics, unique functionalities and novel physics.
References
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Journal ArticleDOI

Van der Waals heterostructures

TL;DR: With steady improvement in fabrication techniques and using graphene’s springboard, van der Waals heterostructures should develop into a large field of their own.
Journal ArticleDOI

2D materials and van der Waals heterostructures

TL;DR: Two-dimensional heterostructures with extended range of functionalities yields a range of possible applications, and spectrum reconstruction in graphene interacting with hBN allowed several groups to study the Hofstadter butterfly effect and topological currents in such a system.
Journal ArticleDOI

Vertical field-effect transistor based on graphene?WS2 heterostructures for flexible and transparent electronics

TL;DR: A new generation of field-effect vertical tunnelling transistors where two-dimensional tungsten disulphide serves as an atomically thin barrier between two layers of either mechanically exfoliated or chemical vapour deposition-grown graphene are described.
Journal ArticleDOI

High-performance single layered WSe₂ p-FETs with chemically doped contacts.

TL;DR: High performance p-type field-effect transistors based on single layered WSe(2) as the active channel with chemically doped source/drain contacts and high-κ gate dielectrics are reported.
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