Bandgap Engineering of Nitrogen‐Doped Monolayer WSe <sub>2</sub> Superlattice and its Application to Field Effect Transistor

ABSTRACT We systematically investigate the electronic structures of pristine monolayer WSe 2 and WSe 2 superlattices with periodic nitrogen substitution. Unlike random doping, which often introduces in‐gap impurity states, periodic nitrogen doping primarily modulates the bandgap, thereby facilitating effective bandgap engineering for electronic and optoelectronic applications. The gap narrows monotonically with increasing dopant density (pristine 8‐row 6‐row 4‐row), directly influencing device switching. We also evaluate the FET performance of nanojunctions created by these configurations by examining the contour plot of current density as a function of temperature and gate voltage, which quantifies how bandgap engineering affects switching characteristics. Our calculations clarify the classical‐quantum crossover in sub‐10 nm 2D FETs: as rises, approaches the thermionic current; as falls, quantum tunneling dominates, and the steep energy dependence of may break the classical limit of subthreshold swing imposed by the Boltzmann tyranny. The optimal gating range (, ) is investigated for each temperature, insensitive to temperature in the high‐temperature regime, confirming the good thermal stability of the FET devices. A comparison study demonstrates that the 4‐row structure, with excessively large , severely low ON/OFF ratio, and restricted operation range, is inappropriate for realistic FET applications. The pristine structure has the highest performance across all measures, but its high (1.1 V) makes it less practical, since such a large threshold voltage may promote time‐dependent dielectric breakdown (TDDB) of the oxide layer, reducing device dependability. The 6‐row and 8‐row structures are slightly inferior to the pristine in terms of performance, but exhibit more favorable values (0.75 V), achieving a balance between reasonable threshold voltage and stable operation range, making them more promising candidates for future FET integration.

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Publication Details

Journal
Advanced Electronic Materials
Published
2026-02-15
DOI
https://doi.org/10.1002/aelm.202500754
Primary Topic
2D Materials and Applications
Type
article
Field-Weighted Citation Impact
0.00

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article

Bandgap Engineering of Nitrogen‐Doped Monolayer WSe 2 Superlattice and its Application to Field Effect Transistor

Yew-Chiong Lo, Yu‐Chang Chen, Likun Wang
Advanced Electronic Materials
2D Materials and Applications
article

Bandgap Engineering of Nitrogen‐Doped Monolayer WSe 2 Superlattice and its Application to Field Effect Transistor

Yew-Chiong Lo, Yu‐Chang Chen, Likun Wang
article en

Abstract

ABSTRACT We systematically investigate the electronic structures of pristine monolayer WSe 2 and WSe 2 superlattices with periodic nitrogen substitution. Unlike random doping, which often introduces in‐gap impurity states, periodic nitrogen doping primarily modulates the bandgap, thereby facilitating effective bandgap engineering for electronic and optoelectronic applications. The gap narrows monotonically with increasing dopant density (pristine 8‐row 6‐row 4‐row), directly influencing device switching. We also evaluate the FET performance of nanojunctions created by these configurations by examining the contour plot of current density as a function of temperature and gate voltage, which quantifies how bandgap engineering affects switching characteristics. Our calculations clarify the classical‐quantum crossover in sub‐10 nm 2D FETs: as rises, approaches the thermionic current; as falls, quantum tunneling dominates, and the steep energy dependence of may break the classical limit of subthreshold swing imposed by the Boltzmann tyranny. The optimal gating range (, ) is investigated for each temperature, insensitive to temperature in the high‐temperature regime, confirming the good thermal stability of the FET devices. A comparison study demonstrates that the 4‐row structure, with excessively large , severely low ON/OFF ratio, and restricted operation range, is inappropriate for realistic FET applications. The pristine structure has the highest performance across all measures, but its high (1.1 V) makes it less practical, since such a large threshold voltage may promote time‐dependent dielectric breakdown (TDDB) of the oxide layer, reducing device dependability. The 6‐row and 8‐row structures are slightly inferior to the pristine in terms of performance, but exhibit more favorable values (0.75 V), achieving a balance between reasonable threshold voltage and stable operation range, making them more promising candidates for future FET integration.

Advanced Electronic MaterialsVol. 12(5)
National Yang Ming Chiao Tung University (TW)
National Center for Theoretical Sciences, Ministry of Education, India, Ministry of Science and Technology, Taiwan, National Science and Technology Council
Openalex Percentile: Top 100%
2D Materials and Applications
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