Multi-Layer Palladium Diselenide as a Contact Material for Two-Dimensional Tungsten Diselenide Field-Effect Transistors

Tungsten diselenide (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>WSe</mi><mn>2</mn></msub></semantics></math></inline-formula>) has emerged as a prom...

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Main Authors: Gennadiy Murastov, Muhammad Awais Aslam, Simon Leitner, Vadym Tkachuk, Iva Plutnarová, Egon Pavlica, Raul D. Rodriguez, Zdenek Sofer, Aleksandar Matković
Format: Article
Language:English
Published: MDPI AG 2024-03-01
Series:Nanomaterials
Subjects:
Online Access:https://www.mdpi.com/2079-4991/14/5/481
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author Gennadiy Murastov
Muhammad Awais Aslam
Simon Leitner
Vadym Tkachuk
Iva Plutnarová
Egon Pavlica
Raul D. Rodriguez
Zdenek Sofer
Aleksandar Matković
author_facet Gennadiy Murastov
Muhammad Awais Aslam
Simon Leitner
Vadym Tkachuk
Iva Plutnarová
Egon Pavlica
Raul D. Rodriguez
Zdenek Sofer
Aleksandar Matković
author_sort Gennadiy Murastov
collection DOAJ
description Tungsten diselenide (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>WSe</mi><mn>2</mn></msub></semantics></math></inline-formula>) has emerged as a promising ambipolar semiconductor material for field-effect transistors (FETs) due to its unique electronic properties, including a sizeable band gap, high carrier mobility, and remarkable on–off ratio. However, engineering the contacts to <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>WSe</mi><mn>2</mn></msub></semantics></math></inline-formula> remains an issue, and high contact barriers prevent the utilization of the full performance in electronic applications. Furthermore, it could be possible to tune the contacts to <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>WSe</mi><mn>2</mn></msub></semantics></math></inline-formula> for effective electron or hole injection and consequently pin the threshold voltage to either conduction or valence band. This would be the way to achieve complementary metal–oxide–semiconductor devices without doping of the channel material.This study investigates the behaviour of two-dimensional <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>WSe</mi><mn>2</mn></msub></semantics></math></inline-formula> field-effect transistors with multi-layer palladium diselenide (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>PdSe</mi><mn>2</mn></msub></semantics></math></inline-formula>) as a contact material. We demonstrate that <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>PdSe</mi><mn>2</mn></msub></semantics></math></inline-formula> contacts favour hole injection while preserving the ambipolar nature of the channel material. This consequently yields high-performance <i>p</i>-type <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>WSe</mi><mn>2</mn></msub></semantics></math></inline-formula> devices with <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>PdSe</mi><mn>2</mn></msub></semantics></math></inline-formula> van der Waals contacts. Further, we explore the tunability of the contact interface by selective laser alteration of the <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>WSe</mi><mn>2</mn></msub></semantics></math></inline-formula> under the contacts, enabling pinning of the threshold voltage to the valence band of <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>WSe</mi><mn>2</mn></msub></semantics></math></inline-formula>, yielding pure <i>p</i>-type operation of the devices.
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spelling doaj.art-a5412c2b9c00426eb787281163681ad02024-03-12T16:51:45ZengMDPI AGNanomaterials2079-49912024-03-0114548110.3390/nano14050481Multi-Layer Palladium Diselenide as a Contact Material for Two-Dimensional Tungsten Diselenide Field-Effect TransistorsGennadiy Murastov0Muhammad Awais Aslam1Simon Leitner2Vadym Tkachuk3Iva Plutnarová4Egon Pavlica5Raul D. Rodriguez6Zdenek Sofer7Aleksandar Matković8Department Physics, Mechanics and Electrical Engineering, Montanuniversität Leoben, Franz Josef Strasse 18, 8700 Leoben, AustriaDepartment Physics, Mechanics and Electrical Engineering, Montanuniversität Leoben, Franz Josef Strasse 18, 8700 Leoben, AustriaDepartment Physics, Mechanics and Electrical Engineering, Montanuniversität Leoben, Franz Josef Strasse 18, 8700 Leoben, AustriaLaboratory of Organic Matter Physics, University of Nova Gorica, Vipavska 13, SI-5000 Nova Gorica, SloveniaDepartment of Inorganic Chemistry, University of Chemistry and Technology Prague, Technická 5, 166 28 Prague, Czech RepublicLaboratory of Organic Matter Physics, University of Nova Gorica, Vipavska 13, SI-5000 Nova Gorica, SloveniaResearch School of Chemistry & Applied Biomedical Sciences, Tomsk Polytechnic University, Lenina ave. 30, 634034 Tomsk, RussiaDepartment of Inorganic Chemistry, University of Chemistry and Technology Prague, Technická 5, 166 28 Prague, Czech RepublicDepartment Physics, Mechanics and Electrical Engineering, Montanuniversität Leoben, Franz Josef Strasse 18, 8700 Leoben, AustriaTungsten diselenide (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>WSe</mi><mn>2</mn></msub></semantics></math></inline-formula>) has emerged as a promising ambipolar semiconductor material for field-effect transistors (FETs) due to its unique electronic properties, including a sizeable band gap, high carrier mobility, and remarkable on–off ratio. However, engineering the contacts to <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>WSe</mi><mn>2</mn></msub></semantics></math></inline-formula> remains an issue, and high contact barriers prevent the utilization of the full performance in electronic applications. Furthermore, it could be possible to tune the contacts to <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>WSe</mi><mn>2</mn></msub></semantics></math></inline-formula> for effective electron or hole injection and consequently pin the threshold voltage to either conduction or valence band. This would be the way to achieve complementary metal–oxide–semiconductor devices without doping of the channel material.This study investigates the behaviour of two-dimensional <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>WSe</mi><mn>2</mn></msub></semantics></math></inline-formula> field-effect transistors with multi-layer palladium diselenide (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>PdSe</mi><mn>2</mn></msub></semantics></math></inline-formula>) as a contact material. We demonstrate that <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>PdSe</mi><mn>2</mn></msub></semantics></math></inline-formula> contacts favour hole injection while preserving the ambipolar nature of the channel material. This consequently yields high-performance <i>p</i>-type <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>WSe</mi><mn>2</mn></msub></semantics></math></inline-formula> devices with <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>PdSe</mi><mn>2</mn></msub></semantics></math></inline-formula> van der Waals contacts. Further, we explore the tunability of the contact interface by selective laser alteration of the <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>WSe</mi><mn>2</mn></msub></semantics></math></inline-formula> under the contacts, enabling pinning of the threshold voltage to the valence band of <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>WSe</mi><mn>2</mn></msub></semantics></math></inline-formula>, yielding pure <i>p</i>-type operation of the devices.https://www.mdpi.com/2079-4991/14/5/481palladium diselenidetungsten diselenidetungsten selenium oxidesemi-metallaser treatmentcontact engineering
spellingShingle Gennadiy Murastov
Muhammad Awais Aslam
Simon Leitner
Vadym Tkachuk
Iva Plutnarová
Egon Pavlica
Raul D. Rodriguez
Zdenek Sofer
Aleksandar Matković
Multi-Layer Palladium Diselenide as a Contact Material for Two-Dimensional Tungsten Diselenide Field-Effect Transistors
Nanomaterials
palladium diselenide
tungsten diselenide
tungsten selenium oxide
semi-metal
laser treatment
contact engineering
title Multi-Layer Palladium Diselenide as a Contact Material for Two-Dimensional Tungsten Diselenide Field-Effect Transistors
title_full Multi-Layer Palladium Diselenide as a Contact Material for Two-Dimensional Tungsten Diselenide Field-Effect Transistors
title_fullStr Multi-Layer Palladium Diselenide as a Contact Material for Two-Dimensional Tungsten Diselenide Field-Effect Transistors
title_full_unstemmed Multi-Layer Palladium Diselenide as a Contact Material for Two-Dimensional Tungsten Diselenide Field-Effect Transistors
title_short Multi-Layer Palladium Diselenide as a Contact Material for Two-Dimensional Tungsten Diselenide Field-Effect Transistors
title_sort multi layer palladium diselenide as a contact material for two dimensional tungsten diselenide field effect transistors
topic palladium diselenide
tungsten diselenide
tungsten selenium oxide
semi-metal
laser treatment
contact engineering
url https://www.mdpi.com/2079-4991/14/5/481
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