Modulation of I-V Characteristics in U-Shaped Armchair Graphene Nanoribbon-Based Tunnel Diode

Here, the transport characteristics of aU-shaped armchair graphene nanoribbon tunnel diode (AGNR-TD) are modulated by adopting a tight-binding model and non-equilibrium Green's function (NEGF) formalism. Initially, we examine a pristine AGNR (pAGNR) which exhibits ballistic current-voltage (I-V) characteristics. To convert ballistics nature to tunnel diode characteristic we considered U-shaped AGNR- TD by introducing a cut of depth (dc) at the upper edge of pAGNR. This pattern resulted in the formation of a single-barrier TD structure. As dc increases from 7.38 A to 22.14 A, negative differential resistance (NDR) is obtained with a peak-to-valley ratio (PVR) of 2.57. In addition, we analyzed the I- <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$V$</tex> nature and transmission probability by varying the potential barrier width (W<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">b</inf>). As W<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">b</inf> increases from 18.46 A to 35.5 A, the corresponding peak current decreases. However, the PVR value rises from 2.57 to 3.18 and the power consumption at the valley drops from 171 nW to 17 nW.

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Published
2024-11-30
DOI
https://doi.org/10.1109/edkcon62339.2024.10870627
Primary Topic
Graphene research and applications
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article
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article

Modulation of I-V Characteristics in U-Shaped Armchair Graphene Nanoribbon-Based Tunnel Diode

Madhusudan Mishra, Deepak Kumar Naik, N. K. Sahoo, A. K. Sahu et al.
Graphene research and applications
article

Modulation of I-V Characteristics in U-Shaped Armchair Graphene Nanoribbon-Based Tunnel Diode

Madhusudan Mishra, Deepak Kumar Naik, N. K. Sahoo, A. K. Sahu, Simran Patra
article en

Abstract

Here, the transport characteristics of aU-shaped armchair graphene nanoribbon tunnel diode (AGNR-TD) are modulated by adopting a tight-binding model and non-equilibrium Green's function (NEGF) formalism. Initially, we examine a pristine AGNR (pAGNR) which exhibits ballistic current-voltage (I-V) characteristics. To convert ballistics nature to tunnel diode characteristic we considered U-shaped AGNR- TD by introducing a cut of depth (dc) at the upper edge of pAGNR. This pattern resulted in the formation of a single-barrier TD structure. As dc increases from 7.38 A to 22.14 A, negative differential resistance (NDR) is obtained with a peak-to-valley ratio (PVR) of 2.57. In addition, we analyzed the I- <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$V$</tex> nature and transmission probability by varying the potential barrier width (W<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">b</inf>). As W<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">b</inf> increases from 18.46 A to 35.5 A, the corresponding peak current decreases. However, the PVR value rises from 2.57 to 3.18 and the power consumption at the valley drops from 171 nW to 17 nW.

Berhampur University (IN)
Openalex Percentile: Top 83%
Graphene research and applications
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