Abstract

We propose far-infrared photodetectors with the graphene nanoribbon (GNR) array as the photosensitive element and the black phosphorus (bP) base layer (BL). The operation of these GNR infrared photodetectors (GNR-IPs) is associated with the interband photogeneration of the electron–hole pairs in the GNR array followed by the tunneling injection of either electrons or holes into a wide gap bP BL. The GNR-IP operating principle is akin to that of the unitraveling-carrier photodiodes based on the standard semiconductors. Due to a narrow energy gap in the GNRs, the proposed GNR-IPs can operate in the far-, mid-, and near-infrared spectral ranges. The cut-off photon energy, which is specified by the GNR energy gap (i.e., is dictated by the GNR width), can be in the far-infrared range, being smaller that the energy gap of the bP BL of ΔG ≃ 300 meV. Using the developed device models of the GNR-IPs and the GNR-IP terahertz photomixers, we evaluate their characteristics and predict their potential performance. The speed of the GNR-IP response is determined by rather short times: the photocarrier try-to-escape time and the photocarrier transit time across the BL. Therefore, the GNR-IPs could operate as terahertz photomixers. The excitation of the plasma oscillations in the GNR array might result in a strong resonant photomixing.

Highlights

  • The quantization of the energy spectrum in the graphene nanoribbon (GNR) arrays, obtained by partitioning of the graphene layer (GL), results in the transformation of the two-dimensional gapless spectrum of the electrons and holes to the spectrum consisting of the sets of onedimensional subbands

  • We focus our analysis on the GNR infrared photodetectors (GNR-IPs) with the undoped GNR array sandwiched between the top cap layer (CL) doped by donors and the bP base layer (BL) doped by acceptors

  • We proposed and evaluated interband far-infrared photodetectors with the GNR array and the bP BL—GNR-IPs

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Summary

Introduction

The quantization of the energy spectrum in the graphene nanoribbon (GNR) arrays, obtained by partitioning of the graphene layer (GL), results in the transformation of the two-dimensional gapless spectrum of the electrons and holes to the spectrum consisting of the sets of onedimensional subbands. Such a choice of the device structure is associated with a relative smallness of the valence band off-set ΔV at the GNR/bP interface in comparison with the pertinent conduction band off-set ΔC. This implies that the IPs of the n-bP/GNR/p-bP/pþ-bP type can have smaller cut-off photon energy (in the far-infrared or even in the terahertz ranges) compared to the IPs of the p-bP∕GNR∕n-bP∕nþ-bP type. The situation is analogous to that in the unitraveling-carrier photodiodes

Main Equations
Spectral Characteristics of the GNR-IP Responsivity and Detectivity
Detection of Modulated Radiation
Plasmonic Response
Discussion
Conclusions
Steady-State Photocurrent
Photocurrent at Modulated Radiation
Plasmonic Oscillations in GNR Arrays
Fermi Energy in the GNR Array
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