<p>Arrays of field-effect mid-wave infrared (MWIR) photodetectors with an HgCdTe absorber and graphene channel were fabricated for room-temperature operation. The proposed device does not require cryogenic cooling for high detectivity, unlike most of the other MWIR photon photodetectors. The photodetectors showed a peak photocurrent of 254&#xa0;<i>µ</i>A at an excitation with 4&#xa0;<i>µ</i>m&#xa0;±&#xa0;40&#xa0;nm wavelength and 2.05&#xa0;mW/cm<sup>2</sup> incident power density. The detector shows a high signal-to-noise ratio of&#xa0;~&#xa0;200 to&#xa0;~&#xa0;1200 when coupled with a DC subtractor. The use of HfO<sub>2</sub> as gate dielectric increases the photocurrent by&#xa0;~&#xa0;15 times compared to Al<sub>2</sub>O<sub>3</sub>. The peak specific detectivity (D*) was 2.36&#xa0;×&#xa0;10<sup>10</sup> Jones when HfO<sub>2</sub> was used as the gate dielectric. A notable achievement of our work is obtaining the performance with a high doping density of&#xa0;~&#xa0;4.34&#xa0;×&#xa0;10<sup>14</sup>&#xa0;cm<sup>−3</sup> in HgCdTe.</p>

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Impact of Al2O3 and HfO2 Gate Dielectrics on Photoresponse of Graphene Channel Field-Effect MWIR Photodetectors with HgCdTe Absorber

  • Md Fazle Rabbe,
  • Volodymyr Sheremet,
  • M. A. H. Sojib,
  • Vitaliy Avrutin,
  • Ümit Ӧzgür,
  • Monica Allen,
  • Jeffery Allen,
  • Randy N. Jacobs,
  • Nibir K. Dhar

摘要

Arrays of field-effect mid-wave infrared (MWIR) photodetectors with an HgCdTe absorber and graphene channel were fabricated for room-temperature operation. The proposed device does not require cryogenic cooling for high detectivity, unlike most of the other MWIR photon photodetectors. The photodetectors showed a peak photocurrent of 254 µA at an excitation with 4 µm ± 40 nm wavelength and 2.05 mW/cm2 incident power density. The detector shows a high signal-to-noise ratio of ~ 200 to ~ 1200 when coupled with a DC subtractor. The use of HfO2 as gate dielectric increases the photocurrent by ~ 15 times compared to Al2O3. The peak specific detectivity (D*) was 2.36 × 1010 Jones when HfO2 was used as the gate dielectric. A notable achievement of our work is obtaining the performance with a high doping density of ~ 4.34 × 1014 cm−3 in HgCdTe.