4.8 Article

High Electric Field Carrier Transport and Power Dissipation in Multilayer Black Phosphorus Field Effect Transistor with Dielectric Engineering

Journal

ADVANCED FUNCTIONAL MATERIALS
Volume 27, Issue 4, Pages -

Publisher

WILEY-V C H VERLAG GMBH
DOI: 10.1002/adfm.201604025

Keywords

black phosphorus; hexagonal boron nitride; micro-Raman; power dissipation

Funding

  1. Ministry of Science, ICT & Future Planning via the National Research Foundation of Korea (NRF) [2016K1A1A2912707, 2013M3A6B1078873]
  2. ONR [N00014-13-1-0662, N00014-13-1-0464]
  3. [DE-SC0012592]
  4. National Research Foundation of Korea [2016K1A1A2912707, 2013M3A6B1078873] Funding Source: Korea Institute of Science & Technology Information (KISTI), National Science & Technology Information Service (NTIS)

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This study addresses high electric field transport in multilayer black phosphorus (BP) field effect transistors with self-heating and thermal spreading by dielectric engineering. Interestingly, a multilayer BP device on a SiO2 substrate exhibits a maximum current density of 3.3 x 10(10) A m(-2) at an electric field of 5.58 MV m(-1), several times higher than multilayer MoS2. The breakdown thermometry analysis reveals that self-heating is impeded along the BP-dielectric interface, resulting in a thermal plateau inside the channel and eventual Joule breakdown. Using a size-dependent electro-thermal transport model, an interfacial thermal conductance of 1-10 MW m(-2) K-1 is extracted for the BP-dielectric interfaces. By using hexagonal boron nitride (hBN) as a dielectric material for BP instead of thermally resistive SiO2 ( approximate to 1.4 W m(-1) K-1), a threefold increase in breakdown power density and a relatively higher electric field endurance is obtained together with efficient and homogenous thermal spreading because hBN has superior structural and thermal compatibility with BP. The authors further confirm the results based on micro-Raman spectroscopy and atomic force microscopy, and observe that BP devices on hBN exhibit centrally localized hotspots with a breakdown temperature of 600 K, while the BP devices on SiO2 exhibit hotspots in the vicinity of the electrode at 520 K.

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