Asymmetric Doping‐Dependent Electron Transport Mobility in InxGa1–xAs/GaAs Quantum Well Field‐Effect Transistor Structure

Author:

Panda Sangita R.1ORCID,Pradhan Manoranjan1,Mallik Sandipan2,Sahu Trinath3

Affiliation:

1. Department of ECE Veer Surendra Sai University of Technology Burla 768018 Odisha India

2. Department of ECE NIST University Berhampur 761008 Odisha India

3. Centre of Excellence in Nano Science and Technology for the Development of Sensors Berhampur University Berhampur 760007 Odisha India

Abstract

We analyze the asymmetric doping‐dependent electron mobility μ of GaAs/InGaAs/GaAs quantum well field‐effect transistor (QWFET) structure. We consider doping concentrations, nd1 and nd2, in the substrate and surface barriers, respectively, and study μ as a function of nd2, taking (nd1 + nd2) unchanged. An increase in nd2 decreases nd1, yielding interesting changes in the occupation of subbands. For well width W < 164 Å, μ is due to single subband occupancy (SSO). Around W = 164 Å, there occurs first SSO, then double subband occupancy (DSO), and again SSO with an increase in nd2. Near the transition of subbands, abrupt discontinuities in μ arise due to inter‐subband effects. Thus, high to low and then high values of μ are obtained, displaying almost flat‐like variations, symmetric about |nd2 − nd1| =0. As W becomes wider, complete DSO occurs throughout the range of nd2 having reduced μ. Alternatively, keeping nd1 unchanged and by increasing nd2, μ raises due to enhanced N s , with a drop near the transition from SSO to DSO. Under SSO, μ is controlled by the ionized impurity and alloy disorder scatterings, while under DSO, the impurity scattering determines μ. Our analysis on μ can help to examine the inter‐subband effects on device characteristics of the QWFET system.

Publisher

Wiley

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