• Rapid Communication

Rigid-band electronic structure of scandium nitride across the n-type to p-type carrier transition regime

Sanjay Nayak, Madhusmita Baral, Mukul Gupta, Jaspreet Singh, Magnus Garbrecht, Tapas Ganguli, S. M. Shivaprasad, and Bivas Saha
Phys. Rev. B 99, 161117(R) – Published 24 April 2019
PDFHTMLExport Citation

Abstract

Intentional doping and unintentional impurities in intrinsic semiconductors generate carriers that enable device operations. Fundamental to the electronic activity of dopants and impurities is the introduction of defect states inside the forbidden energy gap of semiconductors having shallow and/or deep characteristics, which fundamentally define the ability to engineer its physical properties and associated device performance. Here we demonstrate that unintentional electron doping by oxygen (ON) impurities and intentional magnesium hole doping (MgSc) in scandium nitride (ScN) do not introduce any defect states inside its fundamental bandgap and that the rigid-band electronic structure remains unchanged. Employing a combination of spectroscopic techniques as well as first-principles density functional theory analysis, we show that the ON and MgSc defect states in ScN are located inside the bands, which leaves behind the virgin ScN bandgap as well as the valence and conduction band edges that are important for electronic transport. The rigid-band electronic structure of ScN with respect to the electron and hole doping results in high electron and hole concentrations due to the free movement of Fermi level and results in tunable electronic and thermoelectric properties necessary for device applications.

  • Figure
  • Figure
  • Figure
  • Figure
  • Received 10 December 2018
  • Revised 21 February 2019

DOI:https://doi.org/10.1103/PhysRevB.99.161117

©2019 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Sanjay Nayak1,2, Madhusmita Baral3,4, Mukul Gupta5, Jaspreet Singh6, Magnus Garbrecht7, Tapas Ganguli3,4, S. M. Shivaprasad1,2, and Bivas Saha1,2,8,*

  • 1Chemistry and Physics of Materials Unit, Jawaharlal Nehru Centre for Advanced Scientific Research, Bangalore 560064, India
  • 2International Centre for Materials Science, Jawaharlal Nehru Centre for Advanced Scientific Research, Bangalore 560064, India
  • 3Raja Ramanna Centre for Advanced Technology, Indore 452013, India
  • 4Homi Bhabha National Institute, Training school complex, Anushakti Nagar, Mumbai 400094
  • 5UGC-DAE Consortium for Scientific Research, Khandwa Road, Indore-452017, India
  • 6Technical Physics Division, Bhabha atomic research Centre, Mumbai 400094
  • 7Australian Centre for Microscopy and Microanalysis, The University of Sydney, NSW 2006, Australia
  • 8School of Advanced Materials (SAMat), Jawaharlal Nehru Centre for Advanced Scientific Research, Bangalore 560064, India

  • *Author to whom correspondence should be addressed: bsaha@jncasr.ac.in; bivas.mat@gmail.com

Article Text (Subscription Required)

Click to Expand

Supplemental Material (Subscription Required)

Click to Expand

References (Subscription Required)

Click to Expand
Issue

Vol. 99, Iss. 16 — 15 April 2019

Reuse & Permissions
Access Options
Author publication services for translation and copyediting assistance advertisement

Authorization Required


×
×

Images

×

Sign up to receive regular email alerts from Physical Review B

Log In

Cancel
×

Search


Article Lookup

Paste a citation or DOI

Enter a citation
×