Premium
Impact of the NO Anneal on the Microscopic Structure and Chemical Composition of the Si‐Face 4H‐SiC/SiO 2 Interface
Author(s) -
Gruber Gernot,
Gspan Christian,
Fisslthaler Evelin,
Dienstleder Martina,
Pobegen Gregor,
Aichinger Thomas,
Meszaros Robert,
Grogger Werner,
Hadley Peter
Publication year - 2018
Publication title -
advanced materials interfaces
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.671
H-Index - 65
ISSN - 2196-7350
DOI - 10.1002/admi.201800022
Subject(s) - materials science , passivation , oxide , transmission electron microscopy , mosfet , annealing (glass) , scanning transmission electron microscopy , analytical chemistry (journal) , crystallographic defect , silicon carbide , transistor , optoelectronics , condensed matter physics , nanotechnology , layer (electronics) , composite material , electrical engineering , metallurgy , engineering , voltage , chromatography , physics , chemistry
Understanding the microscopic structure of the SiC/SiO 2 interface is crucial for the improvement of SiC based metal‐oxide‐semiconductor field‐effect transistors (MOSFETs). It is well established that interface states degrade the performance and reliability of SiC MOSFETs and that passivation can be achieved by anneals in NO‐containing atmospheres. However, the structural changes associated with the NO anneal and the improvement of the channel electron mobility are still not fully understood. In this study, the SiC/SiO 2 interface of the state‐of‐the art 4H‐SiC n ‐channel MOSFETs with a deposited oxide is extensively investigated with advanced scanning transmission electron microscopy (STEM) and spatially resolved electron energy‐loss spectroscopy (EELS) methods. The samples are treated with different postoxidation anneals (NO vs O 2 ), resulting in strongly differing mobility and point defect density. The most notable structural difference between the samples is an increased N concentration located in the transition region between the SiC and the SiO 2 of the NO‐annealed sample. The N signal is evenly distributed along the whole faceted interface and has a half‐width of w N = (1.8 ± 0.7) nm and an estimated areal density of c N = (4 ± 1) × 10 14 cm −2 . The observations support the idea that the N incorporation happens predominantly directly at the SiC/SiO 2 interface where defect states are passivated.