crystals
Review
Mechanism of Electronegativity Heterojunction of Nanometer
Amorphous-Boron on Crystalline Silicon: An Overview
Paolo Sberna
1
, Piet X. Fang
2,3
, Changming Fang
4
and Stoyan Nihtianov
2,
*
Citation: Sberna,P.; Fang, P.X.; Fang,
C.; Nihtianov, S. Mechanism of
Electronegativity Heterojunction of
Nanometer Amorphous-Boron on
Crystalline Silicon: An Overview.
Crystals 2021, 11, 108.
https://doi.org/10.3390/cryst11020108
Academic Editor: Riccardo Camattari
Received: 30 November 2020
Accepted: 20 January 2021
Published: 26 January 2021
Publisher’s Note: MDPI stays neu-
tral with regard to jurisdictional claims
in published maps and institutional
affiliations.
Copyright: © 2021 by the authors. Li-
censee MDPI, Basel, Switzerland. This
article is an open access article distributed
under the terms and conditions of the
Creative Commons Attribution (CC BY)
license (https://creativecommons.org/
licenses/by/4.0/).
1
Else Kooi Laboratory, Faculty of Electrical Engineering, Mathematics and Computer Science, TU Delft,
Feldmannweg 17, 2628 CT Delft, The Netherlands; p.m.sberna@tudelft.nl
2
Electronic Instrumentation Lab, Faculty of Electrical Engineering, Mathematics and Computer Science,
TU Delft, Mekelweg 4, 2628 CD Delft, The Netherlands; Lele.fang@gmail.com
3
High Field Magnet Laboratory (HFML-EMFL), Radboud University, Toernooiveld 7,
6525 ED Nijmegen, The Netherlands
4
BCAST, Brunel University London, Uxbridge, Middlesex UB8 3PH, UK; Changming.Fang@brunel.ac.uk
* Correspondence: S.Nihtianov@tudelft.nl
Abstract: The discovery of the extremely shallow amorphous boron-crystalline silicon heterojunction
occurred during the development of highly sensitive, hard and robust detectors for low-penetration-
depth ionizing radiation, such as ultraviolet photons and low-energy electrons (below 1 keV). For
many years it was believed that the junction created by the chemical vapor deposition of amor-
phous boron on n-type crystalline silicon was a shallow p-n junction, although experimental results
could not provide evidence for such a conclusion. Only recently, quantum-mechanics based mod-
elling revealed the unique nature and the formation mechanism of this new junction. Here, we
review the initiation and the history of understanding the a-B/c-Si interface (henceforth called the
“boron-silicon junction”), as well as its importance for the microelectronics industry, followed by the
scientific perception of the new junctions. Future developments and possible research directions are
also discussed.
Keywords: rectifying junction; photodiode; chemical vapor deposition; first principle molecular
dynamics; electronegativity
1. Introduction: Initiation and History of Boron-Silicon Junctions and Importance of
Si-Based Junctions/Diodes in Microelectronics
The first report about an ultra-shallow rectifying junction (diode) created by a pure
boron atmospheric/low-pressure chemical vapor deposition (AP/LPCVD) on crystalline
n-type silicon surface was published in 2006 [1]. Initially, the application which led to
the development of this novel rectifying junction was: a linear and high Q-factor varactor
diode designed for the capacitance tuning of frequency in RF circuits [2,3]. The demon-
strated good performance in the varactor application did not attract the expected attention.
Fortunately, in 2006 it became clear that a different field of applications would benefit
even more from the excellent electrical properties of this extremely shallow junction. This
junction would prove useful as an accurate, stable and reliable detector for low-penetration
depth radiation such as UV light and low-energy electrons, which are applied in UV optical
lithography and scanning electron microscopes.
Since 2006 a significant amount of research has been completed in the following
directions: (1) optimization of the critical junction creation process, i.e., the chemical vapor
deposition (CVD) of amorphous boron on n-type crystalline silicon (in a method called
the “PureB” process); (2) device characterization and design optimization for a variety
of applications; and (3) rendering the PureB process CMOS-compatible. Initially it was
believed that the excellent electrical properties of the junction—especially the very low
saturation currents which are typical for deep p-n junctions—were defined by the p
+
Crystals 2021, 11, 108. https://doi.org/10.3390/cryst11020108 https://www.mdpi.com/journal/crystals