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Copyright © 2014 American Scientific Publishers
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Article
Journal of
Nanoscience and Nanotechnology
Vol. 14, 7954–7960, 2014
www.aspbs.com/jnn
Initial Surface Reaction of Di-Isopropylaminosilane
on a Fully Hydroxyl-Terminated Si (001) Surface
Jin-Hoon Yang, Seung-Bin Baek, and Yeong-Cheol Kim
∗
School of Energy, Materials, and Chemical Engineering, Korea University of Technology and Education,
Cheonan, Chungnam 330-708, Republic of Korea
We studied the interaction of di-isopropylaminosilane (SiH
3
N(C
3
H
7
2
, DIPAS) molecules with a fully
hydroxyl-terminated Si (001) surface for SiO
2
thin-film growth by using density functional theory. The
amino group consisting of DIPAS was chosen in order to obtain a high adsorption energy because
its lone-pair electrons in the N atom would help in the adsorption of DIPAS. The absolute value of
the adsorption energy (0.67 eV) of DIPAS was higher than its reaction energy barrier of 0.38 eV.
Thus, DIPAS could react with the surface without desorption. The reaction between DIPAS and the
surface produced a silyl group (–SiH
3
) as a primary product and di-isopropylamine (NH(C
3
H
7
2
,
DIPA) as a by-product. A second DIPAS, which was adsorbed near the pre-adsorbed DIPAS or
–SiH
3
with DIPA, required higher reaction energy barriers of 3.91 or 1.92 eV, respectively, because
of its interaction with the first DIPAS or DIPA. However, when the second DIPAS was adsorbed near
–SiH
3
without DIPA, a low reaction energy barrier of 0.42 eV was required, indicating a negligible
effect of –SiH
3
on the second DIPAS reaction. Therefore, to obtain a highly dense Si layer, DIPA
must desorb from the surface. DIPA requires a relatively high desorption energy of 0.40 eV because
the lone-pair electrons in the N atom of DIPA also enhance its adsorption on the surface. The high
desorption energy could reduce the process window of atomic layer deposition.
Keywords: Atomic Layer Deposition, Di-Isopropylaminosilane, Initial Surface Reaction, Molecule
Interaction, Density Functional Theory.
1. INTRODUCTION
In recent years, SiO
2
has received renewed attention
as a gate spacer and gap-fill oxide in shallow trench
isolation.
1 2
However, due to the miniaturization and inte-
gration of semiconductor circuits, the thin SiO
2
films fab-
ricated by conventional deposition processes have many
problems when they are used for the above applications:
unexpected dopant diffusion at high temperatures, diffi-
cult film thickness controllability, and poor film quality.
3 4
Atomic layer deposition (ALD) is an alternative chemi-
cal vapor deposition-like method, and it has recently come
to the fore among semiconductor fabrication processes.
Thanks to its self-limiting and sequential surface reactions,
ALD film formation controls the film thickness layer-by-
layer on an atomic scale. Moreover, the films formed
by ALD provide excellent uniformity and step coverage
over the entire surface.
5 6
Various silicon precursors, as
ALD sources for the deposition of SiO
2
films, have been
∗
Author to whom correspondence should be addressed.
investigated in the quest to obtain high-quality films at low
operation temperatures.
Among these silicon precursors, organoaminosilane pre-
cursors have received a great deal of attention because of
their catalyst-free reactions and noncorrosive by-product
characteristics.
7 8
Due to the lone-pair electrons of the N
atoms in the precursors, the precursors could be strongly
attracted to the hydroxyl (-OH)-terminated Si surface.
The resulting high adsorption energy could weaken the
bond strengths between the atoms of the precursors, result-
ing in the decrease of the reaction energy barriers between
the precursors and the surface.
9
The by-products contain-
ing the N atom, however, would be hard to desorb due to
the strong attraction with the surface. Therefore, for the
optimization of the ALD precursors, it would be necessary
to study the effect of the N atoms in the precursors on
adsorption and desorption.
Lim et al. experimentally investigated the SiO
2
film using tetrakis-dimethylaminosilane (Si[N(CH
3
2
4
,
TeDMAS).
10
The film deposited below 250
C showed
a low dielectric constant and a leakage current. Won
7954 J. Nanosci. Nanotechnol. 2014, Vol. 14, No. 10 1533-4880/2014/14/7954/007 doi:10.1166/jnn.2014.9474