172
Journal of Non-Crystalline Solids 114 (1989) 172-174 North-Holland
P R E P A R A T I O N
J.Hanna*,
OF
A.Kamo,
Si
T H I N
T.Komiya,
F I L M S
BY
I.Shimizu
S P O N T A N E O U S
C H E M I C A L
D E P O S I T I O N
and H . K o k a d o *
T o k y o I n s t i t u t e of T e c h n o l o g y , I m a g i n g S c i e n c e a n d E n g i n e e r i n g Lab.* a n d G r a d u a t e S c h o o l at N a g a t s u t a , N a g a t s u t a , M i d o r i - k u Y o k o h a m a 227 J A P A N
We
have
proposed
a
novel
p r e p a r a t i o n t e c h n i q u e f o r Si t h i n f i l m s t e r m e d f e a t u r i n g the s p o n t a n e o u s r e a c t i o n s of s i l a n e w i t h f l u o r i n e at the r e d u c e d p r e s s u r e . Fluorine contributed not o n l y i n t o the gas p h a s e r e a c t i o n s so as to a f f o r d f l u o r i n a t e d p r e c u r s o r s , SiHnF, but also into the chemical processes on the growing surface, resulting in promoting the propagation of S i - n e t w o r k s in the films. T h u s t h i s t e c h n i q u e p r o v i d e d us a v a r i e t y of the f i l m s f r o m "amorphous" to '~ingle c r y s t a l l i n e " u n d e r a w i d e c h o i c e of the r e a c t i o n c o n d i t i o n s . The films exhibited rather high photoconductivity in spite of high d e p o s i t i o n r a t e s o v e r i0 A / s e c .
"Spontaneous Chemical Deposition",
I.INTRODUCTION
Little progress, however, has been achieved in
Nowadays thin films of hydrogenated a-Si
by
the o t h e r
problems.
It w o u l d
seem
to be
rf-glow discharge of SiH~ have been established
attributed to a lack of the external parameters
as a large-area electronic material, applied to
for controlling the chemical processes on the
solar cells, electrophotographic drums, TFT
growing surface in the SiH4 plasma process,
arrays for liquid crystal displays and so on.
except the substrate temperature.
Some of the properties in the films, have remained
to be i m p r o v e d
advanced performances in these
however,
for f u r t h e r devices. These
Our attention to a chemical process in the film growth from fluorinated materials,
where
the propagation of Si-network
via a
include a stability to light illumination, hole
chemical
transport characteristics and conductivity
fluorine,
the doped films,
in addition
in
interaction lead
us
proceeds
between to
hydrogen
a new
and
preparation
to a dilemma
technique for Si thin films termed Hydrogen
between the film quality and deposition rates.
Radical Enhanced CVD (HR-CVD). 4) This technique
Much attention has been paid to an enhancement
is featured by "an intentional control" of the
of a rigidity of Si-network in the films for
chemical process in the film growth with an aid
the improvements, because these poor properties
of atomic hydrogen.
are
deeply
concerned
structure of Si-network
with
the
inferior
in the films.
Under the same concept of
"the intentional
control'~ we have developed a novel method for
Great efforts have been made toward the
the films, featured by a non-plasma and purely
improvements in the approaches focused mainly
chemical process based on the
on understanding the chemical processes in the
of SiH4 in the gas phase.
We will describe the
film
general
new
g r o w t h I),2)
and
establishing
a new
preparation technique. 3),4) Indeed, it has been
features of the
fluoro-oxidation
method
termed
"Spontaneous Chemical Deposition'~
demonstrated that application of the magnetic field and the low pressure helps a consistency between
high
deposition
rates
and
the
quality.5), 6)
0022-3093/89/$03.50 © Elsevier Science Publishers B.V. (North-Holland)
2.EXPERIMENT The e x p e r i m e n t a l elsewhere. 7 )
setup
is i l l u s t r a t e d
173
J. Hanna et al. / Preparation of Si thin films by spontaneous chemical deposition
The reactor consisted of a pyrex glass tube,
substrate
distance,
a substrate holder and a gas nozzle for mixing
condition
of
SiH4 and F2, as is illustrated in Fig.l,
dsub.=40mm, and Press.=550mtorr the deposition
and
was hacked by mechanical booster and rotary
dsub..
In a t y p i c a l
SiH4(30sccm),
F2(30sccm),
rate was 12 A/sec.
pumps. Pure silane and fluorine diluted with He
The chemical structure of the films were
down to 10 vol% were used as the raw materials,
easily controlled by the external parameters in
Which
were
introduced
separately.
The
into
substrate
the
monitored by a thermocouple a t t a c h e d substrate
directly.
A
nozzle
temperature,Ts
typical
the gas phase reaction such as the pressure and
was
the ratio of the reactants: the SiHn stretching
to the
mode at 2000cm -I of the it-spectra tended to be
preparation
dominant when either
SiHd/F~
ratio
or
the
condition was similar to that in the rf-glow
pressure
discharge of SiHd.
The substrate temperature
3.RESULTS AND DISCUSSIONS
affect deeply npt only the chemical structures
was
decreased. found
to be more
effective parameter for the control
SiH,
reacted
with
Fz
spontaneously,
but also Si-network structures
and
to
in the films.
when these gasses were mixed through the nozzle
We found a very interesting
at the
reduced pressure similar to that in the
temperature on deposition rates and structures
plasma CVD. The reaction was e x o t h e r m i c and
of the films. Fig.2 shows deposition rates as a
accompanied
function of the substrate temperature.
by
an
intense
blue
chemi-
effects
of the
luminescence mainly from SiF*(420-480nm), as is shown in the photograph of Fig.l.
Substrate holder Nozzle
15
Press. = 5 2 0 - 5 5 0 r e t o r t Substrate Position =
40mm
SiH4:F2 =
S i H4
1:1
ov
r
-0l
,
150
200
L
, _l.
,
300
J
400
500
SubstrateTemp. (o C ) FIGURE 2 Deposition rate as a function temperature FIGURE 1 Schematic diagram of the reactor and photograph of the chemi-luminescence
As
the
temperature
was
crystallization took place The deposition rate was increased as the
of substrate
increased,
the
(filled circles in
Fig.2) and then the deposition rates went down
and d e c r e a s e d
rapidly. Both of the critical temperatures for
exponentially with an increase in the nozzle-
the crystallization and the film d e p o s i t i o n
SiH4 flow rate was increased,
J. Hanna et M./Preparation of Si thin films by spontaneous chemical deposition
174
tended to be shifted down as the gas flow ratio
phase reaction such as a gas flow ratio of SiH4
was d e c r e a s e d .
to F2 and the pressure the Si-network structure
These
facts
suggest
that
fluorine takes part in the chemical processes
in the films can be controlled intentionally.
on the growing
Thus this technique provides us a variety of
surface
so as
to promote
the
The films show high photoconductivity, ~ / r product of 10-Tcm2/V,
films from '~morphous" to "single crystalline" in e p i t a x i a l m a n n e r at low
the
propagation of Si-networks.
not only in the intrinsic
substrate temperature.
a-Si films but also in the ~c-Si films in spite
The experimental observations suggest that fluorine contributes into the chemical process
of high deposition rates over 10 A/sec. We observed the epitaxial growth of Si thin
on
the
growing
surface
directly
so
as
to
were
promote the propagation of Si-network and lead
applied as a substrate at the growth condition
to a long range relaxation of the Si-network at
for pc-Si films on the glass substrate,
the low temperature.
films at 300-400°C
when
e-Si
clearly seen in the photographs
wafers
as is
of the RHEED REFERENCES
patterns from the films. Ts=300°C
i.A.Matsuda and 2 (1987) 14~
Ts=370oC
K.Tanaka,
Mat.Sci.Rep.,
2. R.Robertson and A.Gallagher, J.Chem.Phys., 85 (1986) 3623. 3. T.L.Chu, S.S.Chu, E.G.Bylander, and S.T.Ang, Appl.Phys.Lett., 52 (1988) 807.
i
4. J.Hanna,
FIGURE 3 RHEED patterns from Si thin films prepared at 300°C and 3700C on c-Si(100) 4. CONCLUSIONS We have
established
a new
preparation
technique for Si thin films termed "Spontaneous
Chemical Deposition", which purely
chemical
reactions
process
of s i l a n e
is
of the
with
based
on
a
spontaneous
fluorine
at the
reduced pressure. With
the external
parameters
in the gas
N.Shibata, K.Fukuda, H.Ohtoshi, S.0da, and I.Shimizu, Disordered Semiconductors (Plenum Press, New York, 1987) p435.
5. T.Watanabe, M.Tanaka, K.Azuma, M.Nakatani, T.Sonobe, T.Shimada, Jpn.J.Appl.Phys., 26 (1987) 1215. 6. M.Ohnishi, H.Nishikawa, K.Uchihashi, K.Yoshida, M.Tanaka, K.Ninomiya, M.Nishikuni, N.Nakamura, S.Tsuda, S.Nakano, T.Yazaki, and Y.Kuwano, Jpn.J.Appl.Phys., 27 (1988) 40. 7. J.Hanna, A.Kamo, T.Komiya, H.D.Nguyen, I.Shimizu and H.Kokado, Mat.Res.Soc.Symp. Proc., (1989) in press.