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Photolytic Carbon Deposition by IR-Multiphoton Dissociation of Molecules
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Photolytic Carbon Deposition by IR-Multiphoton Dissociation of Molecules
Photolytic Carbon Deposition by IR-Multiphoton Dissociation of Molecules
Specm~chmrco Actu. Vol. GA. Printed m &cat Britam Photolytic U. Central , One pulses. by the lie have we have dical of by power equilibr...
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Specm~chmrco Actu. Vol. GA. Printed m &cat Britam
Photolytic
U.
Central
,
One pulses.
by
the
lie
have
we have dical
of
by
power
equilibrium. not
the
carbon with
carbon
the
GOR,
way
usual
one
to
of
a IlaCl
try re-
intense
the
IR-multipho-
Assuming
order
can
materials
produced
in
to
thermal
by by
may
rise
solid-state
molecules
of
pulses
this
molecules.
conditions
laser give
deposition
concentration
experimental
of
which
by of
of
hydrogen
the
Sciences
In
available
deposition
the
different
high
reactants
decomposition
investigated
the
the
are
is
Academy
that
carbon
the
radicals,
achieve
a high
ra-
concentration.
our
experiments
TEA-CO2 length
laser of
C3h4) cus. The ments
9 cm.
the
The
were
cell
cence
signal,
length
516
after
which
can
Ue report
the
optimum
molecules
and
show,
tion
is
are
of
the
lecule can
for
C2H4 an be
achieved
by
an
so-called
sticking-effect. laser
strate room
focus
solid
photolytic
effect
carbon carbon
temperature.
of
be
in the
films The
the
are
distance
near
for
tuo
an
and
for
225
centre
at
the
of
the
radical
and
the
wave-
on
to
the
For to
different the
the
g. laser
0.9 the
J mo-
a factor
5
fre-
basis
of
of
investigated e.
of
upto
C3H4.
surface
IJe have
precursor concentra-
up with
substrates, the
of
energies
fields
it.
fo-
measure-
fluores-
each
C2H5C1
parallel on
or
laser
spontaneous
concentration
laser
C2H5Cl the
concentration
optimum laser
of
focus
band).
qualitatively
different between
the
C2 radicals
applied
case
deposited on
of
for
C2 radical by
relative
Swan
The the
C2H4,
the
absorption
CO2 laser
understood
directed
deposition
g., the
multimode with
in
infrared
means
pressure
yield
excitation can
is
of
gas
2 . . . 3 kPa.
enlargement
This
the
of
the
a high
quencies.
e. of
wavelengths
order
sufficient
by
by
observed,
lens
molecules
The
monitored
a line-tunable
dissociation
estimated
transition
that
precursor
irradiation.
be
of
means
IR-multiphoton
was
was
(0,O)
radiation by
the
by
laser
radicals
nm (the
the cell
contains
yield
and
carbon
focused
reaction
decomposed
dissociation
before
produced
b,e have into
which
If
thermal
Molecules
Freudenberg
species
which
example
increases
optimized
the
phases
of
6
of
unimolecular
of rate
T.
Chaussee
molecular
from
product
dissociation
deposition
of
Dissociation
Spectroscopy,
distributions
interes,ting
substrates
ton
and
and
Rudower
far
novel
IR-Multiphoton
Albrecht
Optics
state
reactions
ubtain
laser
H.
excitation
nonthermal
actions.
In
of
by
Berlin-Adlershof,
chemical
on
t-I. Hohmann,
selective
create
0SRC853Y~87 $3.00+0.00 ~ergamon Journals Ltd
lY87
Deposition
Institute
LIDR-1199
to
2. pp 225-226.
Carbon
Radloff
The
No
the
a subthe
NaCl
or
focus
Si, and
at the
226
etal.
W.RADLOFF
surface
of
the substrate
homogeneous
carbon
was about
films
0.8
mm. We obtained
in a reproducible
way.
relatively
The elemental
shown only spurious impurities. By the method of electron fuse diffraction fringes were obtained with lattice plane are
typical
for
The deposition meter.
rate
identical
experimental
0.6
of
about
modification
was derived
We have compared
of
larger
the carbon
the
conditions.
J at the optimum wavelength 0.1
A per pulse.
whereas
for
sures
the deposition
leads
to a rapid
rate
was less increases
deposition
measurements
the different
At a pressure we obtained
The deposition
CJH4 it
carbon
for
diffraction distances
and has
difwhich
hard-amorphous.
from thickness
rates
clean analysis
rate
of for
for
in comparison but the strong on the cell
precursor 0.8
with
a profilo-
molecules
at
kPa and an energy
C2H4 a deposition
rate
C2H5C1 was 2 . . . 3 times to C2H4. At higher homogeneous
windows.
pres-
nucleation
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