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Figure 6.19 Parameter γ in the size growth equation (6.86) as a function of a (6.85) [41, 43].
Let us represent the balance equation for the average cluster size n in the coagula-
tion process analogously to (6.70) in the form
dn
dt D γ
k 0 N sat ( T ) n 2/3
.
(6.86)
The values of
γ
depending on a and defined by (6.85) are given in Figure 6.19 [41,
43].
6.3.4
Cluster Growth in a Hot Gas with Metal-Containing Molecules
In considering the cluster plasma, we will be guided by a plasma consisting of a
buffer gas with metal clusters. A high number density of bound atoms in metal
clusters is realized in the case if a liquid metal-containing compound is inserted
in a flow of a dense plasma. This method of cluster generation in a buffer gas
allows us to obtain an effective source of light [128-131] and is used for prepara-
tion of films of heat-resistant metals as a result of transport of metal clusters and
their deposition onto a surface. So, we consider the scheme of cluster generation if
metal-containing molecules are injected into a hot gas or plasma and are converted
into a gas of metal clusters. The best case for this is if metal-containing molecules
contain halogen atoms, that is, these molecules are MX k ,where M is a metal atom
and X is a halogen atom.
We first find the conditions under which decomposition of metal-containing
molecules in a plasma leads to cluster formation, that is, the process of cluster
generation follows the scheme
MX k
!
M
C
kX , M
C
M n 1
!
M n ,
(6.87)
and in a low-temperature region halogen atoms join to form X 2 molecules. The
equilibrium between components of process (6.87) is described by the scheme
k
2 X 2
M
C
!
MX k
 
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