Description of the dialog box's model parameters
Energy, equals
The secondary electron yield δts has its maximum at the dialog box parameter Energy for normal incident primary electrons.
If an electron
hits the surface with an angle of θ0, the secondary electron
yield δts
will have its maximum at:
SEY, equals
The maximum for the secondary electron yield δts equals the dialog box parameter SEY for normal incident primary electrons.
If an
electron hits the surface with an angle of θ0, the maximum of
the secondary electron yield δts is:
s
The dialog
box parameter s changes the increase
and decrease of the secondary electron yield δts, but the maximum
of δts
is not dependent of s .
Advanced: Model for true secondary electrons
The probability
distribution function (PDF) for the true secondary electrons can be written
as follows:
Here, P is the normalized
incomplete gamma function. The parameters pn and εn are coupled to the
material you choose in the material dialog tab and can also be changed
by the user.
To avoid
the problem that some probabilities can become negative, a modified secondary
electron yield is defined:
In our secondary emission model the probability for the true secondary
electrons is a binomial distribution, where M
is the maximum number of secondary electrons per incident electron and:
See also
Secondary Electron Emission Overview
Material Parameters: default - Secondary Electron Emission
Material Parameters: default - SEE Import
Material Parameters: default - SEE Vaughan
Material Parameters: default - SEE Furman True
Material Parameters: default - SEE Furman Elastic
Material Parameters: default - SEE Furman Rediffused