|
|
|
|
|
Resist
Modeling Process
|
|
|
Photoresist modeling
and simulation requires knowledge of the exposure and
dissolution properties of a resist and the
characteristics of the exposure tool. The sequence
steps in the simulation are shown in Figure 6.
Exposure modeling involves the calculation of the
laser image intensity as a function of position (I(x)).
The propagation of that intensity function into the
photoresist is described by Beer's law and requires
knowledge of the real and complex index of refraction
(n and k) of the resist and substrate. An increment of
dose is applied at the film surface. The energy
deposited (# of photons) in any volume element E(x,z)
is then calculated from the knowledge of the resist
and substrate n, k. The energy is allowed to react
with the PAC to convert a proportion of it to a
photoproduct and to create a local relative PAC
concentration in the film, m(x,z). This process is
continued until a prescribed exposure dose is
accumulated. The interference of light due to
reflections at the resist-substrate interface creates
an oscillation in the exposure energy and thus creates
an oscillation in the PAC concentration. The PAC is
then "diffused" by a baking process to
create a final PAC concentration distribution m'(x,y,z).
Knowledge of the dissolution rate as a function of PAC
concentration (R(m)) then allows the simulation to
remove volume elements at the appropriate rate to
simulate the dissolution and thereby generate a resist
profile. |
|
|
|
|
|
|
|
|
Last
updated Monday, February 14, 2000
© 2000 Photomask Lithography, Willson Research
Group,
University of Texas at Austin
Phone: 512.471.6364
Email:
rathsack@mail.utexas.edu
Site design by Arrion Smith
|
|
|
|
|
|
|
|
|
|
|
|