High temperature superconducting (HTS) devices offer significant performance (higher
signal to noise ratio, sensitivity etc) improvement over conventional devices, becoming more
prominent when device dimensions are scaled down. A typical technology for the
fabrication of devices with very small critical dimensions is electron beam lithography. In
the current work, a detailed study of the electron beam lithography process is
presented using two simulation methods: one based on Monte Carlo simulation and
one based on the Boltzmann transport equation. Simulation energy deposition
results are compared with experimental ones in the case of Si and superconducting
substrates for the first time, with satisfactory agreement found. The experimental
data for statistical distributions of the scattered electrons were calculated in the
case of an epoxy based chemically amplified resist film deposited on Si and on
Y Ba2Cu3O7−δ/SrTiO3. The substrate strongly influences the distribution of the backscattered electrons due to the
different effective atomic number and the mass densities of the substrate and YBCO layer are
studied. It is shown that the decrease of the effective atomic numbers of the substrates (MgO and
SrTiO3
in comparison with YBCO) leads to an increase in the external proximity
effect obtained in regions far from the point of beam incidence on the resist
(2 µm for 25 keV
and 10–11 µm
for 75 keV in the case of MgO). On MgO and
SrTiO3
substrates the proximity effect is lower than on YBCO substrate (bulk YBCO) in regions
near to the point of beam incidence. Using simulation tools, accurate prediction of
final resist profiles (after development) over a wide exposure dose range of dense
sub-quarter-micron structures is performed for both Si and superconducting substrates.