The Middle East Technical University Defocusing Beamline
(METU-DBL) is designed to deliver protons with selectable kinetic
energies between 15–30 MeV, and proton flux
between 106–1010 protons/cm2/s, on a
maximum 21.55 to 15.40 cm target region with a beam uniformity
within ±6%, in accordance with the ESA ESCC No. 25100
specification for single event effects (SEEs) tests in the low
energy range. The achieved high proton fluences, allow users to test
space-grade materials; electronic circuits, ASICs, FPGAs, optical
lenses, structural elements, and coating layers for LEO, GEO, and
interplanetary missions.
The total received dose on the Device-Under-Test (DUT) from
secondary particles created during proton-material interactions at
the first beam collimator and the beam dump never exceed 0.1% of
the dose from primary protons. The METU-DBL is equiped with several
measurement stations and services to the user teams. A secondary
measurement station in a rotating drum that can hold multiple
samples has been constructed next to the first collimator which
provides neutrons for transmission experiments. At the target
region, a robotic table is located, which provides mechanical and
electrical mounting points to the samples and allows multiple
samples to be tested in a row. A modular vacuum box can also be
attached on the robotic table for any test that may require a vacuum
environment. Power rails on the robotic table provide various
outputs for the DUT. For the data acquisition, high-speed networking
and a modular industrial PC are available at the target station. The
design of the METU-DBL control software enables test users to
integrate and optimize the data acquisition and controlling of the
DUT.
The beam properties at the target region are measured with the
diamond, Timepix3, and fiber scintillator detectors mounted on the
robotic table. With diamond and Timepix3 detectors, measurements are
taken from the five different points (center and the four corners)
of the test area to measure the proton flux and ensure that it is
uniform across the full test area. Fiber scintillators on both axes
(X and Y) scan the target area to cross-check the beam profile's
uniformity. Secondary doses during the irradiation are measured by a
Geiger-Müller tube sensitive to electrons and gammas above
0.1 MeV and by a neutron detector located at the entrance of the
R&D room. The room cools down relatively fast after any irradiation
(<1 hour).
Accurate linear energy deposition rates and absorbed doses on the
samples are calculated using MCNP6, FLUKA and Geant4 Monte Carlo
simulations. Alanine dosimetry measurements that are calibrated
against these simulations are also used to estimate the absorbed
dose on the sample.