Sammendrag
Detectors with high radiation tolerance and high time resolution are required for charged particle
in high physics and space applications.
3D detectors were introduced by S. Parker 1 in the middle 90’ and they represented a starting point
for evolved device able to work at fluency up to 2 × 10^16 neq/cm2. A limit to 3D detector is the not
uniformity of electrical field that translates in a not uniform charge collection efficiency after high
radiation doses and an uneven timing for the signal.
Different solution has been proposed in the last decade (eg. Hexagonal geometry of the electrodes)
but many TCAD device simulations suggest parallel trenches as best solution [2]. Two different geometries have been taken into consideration both with parallel trenches. The distance between
trenches of opposite sign is 25 µm in both case and the distance between trenches with equal sign
is fixed to 50 µm. The main difference is trenches length that is respectively of 100 µm and 50 µm.
They have been designed and fabricated by SINTEF MiNaLab, Oslo, Norway on SI-SI, high resistivity,
float zone substrates (6−12 kΩ cm) with an active thickness of 100 µm.
The neutron irradiation of the sensors has been carried out at the TRIGA Mark II reactor at JSI
(Ljubljana, Slovenia) in May 2018 and the characterization was performed afterwards.
The functional characterization has been performed by using a position resolved laser and by using
a setup designed for this type of measurements.
The radiation source is a pulsed laser with a wavelength of 1064 nm that allow a quasi-uniform
release of charge in the silicon substrate and a nominal pulse of 40ps. The laser source is integrated
in a microscope optics that can be moved in the 3 axes with a precision on the micrometer range.
In additional, the detectors are located in a vacuum chamber that avoid problems related to the
humidity/hoarfrost when the detectors works at low temperature. The detector is connected by
using two tungsten micro-needles connected to the readout circuits.
The results are two-dimensional maps of the signal across the 3D single basic cell. The measure has
been repeated for different voltages and temperature.
The data are then normalized to the signals acquired on non-irradiated samples.
At the conference we will report on the device design and technology, as well as on selected results
from the electrical and functional characterization.
[1] S. I. Parker et al., ”3D-A proposed new architecture for solid-state
radiation detectors”, Nucl. Instrum. Methods A, vol. 395, pp. 328-343,
1997.
[2] R. Mendicino, et al. “3D trenched-electrode sensors for charged particle tracking and timing.”
Nucl. Instrum. Methods A 2019.
in high physics and space applications.
3D detectors were introduced by S. Parker 1 in the middle 90’ and they represented a starting point
for evolved device able to work at fluency up to 2 × 10^16 neq/cm2. A limit to 3D detector is the not
uniformity of electrical field that translates in a not uniform charge collection efficiency after high
radiation doses and an uneven timing for the signal.
Different solution has been proposed in the last decade (eg. Hexagonal geometry of the electrodes)
but many TCAD device simulations suggest parallel trenches as best solution [2]. Two different geometries have been taken into consideration both with parallel trenches. The distance between
trenches of opposite sign is 25 µm in both case and the distance between trenches with equal sign
is fixed to 50 µm. The main difference is trenches length that is respectively of 100 µm and 50 µm.
They have been designed and fabricated by SINTEF MiNaLab, Oslo, Norway on SI-SI, high resistivity,
float zone substrates (6−12 kΩ cm) with an active thickness of 100 µm.
The neutron irradiation of the sensors has been carried out at the TRIGA Mark II reactor at JSI
(Ljubljana, Slovenia) in May 2018 and the characterization was performed afterwards.
The functional characterization has been performed by using a position resolved laser and by using
a setup designed for this type of measurements.
The radiation source is a pulsed laser with a wavelength of 1064 nm that allow a quasi-uniform
release of charge in the silicon substrate and a nominal pulse of 40ps. The laser source is integrated
in a microscope optics that can be moved in the 3 axes with a precision on the micrometer range.
In additional, the detectors are located in a vacuum chamber that avoid problems related to the
humidity/hoarfrost when the detectors works at low temperature. The detector is connected by
using two tungsten micro-needles connected to the readout circuits.
The results are two-dimensional maps of the signal across the 3D single basic cell. The measure has
been repeated for different voltages and temperature.
The data are then normalized to the signals acquired on non-irradiated samples.
At the conference we will report on the device design and technology, as well as on selected results
from the electrical and functional characterization.
[1] S. I. Parker et al., ”3D-A proposed new architecture for solid-state
radiation detectors”, Nucl. Instrum. Methods A, vol. 395, pp. 328-343,
1997.
[2] R. Mendicino, et al. “3D trenched-electrode sensors for charged particle tracking and timing.”
Nucl. Instrum. Methods A 2019.