TY - JOUR
T1 - Processing of n+/p-/p+ strip detectors with atomic layer deposition (ALD) grown Al2O3 field insulator on magnetic Czochralski silicon (MCz-si) substrates
AU - Härkönen, J.
AU - Tuovinen, Esa
AU - Luukka, P.
AU - Gädda, A.
AU - Mäenpää, T.
AU - Tuominen, E.
AU - Arsenovich, T.
AU - Junkes, A.
AU - Wu, X.
AU - Li, Z.
PY - 2016
Y1 - 2016
N2 - Detectors manufactured on p-type silicon material are
known to have significant advantages in very harsh
radiation environment over n-type detectors,
traditionally used in High Energy Physics experiments for
particle tracking. In p-type (n+ segmentation on p
substrate) position-sensitive strip detectors, however,
the fixed oxide charge in the silicon dioxide is positive
and, thus, causes electron accumulation at the Si/SiO2
interface. As a result, unless appropriate interstrip
isolation is applied, the n-type strips are
short-circuited. Widely adopted methods to terminate
surface electron accumulation are segmented p-stop or
p-spray field implantations. A different approach to
overcome the near-surface electron accumulation at the
interface of silicon dioxide and p-type silicon is to
deposit a thin film field insulator with negative oxide
charge. We have processed silicon strip detectors on
p-type Magnetic Czochralski silicon (MCz-Si) substrates
with aluminum oxide (Al2O3) thin film insulator, grown
with Atomic Layer Deposition (ALD) method. The electrical
characterization by current-voltage and
capacitance-voltage measurement shows reliable
performance of the aluminum oxide. The final proof of
concept was obtained at the test beam with 200 GeV/c
muons. For the non-irradiated detector the charge
collection efficiency (CCE) was nearly 100% with a
signal-to-noise ratio (S/N) of about 40, whereas for the
2*1015 neq/cm2 proton irradiated detector the CCE was
35%, when the sensor was biased at 500 V. These results
are comparable with the results from p-type detectors
with the p-spray and p-stop interstrip isolation
techniques. In addition, interestingly, when the aluminum
oxide was irradiated with Co-60 gamma-rays, an
accumulation of negative fixed oxide charge in the oxide
was observed.
AB - Detectors manufactured on p-type silicon material are
known to have significant advantages in very harsh
radiation environment over n-type detectors,
traditionally used in High Energy Physics experiments for
particle tracking. In p-type (n+ segmentation on p
substrate) position-sensitive strip detectors, however,
the fixed oxide charge in the silicon dioxide is positive
and, thus, causes electron accumulation at the Si/SiO2
interface. As a result, unless appropriate interstrip
isolation is applied, the n-type strips are
short-circuited. Widely adopted methods to terminate
surface electron accumulation are segmented p-stop or
p-spray field implantations. A different approach to
overcome the near-surface electron accumulation at the
interface of silicon dioxide and p-type silicon is to
deposit a thin film field insulator with negative oxide
charge. We have processed silicon strip detectors on
p-type Magnetic Czochralski silicon (MCz-Si) substrates
with aluminum oxide (Al2O3) thin film insulator, grown
with Atomic Layer Deposition (ALD) method. The electrical
characterization by current-voltage and
capacitance-voltage measurement shows reliable
performance of the aluminum oxide. The final proof of
concept was obtained at the test beam with 200 GeV/c
muons. For the non-irradiated detector the charge
collection efficiency (CCE) was nearly 100% with a
signal-to-noise ratio (S/N) of about 40, whereas for the
2*1015 neq/cm2 proton irradiated detector the CCE was
35%, when the sensor was biased at 500 V. These results
are comparable with the results from p-type detectors
with the p-spray and p-stop interstrip isolation
techniques. In addition, interestingly, when the aluminum
oxide was irradiated with Co-60 gamma-rays, an
accumulation of negative fixed oxide charge in the oxide
was observed.
KW - strip sensor
KW - MCz-Si
KW - ALD
KW - N on p
U2 - 10.1016/j.nima.2016.04.069
DO - 10.1016/j.nima.2016.04.069
M3 - Article
SN - 0168-9002
VL - 828
SP - 46
EP - 51
JO - Nuclear Instruments and Methods in Physics Research. Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
JF - Nuclear Instruments and Methods in Physics Research. Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
ER -