TY - JOUR
T1 - Thin dead-layer avalanche photodiodes enable low-energy ion measurements
AU - Ogasawara, K.
AU - Livi, S. A.
AU - Grotheer, E.
AU - McComas, D. J.
N1 - Funding Information:
This work was supported by Southwest Research Institute's internal research and development (IR&D) program R9684 (ion-beam development), R9755 (APD development) and R8016 (data analysis).
Copyright:
Copyright 2010 Elsevier B.V., All rights reserved.
PY - 2010/3/1
Y1 - 2010/3/1
N2 - As an alternative method for detecting low-energy ions, we describe the performance of a thin dead-layer avalanche photodiode (APD, Hamamatsu spl 6815), which provides high-resolution, proportional, and reliable efficiency with low mass and power even at room temperature. The pulse height distribution of the APD signal shows a significant peak for energies above 2.5 keV for protons and 3.4 keV for helium ions, with a noise level of ∼ 300 electrons (1.1 keV in silicon diode detectors). The response linearity is excellent for light ions, including protons and helium ions, with some non-linearity for heavier ions. The energy resolutions are 15% for 58 keV protons, 16% for 56 keV helium ions, 43% for 55 keV nitrogen ions and 46% for 55 keV argon ions. We also measured the thickness of a dead layer by analyzing the energy defect of 57 keV protons with different angles from the device surface, revealing a dead layer as thin as 340 Å. Considering the whole active-layer thickness of approximately 150 μ m, the maximum detectable energy was calculated to be ∼ 4 MeV / n for protons and helium ions.
AB - As an alternative method for detecting low-energy ions, we describe the performance of a thin dead-layer avalanche photodiode (APD, Hamamatsu spl 6815), which provides high-resolution, proportional, and reliable efficiency with low mass and power even at room temperature. The pulse height distribution of the APD signal shows a significant peak for energies above 2.5 keV for protons and 3.4 keV for helium ions, with a noise level of ∼ 300 electrons (1.1 keV in silicon diode detectors). The response linearity is excellent for light ions, including protons and helium ions, with some non-linearity for heavier ions. The energy resolutions are 15% for 58 keV protons, 16% for 56 keV helium ions, 43% for 55 keV nitrogen ions and 46% for 55 keV argon ions. We also measured the thickness of a dead layer by analyzing the energy defect of 57 keV protons with different angles from the device surface, revealing a dead layer as thin as 340 Å. Considering the whole active-layer thickness of approximately 150 μ m, the maximum detectable energy was calculated to be ∼ 4 MeV / n for protons and helium ions.
KW - Avalanche photodiodes
KW - Particle detectors
KW - Solid-state detectors
KW - Space instrumentation
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U2 - 10.1016/j.nima.2009.12.044
DO - 10.1016/j.nima.2009.12.044
M3 - Article
AN - SCOPUS:76749153277
SN - 0168-9002
VL - 614
SP - 271
EP - 277
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
IS - 2
ER -