Damage generation efficiency of protons and 60Co gammas in III–V infrared semiconductors

J J. V. Logan (Air Force Research Laboratory, Space Vehicles Directorate, Kirtland AFB 1 , New Mexico 87117,) M M. P. Short (Department of Nuclear Science and Engineering, Massachusetts Institute of Technology 2 , 77 Massachusetts Ave., Cambridge, Massachusetts 02139,) W W. L. Helms (Air Force Research Laboratory, Space Vehicles Directorate, Kirtland AFB 1 , New Mexico 87117,) A A. T. Newell (Air Force Research Laboratory, Space Vehicles Directorate, Kirtland AFB 1 , New Mexico 87117,) Z Z. M. Alsaad (Air Force Research Laboratory, Space Vehicles Directorate, Kirtland AFB 1 , New Mexico 87117,) R R. A. Carrasco (Air Force Research Laboratory, Space Vehicles Directorate, Kirtland AFB 1 , New Mexico 87117,) P P. T. Webster (Air Force Research Laboratory, Space Vehicles Directorate 2 , Kirtland AFB, New Mexico 87117,) D D. Maestas (Air Force Research Laboratory, Space Vehicles Directorate, Kirtland AFB 1 , New Mexico 87117,) C C. P. Morath (Air Force Research Laboratory, Space Vehicles Directorate, Kirtland AFB 1 , New Mexico 87117,)

Abstract

Radioisotope (60Co) and particle accelerator (10 s MeV proton) sources are both commonly used to assess the effects of the space radiation environment on electronics and detectors; however, the efficiency of 60Co gammas to generate displacement damage is poorly understood. Here, 60Co and 54.3 MeV proton degradation of the minority carrier lifetime are compared for an InAs/InAsSb superlattice and bulk InAsSb semiconductor infrared detector materials to assess the extent to which 60Co gammas generate displacement damage. It is found that, for equivalent nuclear energy deposition in each sample, the lifetime damage factor for 60Co irradiation is ∼14× higher than anticipated based on the lifetime damage factor from protons. This is explained by the difference in proton and 60Co gamma cascade sizes and dynamics (whereby protons generate large cascades and 60Co gamma-generated electrons generate only isolated Frenkel pairs). This difference drives the smaller damage factor for protons due to the enhanced defect recovery with larger cascades. This efficiency is an important factor to consider when analyzing electronic device performance following 60Co irradiation.

Article Details

Volume / Issue Vol. 139, Issue 12
Published March 28, 2026
ISSN 0021-8979
Publisher American Institute of Physics

Journal Info

Journal of Applied Physics

American Institute of Physics

ISSN: 0021-8979 Physical Sciences

Authors (9)

J

J. V. Logan

Air Force Research Laboratory, Space Vehicles Directorate, Kirtland AFB 1 , New Mexico 87117,

M

M. P. Short

Department of Nuclear Science and Engineering, Massachusetts Institute of Technology 2 , 77 Massachusetts Ave., Cambridge, Massachusetts 02139,

W

W. L. Helms

Air Force Research Laboratory, Space Vehicles Directorate, Kirtland AFB 1 , New Mexico 87117,

A

A. T. Newell

Air Force Research Laboratory, Space Vehicles Directorate, Kirtland AFB 1 , New Mexico 87117,

Z

Z. M. Alsaad

Air Force Research Laboratory, Space Vehicles Directorate, Kirtland AFB 1 , New Mexico 87117,

R

R. A. Carrasco

Air Force Research Laboratory, Space Vehicles Directorate, Kirtland AFB 1 , New Mexico 87117,

P

P. T. Webster

Air Force Research Laboratory, Space Vehicles Directorate 2 , Kirtland AFB, New Mexico 87117,

D

D. Maestas

Air Force Research Laboratory, Space Vehicles Directorate, Kirtland AFB 1 , New Mexico 87117,

C

C. P. Morath

Air Force Research Laboratory, Space Vehicles Directorate, Kirtland AFB 1 , New Mexico 87117,