_version_ 1866929435585806336
author Liu, Lun-Jun
Janssen, Reinier M. J.
Bumble, Bruce
Kane, Elijah
Foote, Logan M.
Bradford, Charles M.
Hailey-Dunsheath, Steven
Agrawal, Shubh
Aguirre, James E.
Athreya, Hrushi
Bracks, Justin S.
Brendal, Brockton S.
Corso, Anthony J.
Filippini, Jeffrey P.
Fu, Jianyang
Groppi, Christopher E.
Joralmon, Dylan
Keenan, Ryan P.
Kowalik, Mikolaj
Lowe, Ian N.
Manduca, Alex
Marrone, Daniel P.
Mauskopf, Philip D.
Mayer, Evan C.
Nie, Rong
Razavimaleki, Vesal
Saeid, Talia
Trumper, Isaac
Vieira, Joaquin D.
author_facet Liu, Lun-Jun
Janssen, Reinier M. J.
Bumble, Bruce
Kane, Elijah
Foote, Logan M.
Bradford, Charles M.
Hailey-Dunsheath, Steven
Agrawal, Shubh
Aguirre, James E.
Athreya, Hrushi
Bracks, Justin S.
Brendal, Brockton S.
Corso, Anthony J.
Filippini, Jeffrey P.
Fu, Jianyang
Groppi, Christopher E.
Joralmon, Dylan
Keenan, Ryan P.
Kowalik, Mikolaj
Lowe, Ian N.
Manduca, Alex
Marrone, Daniel P.
Mauskopf, Philip D.
Mayer, Evan C.
Nie, Rong
Razavimaleki, Vesal
Saeid, Talia
Trumper, Isaac
Vieira, Joaquin D.
contents We report on the effects of cosmic ray interactions with the Kinetic Inductance Detector (KID) based focal plane array for the Terahertz Intensity Mapper (TIM). TIM is a NASA-funded balloon-borne experiment designed to probe the peak of the star formation in the Universe. It employs two spectroscopic bands, each equipped with a focal plane of four $\sim\,$900-pixel, KID-based array chips. Measurements of an 864-pixel TIM array shows 791 resonators in a 0.5$\,$GHz bandwidth. We discuss challenges with resonator calibration caused by this high multiplexing density. We robustly identify the physical positions of 788 (99.6$\,$%) detectors using a custom LED-based identification scheme. Using this information we show that cosmic ray events occur at a rate of 2.1$\,\mathrm{events/min/cm^2}$ in our array. 66$\,$% of the events affect a single pixel, and another 33$\,$% affect $<\,$5 KIDs per event spread over a 0.66$\,\mathrm{cm^2}$ region (2 pixel pitches in radius). We observe a total cosmic ray dead fraction of 0.0011$\,$%, and predict that the maximum possible in-flight dead fraction is $\sim\,$0.165$\,$%, which demonstrates our design will be robust against these high-energy events.
format Preprint
id arxiv_https___arxiv_org_abs_2407_17381
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Cosmic ray susceptibility of the Terahertz Intensity Mapper detector arrays
Liu, Lun-Jun
Janssen, Reinier M. J.
Bumble, Bruce
Kane, Elijah
Foote, Logan M.
Bradford, Charles M.
Hailey-Dunsheath, Steven
Agrawal, Shubh
Aguirre, James E.
Athreya, Hrushi
Bracks, Justin S.
Brendal, Brockton S.
Corso, Anthony J.
Filippini, Jeffrey P.
Fu, Jianyang
Groppi, Christopher E.
Joralmon, Dylan
Keenan, Ryan P.
Kowalik, Mikolaj
Lowe, Ian N.
Manduca, Alex
Marrone, Daniel P.
Mauskopf, Philip D.
Mayer, Evan C.
Nie, Rong
Razavimaleki, Vesal
Saeid, Talia
Trumper, Isaac
Vieira, Joaquin D.
Instrumentation and Methods for Astrophysics
Applied Physics
Instrumentation and Detectors
We report on the effects of cosmic ray interactions with the Kinetic Inductance Detector (KID) based focal plane array for the Terahertz Intensity Mapper (TIM). TIM is a NASA-funded balloon-borne experiment designed to probe the peak of the star formation in the Universe. It employs two spectroscopic bands, each equipped with a focal plane of four $\sim\,$900-pixel, KID-based array chips. Measurements of an 864-pixel TIM array shows 791 resonators in a 0.5$\,$GHz bandwidth. We discuss challenges with resonator calibration caused by this high multiplexing density. We robustly identify the physical positions of 788 (99.6$\,$%) detectors using a custom LED-based identification scheme. Using this information we show that cosmic ray events occur at a rate of 2.1$\,\mathrm{events/min/cm^2}$ in our array. 66$\,$% of the events affect a single pixel, and another 33$\,$% affect $<\,$5 KIDs per event spread over a 0.66$\,\mathrm{cm^2}$ region (2 pixel pitches in radius). We observe a total cosmic ray dead fraction of 0.0011$\,$%, and predict that the maximum possible in-flight dead fraction is $\sim\,$0.165$\,$%, which demonstrates our design will be robust against these high-energy events.
title Cosmic ray susceptibility of the Terahertz Intensity Mapper detector arrays
topic Instrumentation and Methods for Astrophysics
Applied Physics
Instrumentation and Detectors
url https://arxiv.org/abs/2407.17381