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Cosmic Ray Susceptibility of the Terahertz Intensity Mapper Detector Arrays
by
Aguirre, James E.
, Trumper, Isaac
, Bradford, Charles M.
, Corso, Anthony J.
, Janssen, Reinier M. J.
, Joralmon, Dylan
, Agrawal, Shubh
, Lowe, Ian N.
, Keenan, Ryan P.
, Filippini, Jeffrey P.
, Mayer, Evan C.
, Bracks, Justin S.
, Bumble, Bruce
, Foote, Logan M.
, Vieira, Joaquin D.
, Liu, Lun-Jun
, Manduca, Alex
, Fu, Jianyang
, Saeid, Talia
, Athreya, Hrushi
, Razavimaleki, Vesal
, Kane, Elijah
, Mauskopf, Philip D.
, Marrone, Daniel P.
, Brendal, Brockton S.
, Dunsheath, Steven Hailey
, Kowalik, Mikolaj
, Groppi, Christopher E.
, Nie, Rong
in
Aluminum
/ Arrays
/ Balloon-borne experiments
/ Calibration
/ Characterization and Evaluation of Materials
/ Condensed Matter Physics
/ Cosmic rays
/ Design
/ Focal plane devices
/ Inductance
/ Magnetic Materials
/ Magnetism
/ Multiplexing
/ Physics
/ Physics and Astronomy
/ Pixels
/ Radiation
/ Resonators
/ Sensors
/ Star & galaxy formation
/ Star formation
2024
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Cosmic Ray Susceptibility of the Terahertz Intensity Mapper Detector Arrays
by
Aguirre, James E.
, Trumper, Isaac
, Bradford, Charles M.
, Corso, Anthony J.
, Janssen, Reinier M. J.
, Joralmon, Dylan
, Agrawal, Shubh
, Lowe, Ian N.
, Keenan, Ryan P.
, Filippini, Jeffrey P.
, Mayer, Evan C.
, Bracks, Justin S.
, Bumble, Bruce
, Foote, Logan M.
, Vieira, Joaquin D.
, Liu, Lun-Jun
, Manduca, Alex
, Fu, Jianyang
, Saeid, Talia
, Athreya, Hrushi
, Razavimaleki, Vesal
, Kane, Elijah
, Mauskopf, Philip D.
, Marrone, Daniel P.
, Brendal, Brockton S.
, Dunsheath, Steven Hailey
, Kowalik, Mikolaj
, Groppi, Christopher E.
, Nie, Rong
in
Aluminum
/ Arrays
/ Balloon-borne experiments
/ Calibration
/ Characterization and Evaluation of Materials
/ Condensed Matter Physics
/ Cosmic rays
/ Design
/ Focal plane devices
/ Inductance
/ Magnetic Materials
/ Magnetism
/ Multiplexing
/ Physics
/ Physics and Astronomy
/ Pixels
/ Radiation
/ Resonators
/ Sensors
/ Star & galaxy formation
/ Star formation
2024
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Cosmic Ray Susceptibility of the Terahertz Intensity Mapper Detector Arrays
by
Aguirre, James E.
, Trumper, Isaac
, Bradford, Charles M.
, Corso, Anthony J.
, Janssen, Reinier M. J.
, Joralmon, Dylan
, Agrawal, Shubh
, Lowe, Ian N.
, Keenan, Ryan P.
, Filippini, Jeffrey P.
, Mayer, Evan C.
, Bracks, Justin S.
, Bumble, Bruce
, Foote, Logan M.
, Vieira, Joaquin D.
, Liu, Lun-Jun
, Manduca, Alex
, Fu, Jianyang
, Saeid, Talia
, Athreya, Hrushi
, Razavimaleki, Vesal
, Kane, Elijah
, Mauskopf, Philip D.
, Marrone, Daniel P.
, Brendal, Brockton S.
, Dunsheath, Steven Hailey
, Kowalik, Mikolaj
, Groppi, Christopher E.
, Nie, Rong
in
Aluminum
/ Arrays
/ Balloon-borne experiments
/ Calibration
/ Characterization and Evaluation of Materials
/ Condensed Matter Physics
/ Cosmic rays
/ Design
/ Focal plane devices
/ Inductance
/ Magnetic Materials
/ Magnetism
/ Multiplexing
/ Physics
/ Physics and Astronomy
/ Pixels
/ Radiation
/ Resonators
/ Sensors
/ Star & galaxy formation
/ Star formation
2024
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Cosmic Ray Susceptibility of the Terahertz Intensity Mapper Detector Arrays
Journal Article
Cosmic Ray Susceptibility of the Terahertz Intensity Mapper Detector Arrays
2024
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Overview
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
∼
900-pixel, KID-based array chips. Measurements of an 864-pixel TIM array show 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
events
/
min
/
cm
2
in our array. 66 % of the events affect a single pixel, and other 33 % affect
<
5 KIDs per event spread over a 0.66
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
∼
0.124 %, which demonstrates our design will be robust against these high-energy events.
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