Design and testing of Kinetic Inductance Detector package for the Terahertz Intensity Mapper
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| Autores principales: | , , , , , , , , , , , , , , , , , , |
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2022
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| author | Liu, L. -J. Janssen, R. M. J Bradford, C. M. Hailey-Dunsheath, S. Filippini, J. P. Aguirre, J. E. Bracks, J. S. Corso, A. J. Fu, J. Groppi, C. Hoh, J. Keenan, R. P. Lowe, I. N. Marrone, D. P. Mauskopf, P. Nie, R. Redford, J. Trumper, I. Vieira, J. D. |
| author_facet | Liu, L. -J. Janssen, R. M. J Bradford, C. M. Hailey-Dunsheath, S. Filippini, J. P. Aguirre, J. E. Bracks, J. S. Corso, A. J. Fu, J. Groppi, C. Hoh, J. Keenan, R. P. Lowe, I. N. Marrone, D. P. Mauskopf, P. Nie, R. Redford, J. Trumper, I. Vieira, J. D. |
| contents | The Terahertz Intensity Mapper (TIM) is designed to probe the star formation history in dust-obscured star-forming galaxies around the peak of cosmic star formation. This will be done via measurements of the redshifted 157.7 um line of singly ionized carbon ([CII]). TIM employs two R $\sim 250$ long-slit grating spectrometers covering 240-420 um. Each is equipped with a focal plane unit containing 4 wafer-sized subarrays of horn-coupled aluminum kinetic inductance detectors (KIDs). We present the design and performance of a prototype focal plane assembly for one of TIM's KID-based subarrays. Our design strictly maintain high optical efficiency and a suitable electromagnetic environment for the KIDs. The prototype detector housing in combination with the first flight-like quadrant are tested at 250 mK. Initial frequency scan shows that many resonances are affected by collisions and/or very shallow transmission dips as a result of a degraded internal quality factor (Q factor). This is attributed to the presence of an external magnetic field during cooldown. We report on a study of magnetic field dependence of the Q factor of our quadrant array. We implement a Helmholtz coil to vary the magnetic field at the detectors by (partially) nulling earth's. Our investigation shows that the earth magnetic field can significantly affect our KIDs' performance by degrading the Q factor by a factor of 2-5, well below those expected from the operational temperature or optical loading. We find that we can sufficiently recover our detectors' quality factor by tuning the current in the coils to generate a field that matches earth's magnetic field in magnitude to within a few uT. Therefore, it is necessary to employ a properly designed magnetic shield enclosing the TIM focal plane unit. Based on the results presented in this paper, we set a shielding requirement of |B| < 3 uT. |
| format | Preprint |
| id |
arxiv_https___arxiv_org_abs_2211_09308 |
| institution | arXiv |
| publishDate | 2022 |
| record_format | arxiv |
| spellingShingle | Design and testing of Kinetic Inductance Detector package for the Terahertz Intensity Mapper Liu, L. -J. Janssen, R. M. J Bradford, C. M. Hailey-Dunsheath, S. Filippini, J. P. Aguirre, J. E. Bracks, J. S. Corso, A. J. Fu, J. Groppi, C. Hoh, J. Keenan, R. P. Lowe, I. N. Marrone, D. P. Mauskopf, P. Nie, R. Redford, J. Trumper, I. Vieira, J. D. Instrumentation and Methods for Astrophysics Applied Physics Instrumentation and Detectors The Terahertz Intensity Mapper (TIM) is designed to probe the star formation history in dust-obscured star-forming galaxies around the peak of cosmic star formation. This will be done via measurements of the redshifted 157.7 um line of singly ionized carbon ([CII]). TIM employs two R $\sim 250$ long-slit grating spectrometers covering 240-420 um. Each is equipped with a focal plane unit containing 4 wafer-sized subarrays of horn-coupled aluminum kinetic inductance detectors (KIDs). We present the design and performance of a prototype focal plane assembly for one of TIM's KID-based subarrays. Our design strictly maintain high optical efficiency and a suitable electromagnetic environment for the KIDs. The prototype detector housing in combination with the first flight-like quadrant are tested at 250 mK. Initial frequency scan shows that many resonances are affected by collisions and/or very shallow transmission dips as a result of a degraded internal quality factor (Q factor). This is attributed to the presence of an external magnetic field during cooldown. We report on a study of magnetic field dependence of the Q factor of our quadrant array. We implement a Helmholtz coil to vary the magnetic field at the detectors by (partially) nulling earth's. Our investigation shows that the earth magnetic field can significantly affect our KIDs' performance by degrading the Q factor by a factor of 2-5, well below those expected from the operational temperature or optical loading. We find that we can sufficiently recover our detectors' quality factor by tuning the current in the coils to generate a field that matches earth's magnetic field in magnitude to within a few uT. Therefore, it is necessary to employ a properly designed magnetic shield enclosing the TIM focal plane unit. Based on the results presented in this paper, we set a shielding requirement of |B| < 3 uT. |
| title | Design and testing of Kinetic Inductance Detector package for the Terahertz Intensity Mapper |
| topic | Instrumentation and Methods for Astrophysics Applied Physics Instrumentation and Detectors |
| url | https://arxiv.org/abs/2211.09308 |