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Design and performance of the field cage for the XENONnT experiment
Stockholms universitet, Naturvetenskapliga fakulteten, Fysikum. Stockholms universitet, Naturvetenskapliga fakulteten, Oskar Klein-centrum för kosmopartikelfysik (OKC).ORCID-id: 0000-0003-1331-2890
Stockholms universitet, Naturvetenskapliga fakulteten, Fysikum. Stockholms universitet, Naturvetenskapliga fakulteten, Oskar Klein-centrum för kosmopartikelfysik (OKC).ORCID-id: 0000-0001-9984-4411
Stockholms universitet, Naturvetenskapliga fakulteten, Fysikum. Stockholms universitet, Naturvetenskapliga fakulteten, Oskar Klein-centrum för kosmopartikelfysik (OKC). Stockholm Univ, Oskar Klein Ctr, Dept Phys, AlbaNova, S-10691 Stockholm, Sweden.ORCID-id: 0000-0002-4664-5504
Stockholms universitet, Naturvetenskapliga fakulteten, Oskar Klein-centrum för kosmopartikelfysik (OKC). Stockholms universitet, Naturvetenskapliga fakulteten, Fysikum.
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Rekke forfattare: 1642024 (engelsk)Inngår i: European Physical Journal C, ISSN 1434-6044, E-ISSN 1434-6052, Vol. 84, nr 2, artikkel-id 138Artikkel i tidsskrift (Fagfellevurdert) Published
Abstract [en]

The precision in reconstructing events detected in a dual-phase time projection chamber depends on an homogeneous and well understood electric field within the liquid target. In the XENONnT TPC the field homogeneity is achieved through a double-array field cage, consisting of two nested arrays of field shaping rings connected by an easily accessible resistor chain. Rather than being connected to the gate electrode, the topmost field shaping ring is independently biased, adding a degree of freedom to tune the electric field during operation. Two-dimensional finite element simulations were used to optimize the field cage, as well as its operation. Simulation results were compared to 83mKr calibration data. This comparison indicates an accumulation of charge on the panels of the TPC which is constant over time, as no evolution of the reconstructed position distribution of events is observed. The simulated electric field was then used to correct the charge signal for the field dependence of the charge yield. This correction resolves the inconsistent measurement of the drift electron lifetime when using different calibrations sources and different field cage tuning voltages.

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2024. Vol. 84, nr 2, artikkel-id 138
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URN: urn:nbn:se:su:diva-226992DOI: 10.1140/epjc/s10052-023-12296-yISI: 001159991600006Scopus ID: 2-s2.0-85195205079OAI: oai:DiVA.org:su-226992DiVA, id: diva2:1842267
Tilgjengelig fra: 2024-03-04 Laget: 2024-03-04 Sist oppdatert: 2025-02-14bibliografisk kontrollert

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Antochi, Vasile C.Conrad, JanRosso, Andrea GalloJoy, AshleyMahlstedt, JörnTan, Pueh-Leng

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