The MEG-II experiment searches for the lepton-flavor-violating decay: mu -> e + gamma. The reconstruction of the positron trajectory uses a cylindrical drift chamber operated with a mixture of He and iC(4)H(10) gas. It is important to provide a stable performance of the detector in terms of its electron transport parameters, avalanche multiplication, composition and purity of the gas mixture. In order to have a continuous monitoring of the quality of gas, we plan to install a small drift chamber, with a simple geometry that allows to measure very precisely the electron drift velocity in a prompt way. This monitoring chamber will be supplied with gas coming from the inlet and the outlet of the detector to determine if gas contaminations originate inside the main chamber or in the gas supply system. The chamber is a small box with cathode walls, that determine a highly uniform electric field inside two adjacent drift cells. Along the axis separating the two drift cells, four staggered sense wires alternated with five guard wires collect the drifting electrons. The trigger is provided by two 90Sr weak calibration radioactive sources placed on top of a two thin scintillator tiles telescope. The whole system is designed to give a prompt response (within a minute) about drift velocity variations at the 10(-3) level.

Cuna F., Chiarello G., Corvaglia A., Filippis N.D., Grancagnolo F., Manta M., et al. (2020). A 10-3drift velocity monitoring chamber. JOURNAL OF INSTRUMENTATION, 15(9) [10.1088/1748-0221/15/09/C09007].

A 10-3drift velocity monitoring chamber

Chiarello G.;
2020-01-01

Abstract

The MEG-II experiment searches for the lepton-flavor-violating decay: mu -> e + gamma. The reconstruction of the positron trajectory uses a cylindrical drift chamber operated with a mixture of He and iC(4)H(10) gas. It is important to provide a stable performance of the detector in terms of its electron transport parameters, avalanche multiplication, composition and purity of the gas mixture. In order to have a continuous monitoring of the quality of gas, we plan to install a small drift chamber, with a simple geometry that allows to measure very precisely the electron drift velocity in a prompt way. This monitoring chamber will be supplied with gas coming from the inlet and the outlet of the detector to determine if gas contaminations originate inside the main chamber or in the gas supply system. The chamber is a small box with cathode walls, that determine a highly uniform electric field inside two adjacent drift cells. Along the axis separating the two drift cells, four staggered sense wires alternated with five guard wires collect the drifting electrons. The trigger is provided by two 90Sr weak calibration radioactive sources placed on top of a two thin scintillator tiles telescope. The whole system is designed to give a prompt response (within a minute) about drift velocity variations at the 10(-3) level.
2020
The International Conference Instrumentation for Colliding Beam Physics (INSTR2020)
Febbraio 2020
Cuna F., Chiarello G., Corvaglia A., Filippis N.D., Grancagnolo F., Manta M., et al. (2020). A 10-3drift velocity monitoring chamber. JOURNAL OF INSTRUMENTATION, 15(9) [10.1088/1748-0221/15/09/C09007].
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/10447/618971
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