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Processing of the signals from the Liquid Xenon Calorimeter for timing measurements. / Epshteyn, L. B.; Grebenuyk, A. A.; Kozyrev, A. N. et al.

In: Journal of Instrumentation, Vol. 12, No. 2, 02035, 10.02.2017.

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Epshteyn LB, Grebenuyk AA, Kozyrev AN, Logashenko IB, Mikhaylov KY, Ruban AA et al. Processing of the signals from the Liquid Xenon Calorimeter for timing measurements. Journal of Instrumentation. 2017 Feb 10;12(2):02035. doi: 10.1088/1748-0221/12/02/C02035

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Epshteyn, L. B. ; Grebenuyk, A. A. ; Kozyrev, A. N. et al. / Processing of the signals from the Liquid Xenon Calorimeter for timing measurements. In: Journal of Instrumentation. 2017 ; Vol. 12, No. 2.

BibTeX

@article{07863ecaefb945eabf741b98193829ff,
title = "Processing of the signals from the Liquid Xenon Calorimeter for timing measurements",
abstract = "One of the goals of the Cryogenic Magnetic Detector at Budker Institute of Nuclear Physics SB RAS (Novosibirsk, Russia) is a study of hadron production in electron-positron collisions near threshold. The neutron-antineutron pair production events can be detected only by the calorimeters. In the barrel calorimeter the antineutron annihilation typically occurs about 5 ns or later after the beams crossing. For identification of such events it is necessary to measure the time of flight of particles to the LXe-calorimeter with an accuracy of about a few nanoseconds. The LXe-calorimeter consists of 14 layers of ionization chambers with two readout: anode and cathode. The duration of charge collection to the anodes is about 4.5 μs, while the required accuracy of measuring of the signal arrival time is less than 1/1000 of that (i.e. 4.5 ns). Besides, the signals' shapes differ substantially from event to event, so the signal arrival time is measured in two stages. In the paper we describ the development of the special electronics which performs waveform digitization and the on-line measurement of signals' arrival times and amplitudes.",
keywords = "Digital signal processing (DSP), Front-end electronics for detector readout, Trigger algorithms, CMD-3 DETECTOR",
author = "Epshteyn, {L. B.} and Grebenuyk, {A. A.} and Kozyrev, {A. N.} and Logashenko, {I. B.} and Mikhaylov, {K. Yu} and Ruban, {A. A.} and Yudin, {Yu V.}",
note = "Publisher Copyright: {\textcopyright} 2017 IOP Publishing Ltd and Sissa Medialab srl.",
year = "2017",
month = feb,
day = "10",
doi = "10.1088/1748-0221/12/02/C02035",
language = "English",
volume = "12",
journal = "Journal of Instrumentation",
issn = "1748-0221",
publisher = "IOP Publishing Ltd.",
number = "2",

}

RIS

TY - JOUR

T1 - Processing of the signals from the Liquid Xenon Calorimeter for timing measurements

AU - Epshteyn, L. B.

AU - Grebenuyk, A. A.

AU - Kozyrev, A. N.

AU - Logashenko, I. B.

AU - Mikhaylov, K. Yu

AU - Ruban, A. A.

AU - Yudin, Yu V.

N1 - Publisher Copyright: © 2017 IOP Publishing Ltd and Sissa Medialab srl.

PY - 2017/2/10

Y1 - 2017/2/10

N2 - One of the goals of the Cryogenic Magnetic Detector at Budker Institute of Nuclear Physics SB RAS (Novosibirsk, Russia) is a study of hadron production in electron-positron collisions near threshold. The neutron-antineutron pair production events can be detected only by the calorimeters. In the barrel calorimeter the antineutron annihilation typically occurs about 5 ns or later after the beams crossing. For identification of such events it is necessary to measure the time of flight of particles to the LXe-calorimeter with an accuracy of about a few nanoseconds. The LXe-calorimeter consists of 14 layers of ionization chambers with two readout: anode and cathode. The duration of charge collection to the anodes is about 4.5 μs, while the required accuracy of measuring of the signal arrival time is less than 1/1000 of that (i.e. 4.5 ns). Besides, the signals' shapes differ substantially from event to event, so the signal arrival time is measured in two stages. In the paper we describ the development of the special electronics which performs waveform digitization and the on-line measurement of signals' arrival times and amplitudes.

AB - One of the goals of the Cryogenic Magnetic Detector at Budker Institute of Nuclear Physics SB RAS (Novosibirsk, Russia) is a study of hadron production in electron-positron collisions near threshold. The neutron-antineutron pair production events can be detected only by the calorimeters. In the barrel calorimeter the antineutron annihilation typically occurs about 5 ns or later after the beams crossing. For identification of such events it is necessary to measure the time of flight of particles to the LXe-calorimeter with an accuracy of about a few nanoseconds. The LXe-calorimeter consists of 14 layers of ionization chambers with two readout: anode and cathode. The duration of charge collection to the anodes is about 4.5 μs, while the required accuracy of measuring of the signal arrival time is less than 1/1000 of that (i.e. 4.5 ns). Besides, the signals' shapes differ substantially from event to event, so the signal arrival time is measured in two stages. In the paper we describ the development of the special electronics which performs waveform digitization and the on-line measurement of signals' arrival times and amplitudes.

KW - Digital signal processing (DSP)

KW - Front-end electronics for detector readout

KW - Trigger algorithms

KW - CMD-3 DETECTOR

UR - http://www.scopus.com/inward/record.url?scp=85014798881&partnerID=8YFLogxK

U2 - 10.1088/1748-0221/12/02/C02035

DO - 10.1088/1748-0221/12/02/C02035

M3 - Article

AN - SCOPUS:85014798881

VL - 12

JO - Journal of Instrumentation

JF - Journal of Instrumentation

SN - 1748-0221

IS - 2

M1 - 02035

ER -

ID: 8835970