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G$^0$ Electronics and Data Acquisition (Forward-Angle Measurements)

Identifieur interne : 000743 ( France/Analysis ); précédent : 000742; suivant : 000744

G$^0$ Electronics and Data Acquisition (Forward-Angle Measurements)

Auteurs : D. Marchand [France] ; J. Arvieux [France] ; L. Bimbot [France] ; A. Biselli [États-Unis] ; J. Bouvier [France] ; H. Breuer [États-Unis] ; R. Clark [États-Unis] ; J.-C. Cuzon [France] ; M. Engrand [France] ; R. Foglio [France] ; C. Furget [France] ; X. Grave [France] ; B. Guillon [France] ; H. Guler [France] ; P. M. King [États-Unis] ; S. Kox [France] ; J. Kuhn [États-Unis] ; Y. Ky [France] ; J. Lachniet [France] ; J. Lenoble [France] ; E. Liatard [France] ; J. Liu [États-Unis] ; E. Munoz [France] ; J. Pouxe [France] ; G. Quéméner [France] ; B. Quinn [États-Unis] ; J. S. Réal [France] ; O. Rossetto [France] ; R. Sellem [France]

Source :

RBID : Hal:in2p3-00136423

English descriptors

Abstract

The G$^0$ parity-violation experiment at Jefferson Lab (Newport News, VA) is designed to determine the contribution of strange/anti-strange quark pairs to the intrinsic properties of the proton. In the forward-angle part of the experiment, the asymmetry in the cross section was measured for $\vec{e}p$ elastic scattering by counting the recoil protons corresponding to the two beam-helicity states. Due to the high accuracy required on the asymmetry, the G$^0$ experiment was based on a custom experimental setup with its own associated electronics and data acquisition (DAQ) system. Highly specialized time-encoding electronics provided time-of-flight spectra for each detector for each helicity state. More conventional electronics was used for monitoring (mainly FastBus). The time-encoding electronics and the DAQ system have been designed to handle events at a mean rate of 2 MHz per detector with low deadtime and to minimize helicity-correlated systematic errors. In this paper, we outline the general architecture and the main features of the electronics and the DAQ system dedicated to G$^0$ forward-angle measurements.

Url:
DOI: 10.1016/j.nima.2007.11.028


Affiliations:

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Hal:in2p3-00136423

Le document en format XML

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<orgName>Université Grenoble Alpes</orgName>
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<date type="start">2016-01-01</date>
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<addrLine>CS 40700 - 38058 Grenoble cedex</addrLine>
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<ref type="url">http://www.univ-grenoble-alpes.fr</ref>
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<country>France</country>
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<region type="region" nuts="2">Auvergne-Rhône-Alpes</region>
<region type="old region" nuts="2">Rhône-Alpes</region>
</placeName>
<orgName type="university">Université Joseph Fourier</orgName>
<orgName type="institution" wicri:auto="newGroup">Université de Grenoble</orgName>
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<settlement type="city">Grenoble</settlement>
<region type="region" nuts="2">Auvergne-Rhône-Alpes</region>
<region type="old region" nuts="2">Rhône-Alpes</region>
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<orgName type="university">Université Grenoble-Alpes</orgName>
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<author>
<name sortKey="Sellem, R" sort="Sellem, R" uniqKey="Sellem R" first="R." last="Sellem">R. Sellem</name>
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<orgName>Institut de Physique Nucléaire d'Orsay</orgName>
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<orgName>Université Paris-Sud - Paris 11</orgName>
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<addrLine>Bâtiment 300 - 91405 Orsay cedex</addrLine>
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<ref type="url">http://www.u-psud.fr/</ref>
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</hal:affiliation>
<country>France</country>
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<idno type="DOI">10.1016/j.nima.2007.11.028</idno>
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<title level="j">Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment</title>
<idno type="ISSN">0168-9002</idno>
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<date type="datePub">2008</date>
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<keywords scheme="mix" xml:lang="en">
<term>electron scattering</term>
<term>high rate electronics</term>
<term>parity violation</term>
<term>time encoding</term>
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<div type="abstract" xml:lang="en">The G$^0$ parity-violation experiment at Jefferson Lab (Newport News, VA) is designed to determine the contribution of strange/anti-strange quark pairs to the intrinsic properties of the proton. In the forward-angle part of the experiment, the asymmetry in the cross section was measured for $\vec{e}p$ elastic scattering by counting the recoil protons corresponding to the two beam-helicity states. Due to the high accuracy required on the asymmetry, the G$^0$ experiment was based on a custom experimental setup with its own associated electronics and data acquisition (DAQ) system. Highly specialized time-encoding electronics provided time-of-flight spectra for each detector for each helicity state. More conventional electronics was used for monitoring (mainly FastBus). The time-encoding electronics and the DAQ system have been designed to handle events at a mean rate of 2 MHz per detector with low deadtime and to minimize helicity-correlated systematic errors. In this paper, we outline the general architecture and the main features of the electronics and the DAQ system dedicated to G$^0$ forward-angle measurements.</div>
</front>
</TEI>
<affiliations>
<list>
<country>
<li>France</li>
<li>États-Unis</li>
</country>
<region>
<li>Auvergne-Rhône-Alpes</li>
<li>Rhône-Alpes</li>
</region>
<settlement>
<li>Grenoble</li>
</settlement>
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<li>Université Grenoble-Alpes</li>
<li>Université Joseph Fourier</li>
<li>Université de Grenoble</li>
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<name sortKey="Marchand, D" sort="Marchand, D" uniqKey="Marchand D" first="D." last="Marchand">D. Marchand</name>
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<name sortKey="Bimbot, L" sort="Bimbot, L" uniqKey="Bimbot L" first="L." last="Bimbot">L. Bimbot</name>
<name sortKey="Bouvier, J" sort="Bouvier, J" uniqKey="Bouvier J" first="J." last="Bouvier">J. Bouvier</name>
<name sortKey="Cuzon, J C" sort="Cuzon, J C" uniqKey="Cuzon J" first="J.-C." last="Cuzon">J.-C. Cuzon</name>
<name sortKey="Engrand, M" sort="Engrand, M" uniqKey="Engrand M" first="M." last="Engrand">M. Engrand</name>
<name sortKey="Foglio, R" sort="Foglio, R" uniqKey="Foglio R" first="R." last="Foglio">R. Foglio</name>
<name sortKey="Furget, C" sort="Furget, C" uniqKey="Furget C" first="C." last="Furget">C. Furget</name>
<name sortKey="Grave, X" sort="Grave, X" uniqKey="Grave X" first="X." last="Grave">X. Grave</name>
<name sortKey="Guillon, B" sort="Guillon, B" uniqKey="Guillon B" first="B." last="Guillon">B. Guillon</name>
<name sortKey="Guler, H" sort="Guler, H" uniqKey="Guler H" first="H." last="Guler">H. Guler</name>
<name sortKey="Kox, S" sort="Kox, S" uniqKey="Kox S" first="S." last="Kox">S. Kox</name>
<name sortKey="Ky, Y" sort="Ky, Y" uniqKey="Ky Y" first="Y." last="Ky">Y. Ky</name>
<name sortKey="Lachniet, J" sort="Lachniet, J" uniqKey="Lachniet J" first="J." last="Lachniet">J. Lachniet</name>
<name sortKey="Lenoble, J" sort="Lenoble, J" uniqKey="Lenoble J" first="J." last="Lenoble">J. Lenoble</name>
<name sortKey="Liatard, E" sort="Liatard, E" uniqKey="Liatard E" first="E." last="Liatard">E. Liatard</name>
<name sortKey="Munoz, E" sort="Munoz, E" uniqKey="Munoz E" first="E." last="Munoz">E. Munoz</name>
<name sortKey="Pouxe, J" sort="Pouxe, J" uniqKey="Pouxe J" first="J." last="Pouxe">J. Pouxe</name>
<name sortKey="Quemener, G" sort="Quemener, G" uniqKey="Quemener G" first="G." last="Quéméner">G. Quéméner</name>
<name sortKey="Real, J S" sort="Real, J S" uniqKey="Real J" first="J. S." last="Réal">J. S. Réal</name>
<name sortKey="Rossetto, O" sort="Rossetto, O" uniqKey="Rossetto O" first="O." last="Rossetto">O. Rossetto</name>
<name sortKey="Sellem, R" sort="Sellem, R" uniqKey="Sellem R" first="R." last="Sellem">R. Sellem</name>
</country>
<country name="États-Unis">
<noRegion>
<name sortKey="Biselli, A" sort="Biselli, A" uniqKey="Biselli A" first="A." last="Biselli">A. Biselli</name>
</noRegion>
<name sortKey="Breuer, H" sort="Breuer, H" uniqKey="Breuer H" first="H." last="Breuer">H. Breuer</name>
<name sortKey="Clark, R" sort="Clark, R" uniqKey="Clark R" first="R." last="Clark">R. Clark</name>
<name sortKey="King, P M" sort="King, P M" uniqKey="King P" first="P. M." last="King">P. M. King</name>
<name sortKey="Kuhn, J" sort="Kuhn, J" uniqKey="Kuhn J" first="J." last="Kuhn">J. Kuhn</name>
<name sortKey="Liu, J" sort="Liu, J" uniqKey="Liu J" first="J." last="Liu">J. Liu</name>
<name sortKey="Quinn, B" sort="Quinn, B" uniqKey="Quinn B" first="B." last="Quinn">B. Quinn</name>
</country>
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</affiliations>
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