Si Λ ViO: A trigger for Λ -Hyperons

The production of bound kaon–nucleon-states (kaonic-cluster) in the reaction p + p → [ ppK - ] + K + should be investigated in a dedicated measurement at the FOPI detector system at the SIS-accelerator of GSI, by looking for the decay [ ppK - ] → p + Λ → p + p + π - . To select the final states, the...

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Published inNuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment Vol. 617; no. 1; pp. 300 - 302
Main Authors Münzer, Robert, Fabbietti, Laura, Berger, Martin, Hartmann, Olaf
Format Journal Article
LanguageEnglish
Published Elsevier B.V 11.05.2010
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Abstract The production of bound kaon–nucleon-states (kaonic-cluster) in the reaction p + p → [ ppK - ] + K + should be investigated in a dedicated measurement at the FOPI detector system at the SIS-accelerator of GSI, by looking for the decay [ ppK - ] → p + Λ → p + p + π - . To select the final states, the detector system Si Λ ViO has been build up as a trigger for Λ -Hyperons. This detector consists of two layers of segmented silicon-strip-detectors, which are able to measure online the particle multiplicity. These two layers are arranged such, that most of the Λ -Hyperons will decay between them. The trigger signal is generated by comparing online the hit multiplicity on the two layers.
AbstractList The production of bound kaon-nucleon-states (kaonic-cluster) in the reaction p+p-->[ppK super(-)]+K super(+) should be investigated in a dedicated measurement at the FOPI detector system at the SIS-accelerator of GSI, by looking for the decay [ppK super(-)]-->p+ Lambda -->p+p+[pi] super(-). To select the final states, the detector system Si Lambda ViO has been build up as a trigger for Lambda -Hyperons. This detector consists of two layers of segmented silicon-strip-detectors, which are able to measure online the particle multiplicity. These two layers are arranged such, that most of the Lambda -Hyperons will decay between them. The trigger signal is generated by comparing online the hit multiplicity on the two layers.
The production of bound kaon–nucleon-states (kaonic-cluster) in the reaction p + p → [ ppK - ] + K + should be investigated in a dedicated measurement at the FOPI detector system at the SIS-accelerator of GSI, by looking for the decay [ ppK - ] → p + Λ → p + p + π - . To select the final states, the detector system Si Λ ViO has been build up as a trigger for Λ -Hyperons. This detector consists of two layers of segmented silicon-strip-detectors, which are able to measure online the particle multiplicity. These two layers are arranged such, that most of the Λ -Hyperons will decay between them. The trigger signal is generated by comparing online the hit multiplicity on the two layers.
Author Berger, Martin
Fabbietti, Laura
Münzer, Robert
Hartmann, Olaf
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References FOPI Collaboration, Experimental proposal to GSI, 2007.
July 2008.
M.Berger, Diploma thesis, May 2009.
Yamazaki, Akaishi (bib1) 2002; 535
Yamazaki, Akaishi (bib3) 2002; 72
Particle Data Group, Particle Data Booklet
Yamazaki, Akaishi (bib2) 2002; 65
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    fullname: Akaishi
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  publication-title: Phys. Lett. B
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Snippet The production of bound kaon–nucleon-states (kaonic-cluster) in the reaction p + p → [ ppK - ] + K + should be investigated in a dedicated measurement at the...
The production of bound kaon-nucleon-states (kaonic-cluster) in the reaction p+p-->[ppK super(-)]+K super(+) should be investigated in a dedicated measurement...
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StartPage 300
SubjectTerms Accelerators
Accumulation
Decay
Detectors
Kaonic-cluster-states
On-line systems
Online
Spectrometers
Title Si Λ ViO: A trigger for Λ -Hyperons
URI https://dx.doi.org/10.1016/j.nima.2009.06.094
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