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Power Deposition in LHC Magnets Due to Bound-Free Pair Production in the Experimental Insertions

The peak luminosity achieved during Pb-Pb collisions in the LHC in 2015 (3x1027cm⁻²s^{−1}) well exceeded the design luminosity and is anticipated to increase by another factor 2 after the next Long Shutdown (2019- 2020). A significant fraction of the power dissipated in ultra-peripheral Pb-Pb collis...

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Detalles Bibliográficos
Autores principales: Bahamonde Castro, Cristina, Auchmann, Bernhard, Besana, Maria Ilaria, Brodzinski, Krzysztof, Bruce, Roderik, Cerutti, Francesco, Jowett, John, Lechner, Anton, Mertens, Tom, Parma, Vittorio, Redaelli, Stefano, Schaumann, Michaela, Shetty, Nikhil Vittal, Skordis, Eleftherios, Steele, Genevieve, van Weelderen, Rob
Lenguaje:eng
Publicado: 2016
Materias:
Acceso en línea:https://dx.doi.org/10.18429/JACoW-IPAC2016-TUPMW006
http://cds.cern.ch/record/2207361
Descripción
Sumario:The peak luminosity achieved during Pb-Pb collisions in the LHC in 2015 (3x1027cm⁻²s^{−1}) well exceeded the design luminosity and is anticipated to increase by another factor 2 after the next Long Shutdown (2019- 2020). A significant fraction of the power dissipated in ultra-peripheral Pb-Pb collisions is carried by ions from bound-free pair production, which are lost in the dispersion suppressors adjacent to the experimental insertions. At higher luminosities, these ions risk to quench superconducting magnets and might limit their operation due to the dynamic heat load that needs to be evacuated by the cryogenic system. In this paper, we estimate the power deposition in superconducting coils and the magnet cold mass and we quantify the achievable reduction by deviating losses to less sensitive locations or by installing collimators at strategic positions. The second option is considered for the dispersion suppressor next to the ALICE insertion, where a selective displacement of losses to a magnet-free region is not possible.