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Overview of Beam-Beam Effects in the Tevatron
For almost a quarter of a century the Tevatron proton-antiproton collider was the centrepiece of the world's high-energy physics program, from the start of operation in December 1985 until it was overtaken by the LHC in 2011. The initial design luminosity of the Tevatron was 1030 cm-2 s-1; howe...
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Lenguaje: | eng |
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2014
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Acceso en línea: | https://dx.doi.org/10.5170/CERN-2014-004.11 http://cds.cern.ch/record/1955089 |
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author | Shiltsev, V. |
author_facet | Shiltsev, V. |
author_sort | Shiltsev, V. |
collection | CERN |
description | For almost a quarter of a century the Tevatron proton-antiproton collider was the centrepiece of the world's high-energy physics program, from the start of operation in December 1985 until it was overtaken by the LHC in 2011. The initial design luminosity of the Tevatron was 1030 cm-2 s-1; however, as a result of two decades of upgrades, the accelerator has been able to deliver 430-times higher luminosities to each of two high-luminosity experiments, Collider Detector at Fermilab (CDF) and D0. On the way to record high luminosities, many issues related to the electromagnetic beam-beam interaction of colliding beams have been addressed. Below we present a short overview of the beam-beam effects in the Tevatron. |
id | cern-1955089 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2014 |
record_format | invenio |
spelling | cern-19550892023-06-27T04:56:35Zdoi:10.5170/CERN-2014-004.11http://cds.cern.ch/record/1955089engShiltsev, V.Overview of Beam-Beam Effects in the TevatronAccelerators and Storage RingsFor almost a quarter of a century the Tevatron proton-antiproton collider was the centrepiece of the world's high-energy physics program, from the start of operation in December 1985 until it was overtaken by the LHC in 2011. The initial design luminosity of the Tevatron was 1030 cm-2 s-1; however, as a result of two decades of upgrades, the accelerator has been able to deliver 430-times higher luminosities to each of two high-luminosity experiments, Collider Detector at Fermilab (CDF) and D0. On the way to record high luminosities, many issues related to the electromagnetic beam-beam interaction of colliding beams have been addressed. Below we present a short overview of the beam-beam effects in the Tevatron.For almost a quarter of a century the Tevatron proton-antiproton collider was the centrepiece of the world's high-energy physics program, from the start of operation in December 1985 until it was overtaken by the LHC in 2011. The initial design luminosity of the Tevatron was 1030 cm-2 s-1; however, as a result of two decades of upgrades, the accelerator has been able to deliver 430-times higher luminosities to each of two high-luminosity experiments, Collider Detector at Fermilab (CDF) and D0. On the way to record high luminosities, many issues related to the electromagnetic beam-beam interaction of colliding beams have been addressed. Below we present a short overview of the beam-beam effects in the Tevatron.arXiv:1410.3326FERMILAB-CONF-13-107-APCoai:cds.cern.ch:19550892014-10-13 |
spellingShingle | Accelerators and Storage Rings Shiltsev, V. Overview of Beam-Beam Effects in the Tevatron |
title | Overview of Beam-Beam Effects in the Tevatron |
title_full | Overview of Beam-Beam Effects in the Tevatron |
title_fullStr | Overview of Beam-Beam Effects in the Tevatron |
title_full_unstemmed | Overview of Beam-Beam Effects in the Tevatron |
title_short | Overview of Beam-Beam Effects in the Tevatron |
title_sort | overview of beam-beam effects in the tevatron |
topic | Accelerators and Storage Rings |
url | https://dx.doi.org/10.5170/CERN-2014-004.11 http://cds.cern.ch/record/1955089 |
work_keys_str_mv | AT shiltsevv overviewofbeambeameffectsinthetevatron |