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Pumped helium system for cooling positron and electron traps to 1.2 K

Extremely precise tests of fundamental particle symmetries should be possible via laser spectroscopy of trapped antihydrogen ((H) over bar) atoms. (H) over bar atoms that can be trapped must have an energy in temperature units that is below 0.5 K-the energy depth of the deepest magnetic traps that c...

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Detalles Bibliográficos
Autores principales: Wrubel, J, Gabrielse, G, Kolthammer, W S, Larochelle, P, McConnell, R, Richerme, P, Grzonka, D, Oelert, W, Sefzick, T, Zielinski, M, Borbely, J S, George, M C, Hessels, E A, Storry, C H, Weel, M, Mullers, A, Walz, J, Speck, A
Lenguaje:eng
Publicado: 2011
Materias:
XX
Acceso en línea:https://dx.doi.org/10.1016/j.nima.2011.01.030
http://cds.cern.ch/record/1489610
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author Wrubel, J
Gabrielse, G
Kolthammer, W S
Larochelle, P
McConnell, R
Richerme, P
Grzonka, D
Oelert, W
Sefzick, T
Zielinski, M
Borbely, J S
George, M C
Hessels, E A
Storry, C H
Weel, M
Mullers, A
Walz, J
Speck, A
author_facet Wrubel, J
Gabrielse, G
Kolthammer, W S
Larochelle, P
McConnell, R
Richerme, P
Grzonka, D
Oelert, W
Sefzick, T
Zielinski, M
Borbely, J S
George, M C
Hessels, E A
Storry, C H
Weel, M
Mullers, A
Walz, J
Speck, A
author_sort Wrubel, J
collection CERN
description Extremely precise tests of fundamental particle symmetries should be possible via laser spectroscopy of trapped antihydrogen ((H) over bar) atoms. (H) over bar atoms that can be trapped must have an energy in temperature units that is below 0.5 K-the energy depth of the deepest magnetic traps that can currently be constructed with high currents and superconducting technology. The number of atoms in a Boltzmann distribution with energies lower than this trap depth depends sharply upon the temperature of the thermal distribution. For example, ten times more atoms with energies low enough to be trapped are in a thermal distribution at a temperature of 1.2 K than for a temperature of 4.2 K. To date, (H) over bar atoms have only been produced within traps whose electrode temperature is 4.2 K or higher. A lower temperature apparatus is desirable if usable numbers of atoms that can be trapped are to eventually be produced. This report is about the pumped helium apparatus that cooled the trap electrodes of an (H) over bar apparatus to 1.2 K for the first time. Significant apparatus challenges include the need to cool a 0.8 m stack of 37 trap electrodes separated by only a mm from the substantial mass of a 4.2 K loffe trap and the substantial mass of a 4.2 K solenoid. Access to the interior of the cold electrodes must be maintained for antiprotons, positrons, electrons and lasers.
id cern-1489610
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2011
record_format invenio
spelling cern-14896102019-09-30T06:29:59Zdoi:10.1016/j.nima.2011.01.030http://cds.cern.ch/record/1489610engWrubel, JGabrielse, GKolthammer, W SLarochelle, PMcConnell, RRicherme, PGrzonka, DOelert, WSefzick, TZielinski, MBorbely, J SGeorge, M CHessels, E AStorry, C HWeel, MMullers, AWalz, JSpeck, APumped helium system for cooling positron and electron traps to 1.2 KXXExtremely precise tests of fundamental particle symmetries should be possible via laser spectroscopy of trapped antihydrogen ((H) over bar) atoms. (H) over bar atoms that can be trapped must have an energy in temperature units that is below 0.5 K-the energy depth of the deepest magnetic traps that can currently be constructed with high currents and superconducting technology. The number of atoms in a Boltzmann distribution with energies lower than this trap depth depends sharply upon the temperature of the thermal distribution. For example, ten times more atoms with energies low enough to be trapped are in a thermal distribution at a temperature of 1.2 K than for a temperature of 4.2 K. To date, (H) over bar atoms have only been produced within traps whose electrode temperature is 4.2 K or higher. A lower temperature apparatus is desirable if usable numbers of atoms that can be trapped are to eventually be produced. This report is about the pumped helium apparatus that cooled the trap electrodes of an (H) over bar apparatus to 1.2 K for the first time. Significant apparatus challenges include the need to cool a 0.8 m stack of 37 trap electrodes separated by only a mm from the substantial mass of a 4.2 K loffe trap and the substantial mass of a 4.2 K solenoid. Access to the interior of the cold electrodes must be maintained for antiprotons, positrons, electrons and lasers.oai:cds.cern.ch:14896102011
spellingShingle XX
Wrubel, J
Gabrielse, G
Kolthammer, W S
Larochelle, P
McConnell, R
Richerme, P
Grzonka, D
Oelert, W
Sefzick, T
Zielinski, M
Borbely, J S
George, M C
Hessels, E A
Storry, C H
Weel, M
Mullers, A
Walz, J
Speck, A
Pumped helium system for cooling positron and electron traps to 1.2 K
title Pumped helium system for cooling positron and electron traps to 1.2 K
title_full Pumped helium system for cooling positron and electron traps to 1.2 K
title_fullStr Pumped helium system for cooling positron and electron traps to 1.2 K
title_full_unstemmed Pumped helium system for cooling positron and electron traps to 1.2 K
title_short Pumped helium system for cooling positron and electron traps to 1.2 K
title_sort pumped helium system for cooling positron and electron traps to 1.2 k
topic XX
url https://dx.doi.org/10.1016/j.nima.2011.01.030
http://cds.cern.ch/record/1489610
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