Cargando…
BASE – The Baryon Antibaryon Symmetry Experiment
The Baryon Antibaryon Symmetry Experiment (BASE) aims at performing a stringent test of the combined charge parity and time reversal (CPT) symmetry by comparing the magnetic moments of the proton and the antiproton with high precision. Using single particles in a Penning trap, the proton/antiproton...
Autores principales: | , , , , , , , , , , , , , , , , , , , |
---|---|
Lenguaje: | eng |
Publicado: |
2016
|
Materias: | |
Acceso en línea: | https://dx.doi.org/10.1140/epjst/e2015-02607-4 https://dx.doi.org/10.1140/epjst/e2015-02336-2 http://cds.cern.ch/record/2149810 |
_version_ | 1780950443618205696 |
---|---|
author | Smorra, C. Blaum, K. Bojtar, L. Borchert, M. Franke, K.A. Higuchi, T. Leefer, N. Nagahama, H. Matsuda, Y. Mooser, A. Niemann, M. Ospelkaus, C. Quint, W. Schneider, G. Sellner, S. Tanaka, T. Van Gorp, S. Walz, J. Yamazaki, Y. Ulmer, S. |
author_facet | Smorra, C. Blaum, K. Bojtar, L. Borchert, M. Franke, K.A. Higuchi, T. Leefer, N. Nagahama, H. Matsuda, Y. Mooser, A. Niemann, M. Ospelkaus, C. Quint, W. Schneider, G. Sellner, S. Tanaka, T. Van Gorp, S. Walz, J. Yamazaki, Y. Ulmer, S. |
author_sort | Smorra, C. |
collection | CERN |
description | The Baryon Antibaryon Symmetry Experiment (BASE) aims at performing a stringent test of the combined charge parity and time reversal (CPT) symmetry by comparing the magnetic moments of the proton and the antiproton with high precision. Using single particles in a Penning trap, the proton/antiproton $g$-factors, i.e. the magnetic moment in units of the nuclear magneton, are determined by measuring the respective ratio of the spin-precession frequency to the cyclotron frequency. The spin precession frequency is measured by non-destructive detection of spin quantum transitions using the continuous Stern-Gerlach effect, and the cyclotron frequency is determined from the particle's motional eigenfrequencies in the Penning trap using the invariance theorem. By application of the double Penning-trap method we expect that in our measurements a fractional precision of $\delta g/g$ 10$^{-9}$ can be achieved. The successful application of this method to the antiproton will represent a factor 1000 improvement in the fractional precision of its magnetic moment. The BASE collaboration has constructed and commissioned a new experiment at the Antiproton Decelerator (AD) of CERN. This article describes and summarizes the physical and technical aspects of this new experiment. |
id | cern-2149810 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2016 |
record_format | invenio |
spelling | cern-21498102022-05-06T08:11:29Zdoi:10.1140/epjst/e2015-02607-4doi:10.1140/epjst/e2015-02336-2http://cds.cern.ch/record/2149810engSmorra, C.Blaum, K.Bojtar, L.Borchert, M.Franke, K.A.Higuchi, T.Leefer, N.Nagahama, H.Matsuda, Y.Mooser, A.Niemann, M.Ospelkaus, C.Quint, W.Schneider, G.Sellner, S.Tanaka, T.Van Gorp, S.Walz, J.Yamazaki, Y.Ulmer, S.BASE – The Baryon Antibaryon Symmetry ExperimentOther Fields of PhysicsThe Baryon Antibaryon Symmetry Experiment (BASE) aims at performing a stringent test of the combined charge parity and time reversal (CPT) symmetry by comparing the magnetic moments of the proton and the antiproton with high precision. Using single particles in a Penning trap, the proton/antiproton $g$-factors, i.e. the magnetic moment in units of the nuclear magneton, are determined by measuring the respective ratio of the spin-precession frequency to the cyclotron frequency. The spin precession frequency is measured by non-destructive detection of spin quantum transitions using the continuous Stern-Gerlach effect, and the cyclotron frequency is determined from the particle's motional eigenfrequencies in the Penning trap using the invariance theorem. By application of the double Penning-trap method we expect that in our measurements a fractional precision of $\delta g/g$ 10$^{-9}$ can be achieved. The successful application of this method to the antiproton will represent a factor 1000 improvement in the fractional precision of its magnetic moment. The BASE collaboration has constructed and commissioned a new experiment at the Antiproton Decelerator (AD) of CERN. This article describes and summarizes the physical and technical aspects of this new experiment.The Baryon Antibaryon Symmetry Experiment (BASE) aims at performing a stringent test of the combined charge parity and time reversal (CPT) symmetry by comparing the magnetic moments of the proton and the antiproton with high precision. Using single particles in a Penning trap, the proton/antiproton g-factors, i.e. the magnetic moment in units of the nuclear magneton, are determined by measuring the respective ratio of the spin-precession frequency to the cyclotron frequency. The spin precession frequency is measured by non-destructive detection of spin quantum transitions using the continuous Stern-Gerlach effect, and the cyclotron frequency is determined from the particle*s motional eigenfrequencies in the Penning trap using the invariance theorem. By application of the double Penning-trap method we expect that in our measurements a fractional precision of δg/g 10$^{−9}$ can be achieved. The successful application of this method to the antiproton will consist a factor 1000 improvement in the fractional precision of its magnetic moment. The BASE collaboration has constructed and commissioned a new experiment at the Antiproton Decelerator (AD) of CERN. This article describes and summarizes the physical and technical aspects of this new experiment.The Baryon Antibaryon Symmetry Experiment (BASE) aims at performing a stringent test of the combined charge parity and time reversal (CPT) symmetry by comparing the magnetic moments of the proton and the antiproton with high precision. Using single particles in a Penning trap, the proton/antiproton $g$-factors, i.e. the magnetic moment in units of the nuclear magneton, are determined by measuring the respective ratio of the spin-precession frequency to the cyclotron frequency. The spin precession frequency is measured by non-destructive detection of spin quantum transitions using the continuous Stern-Gerlach effect, and the cyclotron frequency is determined from the particle's motional eigenfrequencies in the Penning trap using the invariance theorem. By application of the double Penning-trap method we expect that in our measurements a fractional precision of $\delta g/g$ 10$^{-9}$ can be achieved. The successful application of this method to the antiproton will represent a factor 1000 improvement in the fractional precision of its magnetic moment. The BASE collaboration has constructed and commissioned a new experiment at the Antiproton Decelerator (AD) of CERN. This article describes and summarizes the physical and technical aspects of this new experiment.arXiv:1604.08820oai:cds.cern.ch:21498102016-04-29 |
spellingShingle | Other Fields of Physics Smorra, C. Blaum, K. Bojtar, L. Borchert, M. Franke, K.A. Higuchi, T. Leefer, N. Nagahama, H. Matsuda, Y. Mooser, A. Niemann, M. Ospelkaus, C. Quint, W. Schneider, G. Sellner, S. Tanaka, T. Van Gorp, S. Walz, J. Yamazaki, Y. Ulmer, S. BASE – The Baryon Antibaryon Symmetry Experiment |
title | BASE – The Baryon Antibaryon Symmetry Experiment |
title_full | BASE – The Baryon Antibaryon Symmetry Experiment |
title_fullStr | BASE – The Baryon Antibaryon Symmetry Experiment |
title_full_unstemmed | BASE – The Baryon Antibaryon Symmetry Experiment |
title_short | BASE – The Baryon Antibaryon Symmetry Experiment |
title_sort | base – the baryon antibaryon symmetry experiment |
topic | Other Fields of Physics |
url | https://dx.doi.org/10.1140/epjst/e2015-02607-4 https://dx.doi.org/10.1140/epjst/e2015-02336-2 http://cds.cern.ch/record/2149810 |
work_keys_str_mv | AT smorrac basethebaryonantibaryonsymmetryexperiment AT blaumk basethebaryonantibaryonsymmetryexperiment AT bojtarl basethebaryonantibaryonsymmetryexperiment AT borchertm basethebaryonantibaryonsymmetryexperiment AT frankeka basethebaryonantibaryonsymmetryexperiment AT higuchit basethebaryonantibaryonsymmetryexperiment AT leefern basethebaryonantibaryonsymmetryexperiment AT nagahamah basethebaryonantibaryonsymmetryexperiment AT matsuday basethebaryonantibaryonsymmetryexperiment AT moosera basethebaryonantibaryonsymmetryexperiment AT niemannm basethebaryonantibaryonsymmetryexperiment AT ospelkausc basethebaryonantibaryonsymmetryexperiment AT quintw basethebaryonantibaryonsymmetryexperiment AT schneiderg basethebaryonantibaryonsymmetryexperiment AT sellners basethebaryonantibaryonsymmetryexperiment AT tanakat basethebaryonantibaryonsymmetryexperiment AT vangorps basethebaryonantibaryonsymmetryexperiment AT walzj basethebaryonantibaryonsymmetryexperiment AT yamazakiy basethebaryonantibaryonsymmetryexperiment AT ulmers basethebaryonantibaryonsymmetryexperiment |