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In-beam measurement of the hydrogen hyperfine splitting - towards antihydrogen spectroscopy

Antihydrogen, the lightest atom consisting purely of antimatter, is an ideal laboratory to study the CPT symmetry by comparison with hydrogen. With respect to absolute precision, transitions within the ground-state hyperfine structure (GS-HFS) are most appealing by virtue of their small energy separ...

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Autores principales: Diermaier, M., Jepsen, C.B., Kolbinger, B., Malbrunot, C., Massiczek, O., Sauerzopf, C., Simon, M.C., Zmeskal, J., Widmann, E.
Lenguaje:eng
Publicado: 2016
Materias:
Acceso en línea:https://dx.doi.org/10.1038/ncomms15749
http://cds.cern.ch/record/2226763
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author Diermaier, M.
Jepsen, C.B.
Kolbinger, B.
Malbrunot, C.
Massiczek, O.
Sauerzopf, C.
Simon, M.C.
Zmeskal, J.
Widmann, E.
author_facet Diermaier, M.
Jepsen, C.B.
Kolbinger, B.
Malbrunot, C.
Massiczek, O.
Sauerzopf, C.
Simon, M.C.
Zmeskal, J.
Widmann, E.
author_sort Diermaier, M.
collection CERN
description Antihydrogen, the lightest atom consisting purely of antimatter, is an ideal laboratory to study the CPT symmetry by comparison with hydrogen. With respect to absolute precision, transitions within the ground-state hyperfine structure (GS-HFS) are most appealing by virtue of their small energy separation. ASACUSA proposed employing a beam of cold antihydrogen atoms in a Rabi-type experiment, to determine the GS-HFS in a field-free region. Here we present a measurement of the zero-field hydrogen GS-HFS using the spectroscopy apparatus of ASACUSA’s antihydrogen experiment. The measured value of νHF=1,420,405,748.4(3.4) (1.6) Hz with a relative precision of 2.7 × 10−9 constitutes the most precise determination of this quantity in a beam and verifies the developed spectroscopy methods for the antihydrogen HFS experiment to the p.p.b. level. Together with the recently presented observation of antihydrogen atoms 2.7 m downstream of the production region, the prerequisites for a measurement with antihydrogen are now available within the ASACUSA collaboration.
id cern-2226763
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2016
record_format invenio
spelling cern-22267632022-03-31T02:27:26Zdoi:10.1038/ncomms15749http://cds.cern.ch/record/2226763engDiermaier, M.Jepsen, C.B.Kolbinger, B.Malbrunot, C.Massiczek, O.Sauerzopf, C.Simon, M.C.Zmeskal, J.Widmann, E.In-beam measurement of the hydrogen hyperfine splitting - towards antihydrogen spectroscopyphysics.atom-phOther Fields of PhysicsAntihydrogen, the lightest atom consisting purely of antimatter, is an ideal laboratory to study the CPT symmetry by comparison with hydrogen. With respect to absolute precision, transitions within the ground-state hyperfine structure (GS-HFS) are most appealing by virtue of their small energy separation. ASACUSA proposed employing a beam of cold antihydrogen atoms in a Rabi-type experiment, to determine the GS-HFS in a field-free region. Here we present a measurement of the zero-field hydrogen GS-HFS using the spectroscopy apparatus of ASACUSA’s antihydrogen experiment. The measured value of νHF=1,420,405,748.4(3.4) (1.6) Hz with a relative precision of 2.7 × 10−9 constitutes the most precise determination of this quantity in a beam and verifies the developed spectroscopy methods for the antihydrogen HFS experiment to the p.p.b. level. Together with the recently presented observation of antihydrogen atoms 2.7 m downstream of the production region, the prerequisites for a measurement with antihydrogen are now available within the ASACUSA collaboration.Antihydrogen, the lightest atom consisting purely of antimatter, is an ideal laboratory to study the CPT symmetry by comparison to hydrogen. With respect to absolute precision, transitions within the ground-state hyperfine structure (GS-HFS) are most appealing by virtue of their small energy separation. ASACUSA proposed employing a beam of cold antihydrogen atoms in a Rabi-type experiment to determine the GS-HFS in a field-free region. Here we present a measurement of the zero-field hydrogen GS-HFS using the spectroscopy apparatus of ASACUSA's antihydrogen experiment. The measured value of $\nu_\mathrm{HF}$=$1~420~405~748.4(3.4)(1.6)~\textrm{Hz}$ with a relative precision of $\Delta nu_\mathrm{HF}$/$\nu_\mathrm{HF}$=$2.7\times10^{-9}$ constitutes the most precise determination of this quantity in a beam and verifies the developed spectroscopy methods for the antihydrogen HFS experiment to the ppb level. Together with the recently presented observation of antihydrogen atoms $2.7~\textrm{m}$ downstream of the production region, the prerequisites for a measurement with antihydrogen are now available within the ASACUSA collaboration.arXiv:1610.06392CERN-EP-2016-268oai:cds.cern.ch:22267632016-10-20
spellingShingle physics.atom-ph
Other Fields of Physics
Diermaier, M.
Jepsen, C.B.
Kolbinger, B.
Malbrunot, C.
Massiczek, O.
Sauerzopf, C.
Simon, M.C.
Zmeskal, J.
Widmann, E.
In-beam measurement of the hydrogen hyperfine splitting - towards antihydrogen spectroscopy
title In-beam measurement of the hydrogen hyperfine splitting - towards antihydrogen spectroscopy
title_full In-beam measurement of the hydrogen hyperfine splitting - towards antihydrogen spectroscopy
title_fullStr In-beam measurement of the hydrogen hyperfine splitting - towards antihydrogen spectroscopy
title_full_unstemmed In-beam measurement of the hydrogen hyperfine splitting - towards antihydrogen spectroscopy
title_short In-beam measurement of the hydrogen hyperfine splitting - towards antihydrogen spectroscopy
title_sort in-beam measurement of the hydrogen hyperfine splitting - towards antihydrogen spectroscopy
topic physics.atom-ph
Other Fields of Physics
url https://dx.doi.org/10.1038/ncomms15749
http://cds.cern.ch/record/2226763
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