Additions to Standard Model and Atomic Physics
ORAL
Abstract
Recently, experiments at the ATOMKI laboratory on the possible existence of a
low-energy addition to the Standard Model have generated widespread attention.
While the experimental findings lack an independent confirmation, they give
incentive, from a more general point of view, to investigate the possible
detection of new particles with a rest mass of 15 to 20 MeV, in atomic physics
high-precision experiments. We find that, in this mass range, the effects will
be most pronounced in the spectra of muonic (not electronic) bound systems,
and, most notably, in the hyperfine structure. While it is a challenge to
separate the effects from nuclear-structure corrections to the hyperfine
splitting, this endeavor is definitely not hopeless. In general, in our work
[Phys.Rev.A 101 (2020) 062503], we derive the effective potentials
corresponding to the exchange of a pseudoscalar particle, and a conceivable
hitherto undetected vector particle, in two-body bound systems.
Comparison with the literature reveals
that the corresponding effective potentials may not have been treated
consistently in the past. Among other things, the role of the Coulomb gauge for
the massive vector propagator and its suitability for bound-state calculations
are being discussed.
low-energy addition to the Standard Model have generated widespread attention.
While the experimental findings lack an independent confirmation, they give
incentive, from a more general point of view, to investigate the possible
detection of new particles with a rest mass of 15 to 20 MeV, in atomic physics
high-precision experiments. We find that, in this mass range, the effects will
be most pronounced in the spectra of muonic (not electronic) bound systems,
and, most notably, in the hyperfine structure. While it is a challenge to
separate the effects from nuclear-structure corrections to the hyperfine
splitting, this endeavor is definitely not hopeless. In general, in our work
[Phys.Rev.A 101 (2020) 062503], we derive the effective potentials
corresponding to the exchange of a pseudoscalar particle, and a conceivable
hitherto undetected vector particle, in two-body bound systems.
Comparison with the literature reveals
that the corresponding effective potentials may not have been treated
consistently in the past. Among other things, the role of the Coulomb gauge for
the massive vector propagator and its suitability for bound-state calculations
are being discussed.
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Publication: Phys.Rev.A 101 (2020) 062503
Presenters
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Ulrich D Jentschura
Missouri University of Science & Technol
Authors
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Ulrich D Jentschura
Missouri University of Science & Technol