The Low-Energy Frontier of Particle Physics
By J. Jaeckel, A. Ringwald. 2010
960 citations recorded by the source corpus.
Most embeddings of the Standard Model into a more unified theory, in particular those based on supergravity or superstrings, predict the existence of a hidden sector of particles that have only very weak interactions with visible-sector Standard Model particles. Some of these exotic particle candidates [for instance, axions, axion-like particles, and hidden U(1) gauge bosons] may be very light, with masses in the subelectronvolt range, and may have very weak interactions with photons. Correspondingly, these very weakly interacting subelectronvolt particles (WISPs) may lead to observable effects in experiments (as well as in astrophysical and cosmological observations) searching for light shining through a wall, for changes in laser polarization, for nonlinear processes in large electromagnetic fields, and for deviations from Coulomb's law. We present the physics case and a status report of this emerging low-energy frontier of fundamental physics.
Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/3f60b79f75aa04e1f987f915de9a433a6c3132b0
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In Astronomy and Astrophysics
In Nuclear and High Energy Physics
- J. Redondo
- A. Ringwald
- R. Essig
- Igor G. Irastorza
- Atlas Collaboration
- Tongyan Lin
- K. Zurek
- Samuel D. McDermott
Citations in the corpus
- Cosmological bounds on pseudo Nambu-Goldstone bosons (2011, background): “interacting slim particles (WISPs), which are subjects of growing interest in the low-energy high-precision frontier of particle physics [3].”
- Light dark matter: Models and constraints (2017, neutral): “[129, 132, 133].”
- The ORGAN Experiment: An axion haloscope above 15 GHz (2017, background): “The most well known and theoretically motivated WISPs are axions (or “axion like particles”, ALPs).”
- Radio for hidden-photon dark matter detection (2014, background): “Hidden photons cannot make up all of the dark matter in the tan-shaded region [13], and are excluded entirely by various constraints in the gray shaded regions [19, 27, 41].”
- New axion and hidden photon constraints from a solar data global fit (2015, background): “The kinetic mixing is represented by the parameter χ and together with the hidden photon mass, m, are the parameters that must be constrained (see [9, 54–56] and references therein).”
- Dark photon limits: A handbook (2021, background): “However many of the axion’s experimental signatures are shared by another DM candidate—the dark photon (DP)1 [11, 24, 25]—which can be searched for with very similar techniques [26–39].”
- Constraining the mass of dark photons and axion-like particles through black-hole superradiance (2018, background): “Axion-like particles (ALPs) [7, 8] have properties similar to those of the QCD axion but their mass is not related to the decay constant.”
- Vector Dark Matter from Inflationary Fluctuations (2015, background): “[22] J.”
- Revisiting the SN1987A gamma-ray limit on ultralight axion-like particles (2014, background): “[8–10].”
- Asymmetric dark matter from leptogenesis (2011, background): “Further constraints on d are summarized in [66, 67 ].”