8–10 May 2023
University of Pittsburgh
US/Eastern timezone

Session

DM III

9 May 2023, 16:30
Lawrence Hall 203

Lawrence Hall 203

Conveners

DM III

  • Gopolang Mohlabeng (University of California, Irvine)

Presentation materials

There are no materials yet.

  1. Shuailiang Ge (Peking University)
    09/05/2023, 16:30
    Dark Matter

    Ultralight axions and dark photons are compelling candidates for dark matter. In this talk, I will provide an overview of my recent work (arXiv:2207.05767, 2301.03622) on detecting radio-frequency axions and dark photons using radio telescopes. The detectability relies on two distinct underlying mechanisms. One mechanism involves local dark photon dark matter inducing harmonic oscillations of...

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  2. Javier Acevedo (SLAC)
    09/05/2023, 16:45
    Dark Matter

    The minimum testable dark matter (DM) mass for almost all DM signatures in celestial bodies is determined by the rate at which DM evaporates. DM evaporation has previously been calculated assuming a competition between the gravitational potential of the object, and thermal kicks from the celestial-body matter. I will point out a new effect, where mediators with a range larger than the...

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  3. Leo Kim
    09/05/2023, 17:00
    Dark Matter

    A dissipative dark sector can result in the formation of astrophysical compact objects. In this work, we investigate the formation of exotic compact objects assuming a subdominant inelastic dark matter model, and study the resulting landscape of these objects. Inelastic transitions introduce radiative processes which can impact the formation of compact objects via mutliple cooling channels. In...

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  4. Nirmalya Brahma (McGill University)
    09/05/2023, 17:15
    Dark Matter

    Dark photons can oscillate into SM photons via kinetic mixing in a way that is analogous to neutrino oscillations. Much like the MSW effect for neutrinos in environments of varying density, the probability for dark photons to convert to photons depends on the properties of the ambient background (density, electromagnetic fields, etc.) Resonances are even possible when there is a level-crossing...

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  5. Deepak Sathyan
    09/05/2023, 17:30

    We consider the effect of interactions between supernova neutrinos and dark matter. As these neutrinos travel towards Earth through a column density of dark matter, they could interact via dark mediator, deflecting after the process. Depending on the location of the supernova with respect to Earth, the attenuation of the neutrino flux from a local supernova could be observable by neutrino...

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  6. Dr Sandra Robles (Fermilab)
    09/05/2023, 17:45

    Upcoming neutrino experiments are expected to detect the Diffuse Supernova Neutrino Background (DSNB). This requires pondering all possible sources of background. Sub-GeV dark matter (DM) which annihilates into neutrinos is a potential background that has not been considered so far. We simulate DSNB and DM signals, as well as backgrounds in the Hyper-Kamiokande detector. We find that...

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  7. Tyler Horoho (University of Virginia)
    09/05/2023, 18:00
    Dark Matter

    The constituents of dark matter are still unknown, and the viable possibilities span a very large mass range. Specific scenarios for the origin of dark matter sharpen the focus to within about an MeV to 100 TeV. Most of the stable constituents of known matter have masses in the lower range, and a thermal origin for dark matter works in a simple and predictive manner in this mass range as well....

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  8. Badal Bhalla (University of Oklahoma)
    09/05/2023, 18:15
    Axion and ALP

    Stellar binaries have historically provided a rich target in the search for exotic compact objects such as primordial black holes (PBHs) or MACHOs. A sufficiently heavy compact object flying sufficiently close to a binary will disrupt or soften it, an effect that will show up in binary data as sparseness at large separation bins. While most studies have focused on the softening of wide...

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