Discussion Overview
The discussion revolves around the theoretical exploration of models involving the gauge groups $$SU(3) \otimes U(1)_d$$ and $$SU(3) \otimes SU(2) \otimes U(1)_d$$ in the context of dark matter. Participants are interested in the implications of adding a dark U(1) to the Standard Model and the potential for dark matter to interact through strong forces.
Discussion Character
- Exploratory
- Technical explanation
- Debate/contested
Main Points Raised
- Some participants inquire about the implications of models incorporating $$SU(3) \otimes U(1)_d$$ or $$SU(3) \otimes SU(2) \otimes U(1)_d$$, expressing interest in references and resources.
- There is a suggestion to consider adding a dark U(1) to the Standard Model and studying its implications, with references to existing literature.
- One participant questions the feasibility of coupling dark matter to the strong nuclear force, proposing that dark matter could be hadronic and not reveal itself until deconfinement.
- Another participant raises concerns about the nature of the SU(3) group, questioning whether it is part of the Standard Model or a new "dark SU(3)" with dark gluons, and discusses potential interactions between dark baryons and ordinary nuclei.
- References to strongly interacting dark matter candidates (SIMP) are provided, noting that self-interaction may not necessarily align with QCD and discussing constraints from astrophysical observations.
- A participant clarifies their intent to explore strongly interacting particles alongside weakly interacting ones, indicating a desire to re-engage with the literature after a hiatus.
Areas of Agreement / Disagreement
Participants express varying views on the nature and implications of dark matter interactions, with no consensus reached on the specifics of the models or the feasibility of certain interactions.
Contextual Notes
Some discussions involve assumptions about the properties of dark matter and its interactions, which remain unresolved. The potential implications of dark matter being its own antiparticle and the effects of dark-light hybrid hadrons are also noted as areas of uncertainty.