"Dark matter phenomena" are real, based upon the consensus interpretation of astronomers and astrophysicists looking at astronomy evidence.
Overwhelming evidence shows the existence of "dark matter phenomena" evidenced primarily by the dynamics of galaxies and galaxy clusters, by the gap between all discernible sources of ordinary matter and the amount of matter inferred using a Newtonian approximation of gravity, and by the gap between all discernible sources of ordinary matter and the amount of matter inferred from gravitational lensing of light using a weak field approximation of General Relativity. Cosmic background radiation patterns also support the conclusion that dark matter phenomena are real.
But Stacy McGaugh in his latest blog post at Triton Station, reminds us that there have been no credible and reliable detections of dark matter itself in the Milky Way, even though many hypotheses have been searched for with a variety of means.
Direct detection experiments have come up empty and have probed dark matter particle mass ranges from a bit below 1 GeV to about 1000 GeV.
Macroscopic dark matter candidates like primordial black holes and MACHOs have been ruled out.
No missing momentum signals in collider experiments up to the 13 TeV energies of the Large Hadron Collider have revealed any anomalies that are good dark matter candidates produced in these reactions.
Astronomy searches for dark matter annihilation signatures have come up empty and where there have been anomalies have other explanations that don't require new physics or dark matter particles.
The dynamics of dark matter also, generally speaking, rule out heavy dark matter candidates with particle masses in excess of 1 TeV, or for that matter, in excess of a KeV mass.
The lack of direct detections or detections of decay products doesn't in and of itself rule out the dark matter hypothesis. It just tightens the parameter space for dark matter to something that doesn't interact via Standard Model forces and is stable on a time frame of many billions of years of mean lifetime or more.
But, the problem you get when you impose those conditions is that you can't explain why dark matter isn't observed to have the NFW halo distribution that dark matter like that should have. A self-interaction of dark matter with dark matter only (SIDM) could partially remedy that problem, although efforts to model that and fit parameters for that self-interaction have largely been unsuccessful.
Some dark matter models are ruled out by evidence from Big Bang Nucelosynthesis.
Most importantly, you can't explain why dark matter phenomena can be accurately predicted from the distribution of ordinary matter in a system in a very tight correlation if it has no non-gravitational interactions with ordinary matter.
This is why I strongly favor gravity or fifth force explanations for dark matter phenomena. An extremely light bosonic dark matter particle candidate, however, starts to blur the line between a fifth force and a dark matter particle explanation.
In all other aspects of physics, forces are carried by bosons (i.e. particles with integer intrinsic angular momentums like 0, 1, 2, etc.) that we sometimes simplify to think of as force fields, while the stuff that we think of as matter in a plain English sense of the word, is made up of fermions (i.e. particles with intrinsic angular momentum of 1/2, 3/2, etc.).
7 comments:
I do not understand why it is not accepted that gravitons are dark matter and have been seen in gravity wave experiments.
Because non-perturbative effects are hard to calculate.
arXiv:2512.17672 (hep-ph)
[Submitted on 19 Dec 2025]
Two-lepton tales: Dalitz decays of heavy quarkonia
Pietro Colangelo, Fulvia De Fazio, Riccardo Pinto
We study the Dalitz decays of heavy quarkonia, which result from the internal virtual photon conversion into an lepton pair. Heavy-quark symmetries allow us to establish systematic relations between transitions of different quarkonium states, and to precisely determine the branching fractions for several charmonium and bottomonium decay modes. For charmonium, existing data on and enable us to determine the parameters of the transition form factors and to predict the rates of yet-unobserved modes. The Dalitz transitions of are important, as they can help assessing the structure of this meson. For bottomonium, recent LHCb measurements allow us to predict the branching fractions of and ( . We also investigate the sensitivity of heavy quarkonia Dalitz modes to the contribution of a new light vector mediator, such as the putative .
[Submitted on 10 Dec 2025 (v1), last revised 17 Dec 2025 (this version, v2)]
Potential for the discovery of the protophobic boson at the STCF
Althaf M., Triparno Bandyopadhyay
We study the morphology of the main drift chamber (MDC) proposed to be built around the collision point at the upcoming Super tau-charm facility (STCF), to check for its suitability in discovering the 17 MeV protophobic boson (X17 boson), hypothesised as a solution to the persistent ATOMKI nuclear-transition anomalies. These anomalies, observed in the excited Be, He, C, O nuclear transitions, have been interpreted as evidence for a 17 MeV, protophobic vector boson. Using the TrackEff framework, we perform detector-level simulations of the STCF MDC, and evaluate displaced-vertex sensitivities towards the protophobic boson, across the relevant mass-coupling parameter space. We study benchmark scenarios with visible and dark decay channels to perform likelihood-based significance estimates in order to determine the 5 discovery reach for the protophobic boson. We find that STCF can discover the protophobic boson while tolerating background events for specific regions of the parameter space around the 17 MeV peak. Our analysis establishes the first feasibility study of displaced light-boson searches at the STCF, motivating a full Geant-4 simulation.
Comments: 20 pages, 19 figures
Subjects: High Energy Physics - Phenomenology (hep-ph); High Energy Physics - Experiment (hep-ex)
Cite as: arXiv:2512.10084 [hep-ph]
On the new physics in Bhabha luminometry
at future 𝑒+𝑒− colliders
Clara L. Del Pio(1) and Francesco P. Ucci (2)(3)(∗)
(1) Department of Physics, Brookhaven National Laboratory, Upton, New York 11973, USA
(2) Dipartimento di Fisica ”Alessandro Volta”, Università di Pavia, Via A. Bassi 6, 27100
In Ref. [5], it was shown that the LNP contribution is negligible, being at most of the
order of 𝛿LNP ∼ 6 × 10−6 for the hypothetical 𝑋17 particle, whose existence is still under
scrutiny. Therefore, here we focus on the hypothesis of the new physics scale lying far
above the EW scale ΛNP ≫ ΛEW. In this scenario, the SM Lagrangian can be extended
with all possible higher-dimensional operators, built upon the same fields and symmetries
Saw the first article there. Wasn't convinced of its notability.
So people continue looking for their keys under the lamp post even though the keys were dropped a block away in the dark.
Worded another way, why is it not recognized that gravity wave detectors are dark matter detectors?
Hunting the elusive in CE NS at the ESS
Joakim Cederkäll, Yaşar Hiçyılmaz, Else Lytken, Stefano Moretti, Johan Rathsman
The so-called particle has been proposed in order to explain a very significant resonant behaviour (in both the angular separation and invariant mass) of pairs produced during a nuclear transition of excited Be, He and C nuclei. Fits to the corresponding data point, as most probable explanation, to a spin-1 object, which is protophobic and has a mass of approximately 16.7 MeV, which then makes the potentially observable in Coherent Elastic neutrino ( ) Nucleus Scattering (CE NS) at the European Spallation Source (ESS). By adopting as theoretical framework a minimal extension of the Standard Model (SM) with a generic gauge group mixing with the hypercharge one of the latter, which can naturally accommodate the state compliant with all available measurements from a variety of experiments, we predict that CE NS at the ESS will constitute an effective means to probe this hypothesis, even after allowing for the inevitable systematics associated to the performance of the planned detectors therein.
Subjects: High Energy Physics - Phenomenology (hep-ph)
Cite as: arXiv:2509.15128 [hep-ph]
Post a Comment