mfb said:
What exactly rules out a possible discovery by XENON1T and its follow-up experiments?
Some of sub-GeV mass range is also
excluded by direct searches at the LHC. The latest LHC results even strictly limit
Higgs channel dark matter candidates.
Equally important, if the kind of dark matter that these direct dark matter detection experiments are looking for exists, it would behave in a very particular way that would be reflected in its behavior that can be indirectly observed with astronomy observations such as rotation curve and lensing measurements of inferred dark matter halos. The behavior of the kind of dark matter sought is also the single most well modeled scenario in N-body simulations of dark matter.
For example, generically, dark matter of the kind that could could be found by XENO1T and its follow-up experiments would generate the wrong shaped/wrong density distribution halos (something that baryonic feedback mediated only by gravity and weaker than neutrino weak force interactions
can't alleviate), would
not be able to reconcile measurements based upon rotation curves and those based upon lensing, would
not track baryonic matter distributions as tightly as observation indicates, would
not generate particle velocities sufficient to give rise to the number of observed high velocity galactic cluster systems of which the Bullet Cluster is an example, and would generate more small scale structure (such as satellite galaxies) than is observed by astronomers.
Some of these problems are summarized in a literature review supported by references from
this preprint (references fully described in end notes in the original, paragraph breaks inserted for ease of reading in this non-typeset format):
At the galactic scale masses of M < 1011−12M , the predicted WIMP/ΛCDM dark matter halos are much more numerous than those detected and show very different structural properties with respect to those inferred by the internal motions of galaxies (e.g. see Salucci, F.-Martins & Lapi (2011)). The questioning issues for the WIMP particle are well known as the “missing satellites” ( Klypin et al. (1999)), the “too big too fail” (Boylan-Kolchin et al. (2011)) and the lack of a cuspy central density profiles in the DM halos (Gentile et al. (2004); Spano et al. (2008); Oh et al. (2011) and reference therein).
There are proposals in which astrophysical processes could modify the predictions of the N-body ΛCDM models and the related density profiles to fit the observations (e.g. Vogelsberger et al. (2014); Pontzen & Governato (2012); Di Cintio et al. (2014); Read, Agertz, & Collins (2016)). However, this modelizations are growing in number and in diversity (Karukes & Salucci (2016)) and the cores formation via hypothetical strong baryonic feedbacks requires ad hoc fine tuning.
Let us also remind that WIMP particles have not convincingly been detected in underground experiments (see e.g. Freese (2017)) and they have not emerged even in the most energetic LHC proton-proton collisions (e.g.CMS collaboration (2017)).
Finally, the X and gamma ray radiation coming from annihilating WIMP particles at the center of our and nearby galaxies has not unambiguously been detected ( Freese (2017), e.g. Albert et al. (2016); Lovell et al. (2016)). Thus, to claim that ΛCDM is not anymore the forefront cosmological scenario for dark matter will bring no surprise.
Recent alternative scenarios for dark matter point to a sort of significant self-interactions between the dark particles which seems suitable to explain the observational evidence which has created the ΛCDM crisis. Among those, the Warm Dark Matter, the axion as a BoseEinstein condensate and the self-interacting massive particles scenario (e.g. Freese (2017); Krishna et al. (2017); Suarez et al. (2014); de Vega, Salucci, & Sanchez (2014)) are the most promising. Their common characteristic is that, at galactic scales, dark matter stops to be collisionless and it starts to behave in a way which could make it compatible with observations. However, also these scenarios hardly explain the fact that we continue to find that in galaxies, dark and luminous matter are extremely well correlated (e.g. Gentile et al. (2009)). . . . In fact, the dark-luminous coupling that emerge in spirals is so intricate that it is extremely difficult to frame it in a scenario in which the dark and the luminous galactic components are completely separated but through their gravitational interaction.
(At the large scale structure/CMB/lamda CDM scale, the Standard Model of Cosmology is insensitive to the details of dark matter particle properties from wark dark matter in the roughly keV scale all of the way up to brown dwarf sized MACHOs and stellar black holes, so long as it is very nearly collisionless.)
The noise created by the neutrino background which currently can't be effectively filtered out, undermines the methodology of these experiments long before they have enough resolution to detect warm dark matter that might behave differently in the respects described above.