- #36
ohwilleke
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kimbyd said:From one of the papers you cited:
https://arxiv.org/abs/1407.7544
That last part of the sentence is critical. Baryonic behavior for compact systems is monumentally, absurdly complicated. Both supernovae and high-mass black holes can have galactic-scale impacts, and both have massive modeling problems.
The specific reason why they focus on faint dwarf galaxies is because these systems are likely to be less-impacted by such things. But even there the simulations are both complicated and highly contingent on uncertain initial conditions.
First, the dark matter phenomena, from which a dark mater halo could be inferred, in faint dwarf galaxies, was accurately predicted with MOND about 35 years ago. It was one of the very first predictions made by the theory.
Second, as noted by Brooks, a lot of progress has been made since 2014 in modeling self-interacting dark matter with baryonic effects. She has noted this in at least one of her papers.
Third, if the simulations are both complicated and highly contingent on uncertain initial conditions, why isn't the observed outcome of those processes more complicated or more diverse?
If all of the data in a range of applicability from binary star systems to the largest individual galaxies and systems of central galaxies and galaxy satellites can be explained with a one line non-relativistic formula and a single parameters, then either (1) the universe is extremely finely tuned in advance at high Z to fit every known galaxy, or (2) your model is missing something really huge because none of that complexity or formation history matters in influencing the relationships of bodies in these gravitationally bound systems. I respectfully suggest that option 2 and not option 1 has to be correct.
We know, as a matter of rigorously demonstrated empirical fact that 100% of effects attributed to dark matter at galaxy or galaxy-satellite galaxy system scales or less can be fully described from the current distribution of baryonic matter, a single universal physical constant, and a one line formula, without any regard to the history of the formation of that gravitationally bound system. The magnitude of the observed deviations from this relationship are, in every case, no greater than measurement error (not all astronomy measurements, especially of very distant objects, are terribly precise). There are NO OUTLIERS!
We also know with very high confidence that none of the three Standard Model forces (electromagnetism, the strong force, and the weak force) has anything to do with this relationship, and that the observed effects can not be explained by General Relativity without resorting to either dark matter particles, or a gravitational modification (including "fifth forces" that interact with baryonic matter), or some combination of the two.
This is a big problem for dark matter particle theories.
Generically, in any theory with dark matter particles that form halos that give rise to dark matter phenomena, the history of how a galaxy came to be formed should matter. There is no reason in a dark matter particle theory why a galaxy with a more or less identical distribution of baryonic matter to another galaxy should have exactly the same dark matter halo, unless you formulate an additional second theory that explains that. But, the observational reality is that this that a system's formation history is irrelevant to the behavior of gravitationally bound systems.
Indeed, while the absurdly simple MOND formula does not generalize to galactic clusters, even there, the dark matter phenomena which are observed can be discerned from the baryonic matter distribution in the galactic cluster alone, albeit, with a different relationship. This can be hypothesized in terms of a formation process, but it is experienced as a set of tight phenomenological relationships between baryonic matter distributions and inferred dark matter halo size and shape.
We study the total and dark matter (DM) density profiles as well as their correlations for a sample of 15 high-mass galaxy clusters by extending our previous work on several clusters from Newman et al. Our analysis focuses on 15 CLASH X-ray-selected clusters that have high-quality weak- and strong-lensing measurements from combined Subaru and Hubble Space Telescope observations. The total density profiles derived from lensing are interpreted based on the two-phase scenario of cluster formation. In this context, the brightest cluster galaxy (BCG) forms in the first dissipative phase, followed by a dissipationless phase where baryonic physics flattens the inner DM distribution. This results in the formation of clusters with modified DM distribution and several correlations between characteristic quantities of the clusters. We find that the central DM density profiles of the clusters are strongly influenced by baryonic physics as found in our earlier work. The inner slope of the DM density for the CLASH clusters is found to be flatter than the Navarro--Frenk--White profile, ranging from α=0.30 to 0.79. We examine correlations of the DM density slope α with the effective radius Re and stellar mass Me of the BCG, finding that these quantities are anti-correlated with a Spearman correlation coefficient of ∼−0.6. We also study the correlation between Re and the cluster halo mass M500, and the correlation between the total masses inside 5 kpc and 100 kpc. We find that these quantities are correlated with Spearman coefficients of 0.68 and 0.64, respectively. These observed correlations are in support of the physical picture proposed by Newman et al.
Antonino Del Popolo et al., "Correlations between the Dark Matter and Baryonic Properties of CLASH Galaxy Clusters" (August 6, 2018) (the prior works by Newman, et al., being extended are A. B. Newman, T. Treu, R. S. Ellis, D. J. Sand, C. Nipoti, J. Richard, and E. Jullo, The Density Profiles of Massive, Relaxed Galaxy Clusters. I. The Total Density Over Three Decades in Radius, ApJ 765 (Mar., 2013) 24, [arXiv:1209.1391] and A. B. Newman, T. Treu, R. S. Ellis, and D. J. Sand, The Density Profiles of Massive, Relaxed Galaxy Clusters. II. Separating Luminous and Dark Matter in Cluster Cores, ApJ 765 (Mar., 2013) 25, [arXiv:1209.1392]).
The problem with a dark matter particle theory is not that the reality is too complicated to model. The problem is that far too many factors, that should matter, turn out to be completely irrelevant in practice for reasons that no one has yet managed to articulate.
Note, to be clear, I'm not saying that it is impossible that there is some process of galaxy formation that does produce such a tight relationship. But, whatever that process is, it simply can't be that complicated and it absolutely can't be very initial conditions dependent. If it is a chaotic system as that term is defined in mathematics (i.e. end states are highly sensitive to initial conditions) it has to be one with a very strong attractor to the MOND relationship. Any theory that lacks that property is wrong.
Therefore, the claim that galaxy formation is too complicated so dark matter particle theories should be excused for not having a galaxy formation theory that accurately predicts dark matter halo shapes and sizes falls on deaf ears.
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