The Matter with Dark Matter

 

Abstract

 

Over the decades the dark matter problem, if anything has become more mysterious. The problem lies in that the existence of dark matter is inferred solely from its gravitational effects. In recent years there has been an alternative to dark matter for explaining these gravitational effects. Know as Modified Newtonian Dynamics (MOND) it describes the motion of bodies in a gravitational field by assuming that in the limit of small accelerations () Newton’s second law does not accurately describe an objects motion. Though these two ideas have some promising results, they come from studying rotation curves of many individual galaxies or the dynamics of galaxy clusters having thousands of members. In this investigation I will examine the gravitational effects beyond the optical radius of galaxies by looking at velocities of satellites orbiting isolated galaxies in the same way one looks at the velocities of stars in a galaxy. Using the Sloan Digital Sky Survey (SDSS) I will be able to look at over 1 million galaxies which will give us a sample size needed for such a study. By knowing how gravity works between galaxies together with how it works within galaxies may provide new insight about MOND, to what dark matter is, or may turn up something completely new.


Background

 

The discovery by Zwicky (1933) that visible matter accounts for only a tiny fraction of all of the mass in the universe may turn to have been one of the most profound new insights produced by scientific exploration during the 20th century. From observations of the radial velocities of eight galaxies in the Coma Cluster, Zwicky found an unexpectedly large velocity dispersion, . Zwicky concluded that the mean density of the Coma Cluster would have to be 400 times greater than that which is derived from luminous matter for a velocity dispersion of 1000 km/s. Six years later, Babcock (1936) obtained long-slit spectra of the Andromeda galaxy, which showed that the outer regions of M31 were rotating with an unexpectedly high velocity, indicating either a high outer mass-to-light ratio or strong dust absorption. These observations indicated that the mass in the outer regions of the Andromeda galaxy increased with distance from the center of the galaxy, even though the optical luminosity of M31 did not. From these observations Roberts & Whitehurst (1975) concluded that the mass-to-light ratio had to be  in the outermost regions of the galaxy. This together with papers on the stability of galactic disks by Ostriker & Peebles (1973), and that the mass of a galaxy increases with increasing radius (Ostriker, Peebles, & Yahil 1974), first convinced the majority of astronomers that missing mass existed. Ostriker & Peebles (1973) concluded that instabilities in galaxy disks could be prevented by a massive spherical “halo” component (Bergh 1999).

 

By the mid 70’s the majority of astronomers were convinced that unseen mass existed in the universe. However, it was unknown what form the mass took, whether it was late M dwarfs, brown dwarfs, white dwarfs, black holes, very hot gas or in some other unknown form. In the late 70’s it was not clear that a paradigm shift (Kuhn 1962) would be required to interpret the new observations that seemed to support the ubiquitousness of missing matter in the universe. It had also been speculated that such a paradigm shift might not be required if Newton’s Laws break down at small accelerations (Milgrom & Bekenstein 1987).


Scientific Research

 

Estimates of the dark matter halo of galaxies are made with rotation curves. These rotation curves can rarely be measured beyond about twice the optical radius. Detection of the extended dark matter halo requires dynamical probes well beyond the optical radius. Satellite galaxies have provided a unique dynamical probe well beyond the optical radius of the central "primary" galaxy (Prada et al. 2003). While the inner parts of galaxy halos have density distributions that yield approximately flat rotation curves (example shown below), our understanding of the profile at larger distances is much poorer. The

 

(Top) Three parts of a galaxy. (Bottom) Example of a rotation curve showing the radial velocity becomes constant at large radii

 

issue is critical because the density profile that gives rise to a flat rotation curve () is different from that predicted by cosmological models (NFW Navarro, Frenk, & White 1997) at larger distances (or - Newtonian). A method to probe the mass distribution at large radii is to look at the velocities of satellites of a galaxy. However, because the number of detectable satellites around galaxies outside of the Local Group is small, one needs to study many galaxies to accumulate enough statistics to study the profiles of other galaxies. As a result, observational efforts to study the dynamics of satellites have been some what limited (Erickson, Gottesman, & Hunter 1987; Zaritsky et al. 1993; Zaritsky & White 1994; Zaritsky et al. 1997; McKay et al. 2002). Early results were obtained by Zaritsky et al. (1993), Zaritsky & White (1994) and Zaritsky et al. (1997), who compiled and studied a sample of about 100 satellites of nearby isolated spiral galaxies with an average of 1–2 satellites per primary galaxy. It was found that the line-of-sight velocity dispersion of the satellites does not decline with the projected distance to the primary galaxy. This result has been generally considered a strong argument for the presence of dark matter at large distances (~200–400 kpc) from the galaxy center. Zaritsky & White (1994) also found that the satellite velocity dispersion does not correlate with the luminosity of the primary galaxy (Prada et al. 2003).

 

Prada et al. used SDSS data to plot the line-of-sight velocity differences of satellites for primaries in the magnitude range -19.5 < MB < -20.5 (sample 1). This plot is shown below as well as one reproduced by me. The dashed curve shows the r.m.s. velocities for raw data with no interlopers removed. The full curve shows theoretical prediction for equilibrium NFW halo with mass.

 

 (Left) from Prada et al. (2003). (Right) my plot.

 

They also plotted a second sample with magnitude range -19.5 < MB < -20.5. This plot is shown below. We do not agree in what the velocity dispersion should be at larger radii. The dashed curve shows the r.m.s. velocities for raw data with no interlopers removed. The full curve shows theoretical prediction for equilibrium NFW halo with mass.

(Left) from Prada et al. (2003). (Right) my plot.

 

The reasons for the disagreement between plots is not known, which gives another reason that more work needs to be done on this method.


Expanding on the Scientific Research

 

Deciding which galaxies around a primary galaxy are truly satellites can be improved by knowing their morphology classifications. In the past, most of morphology classification was done visually. In recent years the vast amount of data produced by large surveys (such as SDSS, NED and 2MASS) has made visual inspection a daunting task. One potential solution to this problem is to automate galaxy classification using a neural network trained to distinguish patterns and relationships using various photometric indexes. We will present preliminary galaxy classification results using this method.

 

 


Reference

 

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Ostriker, J. P., and Peebles, P. J. E., and Yahil, A. 1974, Apj, 193, L 1

Kuhn, T. 1962, The Structure of Scientific Revolutions (Chicago: Univ. Chicago Press)

Milgrom, M., and Bekenstein, J. 1987, in IAU Symp. 117, Dark Matter in the Universe,

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