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3.5. Redshift Surveys: Defining Physical Structures

The previous manifestations of structure in the Universe were all based on the distribution of galaxies as projected onto the plane of the sky. This was the state of the field as of 1980. To make further progress it was necessary to move beyond projected galaxy distributions and into the realm of three-dimensional data sets. To do this necessitated the acquisition of galaxy redshifts. This is a somewhat daunting observational challenge. If the galaxies have lots of neutral hydrogen, then the Arecibo radio telescope will be able to detect that galaxy and get a redshift in approximately 10 minutes of observing time, for galaxies with velocities leq 10,000 km s-1. Unfortunately, the Arecibo telescope can only observe galaxies that are located between declinations of 0 and 40°. Nonetheless, throughout the 1980s, Arecibo staff astronomers, specifically Martha Haynes and Riccardo Giovanelli, measured redshifts for thousands of galaxies that are accessible in the Arecibo declination strip. Those observations were the first to define a large scale feature called the Pisces- Perseus supercluster (see Giovanelli and Haynes 1985; Giovanelli et al. 1986), which is a large, "sheet-like" structure with mean redshift 5500 km s-1.

Optical redshifts of galaxies can be much harder to obtain. If the galaxy has active star formation then it will be rich in emission lines from H II regions. Emission line redshifts require little integration time as only the emission line needs to be detected instead of the continuum light from the galaxy. In this case, using a telescope of diameter approx 1.5-m, a redshift can be obtained in about 5 minutes of integration time. Approximately 20% of all galaxies have sufficient emission line strength to allow for this rapid determination of redshift. For most galaxies redshifts must be determined from the absorption lines which come from the integrated contribution of all the stellar atmospheres in the galaxy. The principle absorption lines that can be detected are the H and K lines of Calcium at 3933 and 3963 Å, the Magnesium I line at 5175 Å and the Sodium D lines at 5800 Å. A typical absorption line spectrum of a galaxy is shown in Figure 3-9. On a 1.5 telescope an exposure time of 15-60 minutes is required to get sufficient signal-to-noise to determine an absorption line redshift. To get redshifts of thousands of galaxies in this manner required a dedicated telescope, patience, and an institutional commitment to performing this kind of service for the community.

Figure 3-9

Figure 3-9: A typical absorption line spectrum of a galaxy showing the many absorption lines in the spectrum. The principal lines used for redshift determination are the Calcium H and K lines at wavelength about 3900 angstroms, the Magnesium I complext at 5175 angstroms, and the sodium D lines at 5800 angstroms. Image courtesy of Jeff Willick.

These qualities were found in the form of Marc Davis, Steve Shectman and John Huchra at the Smithsonian Astrophysical Observatory. In the late 70's, Davis and Shectman designed a redshift machine for the 60-inch telescope at Mt. Hopkins. This spectrograph was optimized to detect the Mg I and Sodium D lines for purposes of determining a redshift and was known as the Z-machine. In 1979 this telescope plus detector was commissioned and the first redshift surveys were made. The pursuit of galaxy redshifts requires dedicated, patient and persistent observers. All of these qualities were found in Huchra and together with Davis, the performed the first redshift survey which contained approx 2500 galaxies brighter than b = 14.5. After this survey was completed, Margaret Geller joined the project and brought a fresh theoretical insight that allowed this rich data set to blossom into the first clear view and characterization of the 3D galaxy distribution. Much of this was based on a redshift survey of 20,000 galaxies brighter than b = 15.5. This basic dataset, known as the CFA Redshift Survey has been second only to the observations of the CMB in terms of its historic observational value to the field of cosmology. It is also safe to say that when this survey started, no astronomer could have predicted the complexity of the galaxy distribution that would be revealed by an obscure 1.5-m telescope located above the desert in Arizona.

The disadvantage of the CFA redshift survey instrumentation is that only one galaxy at a time could be observed. A revolution in galaxy redshift survey efficiency occurred in the mid 80's with the development of multi-fiber spectrography. In essence, galaxy coordinates are machined into a "plug-board" in which optical fibers are placed. Each optical fiber is fed to the spectrograph and the CCD detector. This allows for multiple objects to be observed in a single exposure. Multiple object spectrography can generally measure between 20 and 200 objects simultaneously which represents an enormous gain over the one galaxy at a time approach. Such an instrument is most valuable when measuring redshifts in a field where there are lots of galaxies. This could either be in a galaxy cluster or in some deep field where there are lots of faint galaxies. Initial work by Couch et al. (1985), Ellis et al. (1985), and Broadhurst et al. (1988) directly showed the tremendous advantage afforded by multiple object spectroscopy.

In tooling up to do the Southern Hemisphere equivalent of the CFA redshift survey, Steve Shectman took full advantage of multiple object spectroscopy and was able to measure as many redshifts that are in the CFA survey in a much shorter period of time. However, there are two potential problems with fiber-based spectroscopy:

bullet Since the fibers can not be put arbitrarily close together, there is a selection effect against detecting close pairs of galaxies.

bullet The S/N of the spectrum is extremely dependent upon the central surface brightness of the galaxy. A typical fiber has an angular extent of 1-5 arcseconds, depending upon the camera optics. Galaxies of low surface brightness are therefore greatly underrepresented in fiber surveys.

However, this two minor problems only impact studies of the small-scale clustering of galaxies. On a large scale, their impact is negligible.

There are now about 100,000 redshifts measured between the CFA survey and a complimentary survey initiated in the southern hemisphere a few years ago by Steve Shectman. In a few years, the Sloan Digital Sky Survey hopes to have measured 106 galaxy redshifts although its hard to believe this increase will significantly change the view of LSS that is presently defined by approx 100,000 redshifts.

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