This is a guest post by Ketron Mitchell-Wayne, graduate student at the University of California-Irvine. He and other CANDELS team member recently published a paper in Nature. This paper was the subject of a recent press release. Here, Ketron describes the project and the role that he played.
The cosmic extragalactic background light is a product of many different component emissions throughout all cosmic times. Recent CANDELS observations have opened up a new window of opportunity for measuring this cosmic background light at optical and near infrared wavelengths. We have assembled Hubble frames taken over a 10 year period and mosaiced them to produce some of the deepest images suitable for such a study. With the mosaics, we can study this diffuse, clumpy light that resides behind all the resolved stars and galaxies in the mosaics. With statistics, we have attributed a fraction of this diffuse background to the first light galaxies during reionization. Here's a short summary of the work that I did, over the course of two years, in order to make these very interesting measurements.
My main job for this paper was generating the 
mosaics and making the statistical measurements. I started working on 
the data reduction in the summer of 2013 and have spent the better part 
of the last two years working on the project. Anton Koekemoer had a data
 reduction pipeline set up for all the incoming CANDELS data, but I 
wanted to incorporate archival data in our analysis too. So I had a 
number of reduction steps to complete on thousands of frames, even 
before making the mosaics (which is in itself very difficult).
Once
 we had mosaics in multiple bands (left panel of Figure 1), I generated a source mask. We want to
 isolate the background light signal, so foreground stars and galaxies 
need to be removed from the image. The dark areas in the second panel of
 Figure 1 is the source mask (just zeros in the array).
At
 this point I could start making statistical measurements of the 
background light in the mosaiced, source-subtracted maps. The methods we
 used aren't new, but much of the dataset was. We used a very similar 
method to what was used in the Cosmic Microwave Background (CMB) 
studies. We look at "empty pixels" (what's left over after source 
removal) and measure whether or not some group of pixels in one part of 
the image is correlated with another group of pixels in a different part
 of the image. This is the angular power spectrum, which quantifies 
these correlations, as a function of angular scale. This is exactly what
 the CMB team did to measure the microwave background power spectrum, 
which is paramount in our understanding of cosmology. 
I
 made maps in five different wavelength ranges, or "bands": 0.6, 0.7, 
0.85, 1.25 and 1.6 microns. The shortest band is in the yellow range of 
visible light, and the longest two are in the near-infrared (NIR), which
 our eyes aren't sensitive to. This wavelength range (1 micron) is 
special because it is sensitive to Lyman break signatures with a 
multi-wavelength study, and it is the wavelength at which we expect a 
signal from the reionization epoch. Figure 2 shows the brightness of the 
background light in each of these bands. Each of the bands has a common 
component - what we call "intrahalo light" - which is the light emitted 
by stars which have been tidally stripped from their host galaxies via 
mergers or interactions. But in Figure 2 you can see that the brightness drops 
significantly from the two NIR bands to the shorter bands. We think this
 is because the NIR bands are picking up, in addition to intrahalo 
light, a high-redshift signal from the first light galaxies. Because the
 photons from the reionization era have been redshifted by a factor of 
about 10, we expect their signal to peak between 0.9 and 1.1 microns, 
with no shortward contribution below the Lyman break at about 0.8 
microns.
We're studying the background light, 
which traces emission from many different kinds of sources over all 
cosmological times. So we don't have a direct image of only the first 
galaxies. With sophisticated modeling, we were able to separate the 
different component emissions, and isolate the signal from the first 
galaxies. So what we have, via statistical methods, is a description of 
the astrophysical environment 500 million years after the big bang. The 
third panel in Fig 1 is a reconstruction of what they would look like 
based on our statistical measurements. Cosmological theory suggests that
 these first light galaxies are the progenitors to our milky way, and 
all other evolved galaxies.


 
 
