Hubble Diagram is probably the most traditional of cosmological test. It plots relative luminosity distance sources as a functional derived shift. In earlier on the brightest things that astronomers could think of to look at the brightest cluster galaxies, they can be detected out to [UNKNOWN] from using the technology available at that time, that there are not to be quite far enough to really sense cosmological effects. But moreover the problem was that galaxies had been made out of stars, evolve, because stars evolve. And, moreover, they merge, so their total stellar mass increases. And so by the 1980's, it became clear, that Hubble diagram for galaxies, is basically an impossible task. Because the evolutionary effects really dominate over any cosmological effect. The difference between different evolutionary models is much larger than between any plausible range of cosmological models. Supernovae were also suggested as standard candles, as early as the 1960's by [UNKNOWN] collaborators. But back then, nobody knew how to make them standard enough for this purpose. The revival of this test came in mid 1990s, where astronomers learned how to standardize brightness of supernovae in the ways that we covered earlier in the class. And because they can be seen further away telescopes are bigger and detectors are better, suddenly they became a viable cosmological test again. Do note that some uncertainties still remain about the origin of, of supernova type 1a and exactly what happens in those explosions, but astronomers strive to come up with tests to control all possible systematics. We do see some variation for light curves but most of it can be then taken out through standardization procedures. The some remaining questions such as whether there is an additional parameter, there is an evolution and there are hints that indeed such things do happen, but at such a subtle level they do not affect the cosmological results. Still, keep in mind these are Messy stellar explosions which we can barely model in computers today. And the more realistic the models would get, the more complicated they look. So it's still possible that some additional uncertainties might be present using supernovae standard [UNKNOWN]. These are examples of images of some of the very distant super novae taken with Hubble space telescope. This is just to indicate how difficult these observations are. Not only do these faint supernovae have to be discovered, they have to be discovered early, their light curves mapped, their red shifts obtained, all of the different corrections applied, and only then they can be used in Hubble diagram. All of this requires a lot of effort by the best people and the best equipment that we have. Anyway, that was done in mid 90's, by 2 groups working independently. One was the supernova cosmology project, at Lawrence Berkeley Lab, led by Saul Perlmutter, and the other one, was, High redshift Supernova Team, led by Brian Schmidt, and Adam Riess. The 2 groups, essentially produced the same result, at roughly the same time. And more or less, independent. They both found out, that the high redshift supernova Hubble diagram, requires introduction of the cosmological constant or vacuum energy density in order to fit the data. Whereas, there was a lot of circumstantial evidence for cosmological constant prior to that. This was the first time that majority of physicists really started paying attention and taking this possibility seriously. Here we see Hubble diagrams with the main trend line subtracted a particular model subtracted and then residuals fit for variety fodder models. The model that fits the data best, is the one that includes cosmological constant, at a level of approximately 70% of critical density. This was a spectacular result, and the 3 leaders of the groups, deservedly got Nobel Prize, for that work. Although, again, it's important to point out, that These are large, team efforts, and not necessarily reducible to a handful of individuals. This is how science today operates. Here is the Hubble diagram replotted now in the original traditional sense of scale factor versus time. And so, the points extend to the past, you can see that they select a particular curve And that curve, corresponds to, cosmological constant, driven universe, that expands forever. Many other groups, have undertaken this work since then, and they all pretty much agree. The results just get better, and better. Here is an example of one of the more modern High redshift supernova Hubble diagrams, and colors of points correspond to those, from different groups. As you can see, there is an excellent mutual agreement, and the signal to noise is really getting to be very good. So this was the upshot, of the supernova Hubble diagram. On the plot of Critical dense, I'm, on the plot of, density parameters, matter on the x-axis and vacuum or cosmological constant on the y-axis. The measurements define an error ellipse, which is tilted and the plot universe corresponds to a diagonal straight line, as shown here. They do intersect and intersect roughly at density of matter of .3 for critical density and density vacuum about 0.7 for critical density. So this is the 1st time it was possible to say that if the universe was flat, then there must be a cosmological constant. But note that these error ellipses are pretty large and they do not really nail down the exact cosmological model. The zero value of cosmological constant is sufficiently far from the best fit that it can be excluded. But exactly what mixture of vacuum density and matter densities at play had to be determined using some other method. An interesting twist to this is to use cosmic gamma ray bursts as alternative standard candles, these are even more spectacular explosions. But it turns out, that their gamma variable luminosity can be also standardized to a nearly constant value using a variety of other parameters. At any rate, it's an independent test on what supernova results are and here are the error contours from gamma ray bursts alone. There are bigger than those from supernovae because gamery versus not quite a good standard candle but they produce more or less the same result. Now few words about the other classical cosmological test, the angular diameter test. Here we compare relative angular diameter distances to source as the different [UNKNOWN], and in the past things like isophotal sizes of giant elliptical galaxies, mean seperation of galaxies in clusters, or seperation of radio lobes in radio sources, we're all suggested that as standard rulers. And non of them really is for the same reasons as before evolution. Here is some of the earlier results trying to do that and interestingly enough all of these have also in consistent in what we now know is the correct cosmology. But People simply could not be sure, because of the evolutionary effect that was not well understood at the time. This test got revived through the cosmic microwave background. And it's probably now the most important of all of our tools. So next time we will talk about cosmology Cosmic microwave background fluctuations. What really led us into the era of precision cosmology.