Who knows? It is not science' job to answer the question "why does existence exist?"
Cosmology progresses by asking and investigating questions that are TIMELY in the sense of being RIPE to be answered based on what we currently know and are able to observe. Now these particular researchers (like Ed Wilson Ewing) are focusing on OUR PARTICULAR START OF EXPANSION.
The idea of a "singularity" is kind of absurd, a symptom of the breakdown of a 1915 theory that doesn't allow for quantum effects. So what
really
happened at the start of expansion.
So you make a model involving some quantum effects in basic GR and you run it back in time and instead of a blowup, failure, "singularity" glitch you see it rebound and expand out again going back in time. So you see a prior collapse phase that rebounds.
you don't ask where that came from because that is not a ripe question to be addressed. the aim is to understand a particular event, the start of expansion, and to derive predictions. Can you model it so that it fits the observational data? Can you get a SIMPLER best fit model?
Maybe with this new model you can get the observed EFFECTS OF INFLATION without having to postulate an exotic "inflaton" field that conveniently dies away when it has smoothed things out just the right amount. maybe the smoothness is inherited from a prior contracting phase aided by the bounce mechanism itself. Interesting possibility. Let's study it.
Seriously MyKK, how about giving this 14 page paper a try. It has some non-technical parts and I think it exemplifies the best in bounce cosmology (the most empirical/observational) at the moment. I'm a Wilson-Ewing fan.
http://arxiv.org/abs/1412.2914
A ΛCDM bounce scenario
Yi-Fu Cai,
Edward Wilson-Ewing
(Submitted on 9 Dec 2014 (
v1), last revised 28 Jan 2015 (this version, v2))
We study a contracting universe composed of cold dark matter and radiation, and with a positive cosmological constant. As is well known from standard cosmological perturbation theory, under the assumption of initial quantum vacuum fluctuations the Fourier modes of the comoving curvature perturbation that exit the (sound) Hubble radius in such a contracting universe at a time of matter-domination will be nearly scale-invariant. Furthermore, the modes that exit the (sound) Hubble radius when the effective equation of state is slightly negative due to the cosmological constant will have a slight red tilt, in agreement with observations. We assume that loop quantum cosmology captures the correct high-curvature dynamics of the space-time, and this ensures that the big-bang singularity is resolved and is replaced by a bounce. We calculate the evolution of the perturbations through the bounce and find that they remain nearly scale-invariant. We also show that the amplitude of the scalar perturbations in this cosmology depends on a combination of the sound speed of cold dark matter, the Hubble rate in the contracting branch at the time of equality of the energy densities of cold dark matter and radiation, and the curvature scale that the loop quantum cosmology bounce occurs at. Importantly, as this scenario predicts a positive running of the scalar index, observations can potentially differentiate between it and inflationary models. Finally, for a small sound speed of cold dark matter, this scenario predicts a small tensor-to-scalar ratio.
14 pages, 8 figures.