tim9000 said:
So what's the difference between the 'light cone' and the Hubble sphere?
Light cones trace the path of signals (light) traveling through spacetime. A past light cone with the tip at the observer (i.e. here and now) shows the path of all signals that you're seeing now. If you e.g. look at where the line of a lightcone crosses with the dotted line representing redshift z=1:
you can see where in the spacetime the emitter was. That is, at what time the presently observed signal of a z=1 galaxy was emitted, and how far it was at the time of emission. At the time of observation (apex of the light cone) you can't see anything outside the light cone shown, and you have seen everything inside the light cone at some time in the past.
In a static, non-expanding space light cones would look like straight lines forming a triangle, i.e. like this:
(or a cone, if you use 2+1 dimensions rather than 1+1, hence light
cone). If the space is expanding, those nice triangular light cones get distorted into what you see on the first graph. But notice that as the lines converge on the observer, where expansion is less and less significant, it looks more and more triangular in shape.
A triangular light cone in a static universe would expand to cover arbitrary large distance - as you draw triangles with vertices at successively further times (higher on the t axis), the base gets progressively and indefinitely larger. This means that in a static universe you could see signals from arbitrarily far away, as long as you waited long enough for the signal to reach you.
In expanding universes, the distorted light cones also grow indefinitely in time, but, not being triangular, their bases don't cover arbitrarily large distances.
Here's an animation of how light cones evolve in our expanding universe:
http://yukterez.net/lcdm/lcdm-flrw-animation.gif
(taken from:
http://yukterez.net/)
(Hmmm, something's wrong with the gif. I'll see if I can fix it - in the meantime, the animation can be seen here:
http://yukterez.net/lcdm/i.html#plot)
The one on the right is the exact same graph, only drawn in different coordinates that allow us to better see what's going on at the base of the graph. The comoving distance scale can be understood as proper ('regular') distance at the present time, and to translate it to proper distance at any other time, it has to be multiplied by the scale factor 'a' shown on the right (growing from 0 to infinity), so that the base of the graph, despite being so splayed, actually represents very short proper distances (and the top shows very far ones).
The Hubble sphere, on the other hand, is just a sphere with a radius marking recession velocity equal to the speed of light. It is quite unrelated to a light cone.
tim9000 said:
So we can see superluminal recession because the Hubble sphere is expanding toward the light, but I'm still having trouble understanding the diagram, why is the event horizon a region and not completely to the right and left outside the Hubble Sphere?
I don't think the dashed area is meant to convey anything special, apart from 'colour'-coding the graph for ease of use. The horizon is definitely just the outer line, not the whole area.
tim9000 said:
Why/how is the event horizon asymptotic at 17.3 b yrs?
This has to do with the dark energy content in the universe. There is a certain (constant as per the LCDM) density of dark energy per unit volume of space in our universe, and that determines how far away the horizon will be.
If not for all the matter and radiation in the universe, i.e., if we had an universe with dark energy only, there would be no asymptotic approach of the horizon to that value, but it'd be exactly that, forever. It would also be equal to where the Hubble radius (aka sphere) would be, since without any matter or radiation to 'pull' everything together and slow the expansion down, anything (a test point of sorts, since there's no galaxies in this universe) finding itself receding more rapidly than c, would never be able to send a signal to the observer.
As the universe expands and radiation and matter get diluted, their meddling influence on what dark matter 'wants' the universe to expand like gets diminished. That's why in the far future (infinity), when matter and radiation densities approach zero, the event horizon, as well as Hubble radius approaches the value they'd have without any matter or radiation.