Research Blog
Welcome to my Research Blog.
This is mostly meant to document what I am working on for myself, and to communicate with my colleagues. It is likely filled with errors!
This project is maintained by ndrakos
I have code that calculates the ionized bubble around each galaxy as a Strogrem sphere. The solution seems reasonable down to about redshift 8, where the bubbles stop growing as rapidly as I expect. This results in an ionized volume that is too low (see my last post).
Overall, I expect a characteristic size of about 100 cMpc by redshift 6 (see here), but am instead getting a characteristic size of about 1 cMpc.
I am considering the galaxies in between redshifts 6 and 6.5 in my “test” DREaM catalog (which only contains the most massive/brightest galaxies)
This is what the evolution of bubble sizes these sample galaxies look like:
Where the solution seems to run into problems is around redshift 8, which is where ionized bubbles should be overlapping.
I attempted to approximate how much individual bubble sizes should increase by adding a background in the calculation; i.e. \(f_{ esc} \dot{N}_{ion}\) became \(f_{ esc} \dot{N}_{ ion} + \dot{N}_{background}\), where \(\dot{N}_{background} = \dot{n} Q V\), \(Q\) is the ionized fraction and \(V\) is the volume of the bubble.
This seemed to increases the final bubble sizes by a factor of 2, which isn’t quite enough.
I am using an implicit Euler scheme which should be stable. Nethertheless, I tried increasing the time steps, and switched to integrating along points that were linearly spaced in \(a\), the scale factor. These changes did not make any difference.
The Yajima et al. 2018 paper considers adding a boost factor. That is, they artificially increase the radius by a factor, f \(R \rightarrow f R\). They state that \(f=2\), e.g., corresponds to 8 similar galaxies in the overlapped regions.
Following a similar idea, I considered a boost, such that the volume increases by an extra factor of \(V\) every time it overlaps with a bubble (where N is the number of bubbles)
If we consider a mean free path \(l\) in which we will hit a bubble of size \(R\), and assume all bubbles are of similar size, we can argue
\(\dfrac{R^3}{l^3} = \dfrac{Q}{1-Q}\) and \(n= \dfrac{1}{l \sigma} = \dfrac{1}{3V}\left(\dfrac{Q}{ (1-Q)}\right)\).
Therefore, at every timestep, when a bubble increases by volume \(dV\), I multiple the volume by \(1 + \dfrac{dV}{3V_i)}\left(\dfrac{Q(z)}{ (1-Q(z))}\right)\). In reality, the growth of the bubbles should be stochastic, with discrete jumps every time bubbles overlap. However, since I am only concerned with the final bubble size, I’m not too worried about getting an averaged growth history.
Here is the resulting bubble sizes (physical Mpc):
It’s a little hard to see what’s happening, since the bubble sizes tend to go to infinity. However, when I tested this same prescription with the galaxies between redshifts 7-8, I got a characteristic size of about 10 cMpc, which is around what I would expect. Therefore, I’m pretty happy with this method, and will run it on the full catalog and check the resulting ionization fraction.