Plotting Examples

There are a variety of methods that can be used to visualize a network.

import pynucastro as pyna

Standard view

Let’s build a quick network that represents He, C, and O burning

library = pyna.ReacLibLibrary()

sub = library.linking_nuclei(["p", "n", "he4", "c12", "n13", "n14", "o16",
                              "ne20", "ne21", "na23", "mg23", "mg24", "al27",
                              "si27", "si28"])
rc = pyna.RateCollection(libraries=sub)

/opt/hostedtoolcache/Python/3.11.11/x64/lib/python3.11/site-packages/pynucastro/networks/rate_collection.py:576: UserWarning: ReacLib neutron decay rate (<n_to_p_weak_wc12>) does not account for degeneracy at high densities. Consider using tabular rate from Langanke.
  warnings.warn(msg)

The standard network plot of this is:

fig = rc.plot()

Ignoring fixed x limits to fulfill fixed data aspect with adjustable data limits.

Rotated view

Since everything lies close to the diagonal, it is hard to see the structure. We can instead look at a rotated view of the network.

While we’re at it, we’ll also color the rates by reaction rate strength

rho = 1.e4
T = 1.e8
comp = pyna.Composition(rc.get_nuclei())
comp.set_solar_like()

fig = rc.plot(rho, T, comp, rotated=True)

This looks a bit crowded, since it is showing all of the links to \({}^4\mathrm{He}\) from reactions of the form \(A(x, \alpha)B\). We can hide those links with hide_xalpha=True

fig = rc.plot(rho, T, comp, rotated=True, hide_xalpha=True)

We can also plot the edges curved, to help distinguish the forward and reverse rates

fig = rc.plot(rho, T, comp, rotated=True, hide_xalpha=True,
              curved_edges=True)

We can also label edges if desired

edge_labels = {(pyna.Nucleus("he4"), pyna.Nucleus("c12")):
               r"$\alpha(\alpha\alpha,\gamma){}^{12}\mathrm{C}$"}

fig = rc.plot(rho, T, comp, rotated=True, hide_xalpha=True,
              edge_labels=edge_labels, size=(1200, 700),
              curved_edges=True)

Filters

We can use a rate filter to show only certain links. For example, to show only links involving proton capture, we can do:

fig = rc.plot(rho, T, comp, rotated=True, hide_xalpha=True,
              rate_filter_function=lambda r: pyna.Nucleus("p") in r.reactants)

We can also highlight rates using the highlight_filter_function mechanism. This takes a function that operates on a rate and returns True if we wish to highlight the rate (i.e., as if we used a highlighter marker over the line).

Here’s an example where we highlight the rates that have \(Q > 0\)

fig = rc.plot(rotated=True, hide_xalpha=True, size=(1500, 600),
              highlight_filter_function=lambda r: r.Q > 0,
              curved_edges=True)

Plotting the Jacobian

For implicit integration, we solve:

\[\dot{\bf Y} = {\bf f}({\bf Y})\]

and the Jacobian, \({\bf J} = \partial {\bf f} / \partial {\bf Y}\) plays an important role in solving for the update.

We can visualize the Jacobian of our network easily. By default, we will show all elements where

$$\frac{\mathrm{max}{i,j} (|J{ij}|)}{|J_{ij}|} > 10^{10}$$

but this ratio can be set via the rate_scaling keyword argument.

rho = 1.e4
T = 2.e9
comp.set_equal()
fig = rc.plot_jacobian(rho, T, comp, rate_scaling=1.e10)

Note

If you set rate_scaling too large, then roundoff error in mapping the Jacobian elements to colors can cause elements that are zero to appear colored. It is best to stay below 1.e15 to minimize roundoff.

Plot nuclides on a grid

Nuclides in a network may also be visualized as cells on a grid of Z vs. N, colored by some quantity. This can be more interpretable for large networks.

Calling gridplot without any arguments will just plot the grid – to see anything interesting we need to supply some conditions. Here is a plot of nuclide mass fraction on a log scale, with a 36 square inch figure:

rate_names = ["c12(p,g)n13", 
              "c13(p,g)n14",
              "n13(,)c13",
              "n13(p,g)o14",
              "n14(p,g)o15",
              "n15(p,a)c12",
              "o14(,)n14",
              "o15(,)n15"]
rates = library.get_rate_by_name(rate_names)
rc = pyna.RateCollection(rates=rates)

rho = 1.e4
T = 1.e8
comp = pyna.Composition(rc.get_nuclei())
comp.set_solar_like()

fig = rc.gridplot(comp=comp, color_field="X", scale="log", area=36)

The plot is configurable through a large number of keyword arguments. Here we want to look at the rates at which nuclides are being created or destroyed, so we color by \(\dot{Y}\), the rate of change of molar abundance. Density and temperature need to be supplied to evaluate the rates. A full list of valid keyword arguments can be found in the API documentation.

fig = rc.gridplot(comp=comp, rho=rho, T=T, color_field="ydot", area=36,
                  cmap="RdGy", cbar_bounds=(-0.1, 0.1))

Unlike the network plot, this won’t omit hydrogen and helium by default. To just look at the heavier nuclides, we can define a function to filter by proton number. Here we also plot activity, which is the sum of all rates contributions to Ydot ignoring the sign.

ff = lambda nuc: nuc.Z > 2
fig = rc.gridplot(comp=comp, rho=rho, T=T, color_field="activity", scale="log",
                  filter_function=ff, area=20, cmap="Blues")

Network chart

A network chart shows how each rate affects each nucleus

fig = rc.plot_network_chart(rho, T, comp)