Lab Goals#

Our goal is to model nuclear processes in an accreting O/Ne white dwarf to understand temporal evolution (and ultimately whether the white dwarf can explode).

We need to understand some concepts from astronomy:

  • Electron degeneracy and the equation of state

  • The structure of white dwarfs

  • Nuclear reactions, including strong-mediated and weak-interactions (like electron-capture and \(\beta\)-decay).

We’ll start with a framing of the problem and then discuss the concepts.

Urca intro#

We will consider the competition of different nuclear processes. For weak interactions, we have:

  • Electron-capture: a nucleus captures an electron, converting a proton to a neutron.

  • \(\beta\)-decay: a neutron in a nucleus decays into a proton + electron

Each of these processes emits a neutrino, which carries energy out of the star—this can lead to cooling.

The Urca process is when the electron-capture and \(\beta\)-decay competes, converting a nucleus back and forth, and robbing the star of energy.

The high densities inside a white dwarf can inhibit these processes, so we need to understand how electrons behave at white dwarf densities.

Tip

Why is it called Urca?

Gamow and Schenberg named it after the Cassino da Urca in Urca, Rio de Janeiro.

the Urca Process results in a rapid disappearance of thermal energy from the interior of a star, similar to the rapid disappearance of money from the pockets of the gamblers on the Casino de Urca.

Environments where Urca is at play#

We will focus on cooling in massive O/Ne WDs. Some background (and inspiration for these labs) can be found in:

Beyond the setup in this lab, we can encounter Urca in other contexts: