TY - JOUR
T1 - Structure and dynamics of the internetwork solar chromosphere
T2 - Results of a small-scale dynamo simulation
AU - Przybylski, D.
AU - Cameron, R.
AU - Solanki, S. K.
AU - Rempel, M.
AU - Danilovic, S.
AU - Leenaarts, J.
N1 - Publisher Copyright:
© The Authors 2025.
PY - 2025/11/1
Y1 - 2025/11/1
N2 - Context. The heating and structure of the solar chromosphere depends on the underlying magnetic field, among other parameters. The lowest magnetic flux of the solar atmosphere is found in the quiet Sun internetwork and is thought to be provided by the small-scale dynamo (SSD) process. Aims. Our aim is to understand the chromospheric structure and dynamics in a simulation with purely SSD generated magnetic fields. Methods. We performed a 3D radiation-magnetohydrodynamic (rMHD) simulation of the solar atmosphere, including the necessary physics to simulate the solar chromosphere. No magnetic field was imposed beyond that generated by an SSD process. We analysed the magnetic field in the chromosphere, and the resulting energy balance. Results. Plasma at chromospheric temperatures reaches high into the atmosphere, with small, transient regions reaching coronal temperatures. An average Poynting flux of 5×106 erga cm-3 s-1 is found at the base of the chromosphere. The magnetic field in the chromosphere falls off more slowly with height than predicted by a potential field extrapolation from the radial component of the photospheric field. Starting in the middle chromosphere, the magnetic energy density is an order of magnitude higher than the kinetic energy density and, in the upper chromosphere, is also higher than the thermal energy density. Nonetheless, even in the high chromosphere, the plasma-β in shock fronts and low-field regions can locally reach values above unity. Conclusions. The interactions between shocks and the magnetic field are essential to understanding the dynamics of the internetwork chromosphere. The SSD generated magnetic fields are strong enough to dominate the energy balance in the mid to upper chromosphere. The energy flux into the chromosphere is 8.16× 106 erga cm-2s-1, higher than the canonical values required to heat the quiet Sun chromosphere and corona. Possibly due to the limited box size, the simulation is unable to maintain a million-degree corona.
AB - Context. The heating and structure of the solar chromosphere depends on the underlying magnetic field, among other parameters. The lowest magnetic flux of the solar atmosphere is found in the quiet Sun internetwork and is thought to be provided by the small-scale dynamo (SSD) process. Aims. Our aim is to understand the chromospheric structure and dynamics in a simulation with purely SSD generated magnetic fields. Methods. We performed a 3D radiation-magnetohydrodynamic (rMHD) simulation of the solar atmosphere, including the necessary physics to simulate the solar chromosphere. No magnetic field was imposed beyond that generated by an SSD process. We analysed the magnetic field in the chromosphere, and the resulting energy balance. Results. Plasma at chromospheric temperatures reaches high into the atmosphere, with small, transient regions reaching coronal temperatures. An average Poynting flux of 5×106 erga cm-3 s-1 is found at the base of the chromosphere. The magnetic field in the chromosphere falls off more slowly with height than predicted by a potential field extrapolation from the radial component of the photospheric field. Starting in the middle chromosphere, the magnetic energy density is an order of magnitude higher than the kinetic energy density and, in the upper chromosphere, is also higher than the thermal energy density. Nonetheless, even in the high chromosphere, the plasma-β in shock fronts and low-field regions can locally reach values above unity. Conclusions. The interactions between shocks and the magnetic field are essential to understanding the dynamics of the internetwork chromosphere. The SSD generated magnetic fields are strong enough to dominate the energy balance in the mid to upper chromosphere. The energy flux into the chromosphere is 8.16× 106 erga cm-2s-1, higher than the canonical values required to heat the quiet Sun chromosphere and corona. Possibly due to the limited box size, the simulation is unable to maintain a million-degree corona.
KW - Sun: atmosphere
KW - Sun: chromosphere
KW - Sun: magnetic fields
UR - https://www.scopus.com/pages/publications/105022487174
U2 - 10.1051/0004-6361/202554656
DO - 10.1051/0004-6361/202554656
M3 - Article
AN - SCOPUS:105022487174
SN - 0004-6361
VL - 703
JO - Astronomy and Astrophysics
JF - Astronomy and Astrophysics
M1 - A148
ER -