Authors:
Dr. Pierdavide Coïsson | Université de Paris, Institut de physique du globe de Paris, CNRS | France
Louis Chauvet | Université de Paris, Institut de physique du globe de Paris, CNRS
Dr. Gauthier Hulot | Université de Paris, Institut de physique du globe de Paris, CNRS
Martin Jenner | Université de Paris, Institut de physique du globe de Paris, CNRS
Dr. Pierre Vigneron | Université de Paris, Institut de physique du globe de Paris, CNRS
Dr. Dalia Buresova | Institute of atmospheric physics CAS
Dr. Vladimir Truhlik | Institute of atmospheric physics CAS
Dr. Jaroslav Chum | Institute of atmospheric physics CAS
Dr. Janusz Mlynarczyk | AGH University
Prof. Andrzej Kulak | AGH University | Poland
In the recent years, regular burst-mode measurements campaigns of the Absolute Scalar Magnetometers (ASM) onboard two of the Swarm satellites have been conducted. During one week every month for each satellite, the total intensity of the Earth’s magnetic field has been measured using a sampling frequency of 250 Hz, enabling the detection of electromagnetic signals in the Extremely Low Frequencies (ELF).
It has been possible to observe a large number of whistlers excited by the most powerful lightning strikes occurring in the lower atmosphere. These detections can occur several thousand km away from the lightning strike location, because these signals propagate in the wave-guide between the Earth surface and the ionosphere before entering the ionised layers and reaching the satellites.
At the end of 2021 the orbital planes of the Swarm satellites overlapped while they were orbiting in counter-rotation. Several simultaneous burst-mode campaigns were acquired on both satellites, providing unique opportunities of detections of multiple whistlers generated by a single lightning. They revealed the complexity of the permeability of the ionosphere in this frequency range: some events have been detected by both satellites at several thousand km distance, while other events have been detected only by one satellite even if they were closer to each other.
The dispersion of the whistler signals as detected at satellite altitude depends on the electrons and ions present along the propagation path of these signals. It can be modeled by computing the propagation time of each frequency component using ray-tracing techniques. By also taking advantage of the simultaneous in-situ electron density measurements of the Electric Field Instrument (EFI) of Swarm, it is possible to constrain the ionosphere in the region below the satellite. This has been validated using data from ionosondes and the Ionosphere Real-Time Assimilative Model (IRTAM), used to specify real-time foF2 and hmF2 global maps, (improve the climatological International Reference Ionosphere (IRI) model - suggest to be deleted). Even if the whistler signals occur randomly, this opens new observational capabilities in areas where no ground-based observations of the ionosphere are possible. Whistler analysis will be particularly important in the coming years, when we will reach the solar maximum and the increase of ionisation will produce larger dispersions. No other LEO mission explored the ELF under this condition.
Extended opportunities to detect and characterise whistlers in the ELF will also be obtained with the NanoMagSat mission, for which continuous 2 kHz measurements will be acquired. The larger spectrum will enable the observation of proton whistlers and the multiple observation points provided by all available satellites of Swarm and NanoMagSat constellations could provide unique opportunities to study the permeability of the ionosphere to ELF signals and monitor the lower ionosphere from space.