TY - JOUR
T1 - Statistical Observations of Proton‐Band Electromagnetic Ion Cyclotron Waves in the Outer Magnetosphere
T2 - Full Wavevector Determination
AU - Toledo‐Redondo, Sergio
AU - Lee, Justin H.
AU - Vines, Sarah K.
AU - Albert, I. F.
AU - André, Mats
AU - Castilla, A.
AU - Dargent, Jérémy P.
AU - Fu, Huishan
AU - Fuselier, Stephen A.
AU - Genot, V.
AU - Graham, Daniel B.
AU - Kitamura, Naritoshi
AU - Khotyaintsev, Yu. V.
AU - Lavraud, Benoit
AU - Montagud‐Camps, Victor
AU - Navarro, Enrique A.
AU - Norgren, Cecilia
AU - Perrone, D.
AU - Phan, Tai D.
AU - Portí, Jorge A.
AU - Salinas, Alfonso
AU - Stawarz, Julia E.
AU - Vaivads, Andris
PY - 2024/5
Y1 - 2024/5
N2 - Electromagnetic Ion Cyclotron (EMIC) waves mediate energy transfer from the solar wind to the magnetosphere, relativistic electron precipitation, or thermalization of the ring current population, to name a few. How these processes take place depends on the wave properties, such as the wavevector and polarization. However, inferring the wavevector from in‐situ measurements is problematic since one needs to disentangle spatial and time variations. Using 8 years of Magnetospheric Multiscale (MMS) mission observations in the dayside magnetosphere, we present an algorithm to detect proton‐band EMIC waves in the Earth's dayside magnetosphere, and find that they are present roughly 15% of the time. Their normalized frequency presents a dawn‐dusk asymmetry, with waves in the dawn flank magnetosphere having larger frequency than in the dusk, subsolar, and dawn near subsolar region. It is shown that the observations are unstable to the ion cyclotron instability. We obtain the wave polarization and wavevector by comparing Single Value Decomposition and Ampere methods. We observe that for most waves the perpendicular wavenumber (k⊥) is larger than the inverse of the proton gyroradius (ρ i ), that is, k⊥ρ i > 1, while the parallel wavenumber is smaller than the inverse of the ion gyroradius, that is, k‖ρ i < 1. Left‐hand polarized waves are associated with small wave normal angles (θ Bk < 30°), while linearly polarized waves are associated with large wave normal angles (θ Bk > 30°). This work constitutes, to our knowledge, the first attempt to statistically infer the full wavevector of proton‐band EMIC waves observed in the outer magnetosphere.
AB - Electromagnetic Ion Cyclotron (EMIC) waves mediate energy transfer from the solar wind to the magnetosphere, relativistic electron precipitation, or thermalization of the ring current population, to name a few. How these processes take place depends on the wave properties, such as the wavevector and polarization. However, inferring the wavevector from in‐situ measurements is problematic since one needs to disentangle spatial and time variations. Using 8 years of Magnetospheric Multiscale (MMS) mission observations in the dayside magnetosphere, we present an algorithm to detect proton‐band EMIC waves in the Earth's dayside magnetosphere, and find that they are present roughly 15% of the time. Their normalized frequency presents a dawn‐dusk asymmetry, with waves in the dawn flank magnetosphere having larger frequency than in the dusk, subsolar, and dawn near subsolar region. It is shown that the observations are unstable to the ion cyclotron instability. We obtain the wave polarization and wavevector by comparing Single Value Decomposition and Ampere methods. We observe that for most waves the perpendicular wavenumber (k⊥) is larger than the inverse of the proton gyroradius (ρ i ), that is, k⊥ρ i > 1, while the parallel wavenumber is smaller than the inverse of the ion gyroradius, that is, k‖ρ i < 1. Left‐hand polarized waves are associated with small wave normal angles (θ Bk < 30°), while linearly polarized waves are associated with large wave normal angles (θ Bk > 30°). This work constitutes, to our knowledge, the first attempt to statistically infer the full wavevector of proton‐band EMIC waves observed in the outer magnetosphere.
KW - plasma waves
KW - ion cylotron waves
KW - magnetosphere
U2 - 10.1029/2024ja032516
DO - 10.1029/2024ja032516
M3 - Article
SN - 2169-9402
VL - 129
JO - Journal of Geophysical Research: Space Physics
JF - Journal of Geophysical Research: Space Physics
IS - 5
M1 - e2024JA032516
ER -