6533b824fe1ef96bd1280aee

RESEARCH PRODUCT

Collisionless shock heating of heavy ions in SN 1987A

Fabio RealeDavid N. BurrowsKari A. FrankGiovanni PeresOleh PetrukSalvatore OrlandoFabrizio BocchinoCostanza ArgiroffiMarco Miceli

subject

Shock wave010504 meteorology & atmospheric sciencesAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesElectronAstrophysics01 natural sciencesmagnetohydrodynamics (MHD)Spectral lineIonISM: cloud0103 physical sciencesISM: individual objects: SN 1987ASupernova remnant010303 astronomy & astrophysicsAstrophysics::Galaxy AstrophysicsISM: supernova remnantacceleration of particle0105 earth and related environmental sciencesHigh Energy Astrophysical Phenomena (astro-ph.HE)PhysicsAstronomy and AstrophysicsX-rays: ISMSupernovaElectron temperatureAstrophysics - High Energy Astrophysical PhenomenaHeliosphere

description

Astrophysical shocks at all scales, from those in the heliosphere up to the cosmological shock waves, are typically "collisionless", because the thickness of their jump region is much shorter than the collisional mean free path. Across these jumps, electrons, protons, and ions are expected to be heated at different temperatures. Supernova remnants (SNRs) are ideal targets to study collisionless processes because of their bright post-shock emission and fast shocks. Although optical observations of Balmer-dominated shocks in young SNRs showed that the post-shock proton temperature is higher than the electron temperature, the actual dependence of the post-shock temperature on the particle mass is still widely debated. We tackle this longstanding issue through the analysis of deep multi-epoch and high-resolution observations of the youngest nearby supernova remnant, SN 1987A, made with the Chandra X-ray telescope. We introduce a novel data analysis method by studying the observed spectra in close comparison with a dedicated full 3-D hydrodynamic simulation. The simulation is able to reproduce self-consistently the whole broadening of the spectral lines of many ions altogether. We can therefore measure the post shock temperature of protons and selected ions through comparison of the model with observations. We have obtained information about the heating processes in collisional shocks by finding that the ion to proton temperature ratio is always significantly higher than one and increases linearly with the ion mass for a wide range of masses and shock parameters.

10.1038/s41550-018-0677-8http://hdl.handle.net/10447/339488