Magnetars are neutron stars with magnetic fields of $10^{14}$–$10^{15}$ G, orders of magnitude above the QED critical field (4.4×$10^{13}$ G). In such fields, the vacuum becomes an anisotropic medium: photons of different polarizations travel at different speeds, much like light in a crystal. This effect, predicted by Heisenberg and Euler as early as 1936, had not yet received direct observational confirmation. The present work continues a series of polarimetric studies of magnetars initiated by IXPE; earlier measurements yielded polarization degrees no higher than 20%, which was interpreted as evidence for a condensed surface.
Observations were carried out simultaneously with three instruments: IXPE (2–8 keV, polarimetry), NICER (0.2–12 keV, spectroscopy), and the 64-meter Parkes radio telescope (2.5–4 GHz, polarimetry). The radio data allowed the rotation geometry to be determined: the angle between the magnetic and rotation axes is α≈3.4°, and the angle between the rotation axis and the line of sight is ζ≈7.5°, making it a nearly aligned rotator. The X-ray pulse profiles and the Stokes Q/I and U/I curves were compared with radiation transfer simulations in a magnetized atmosphere and magnetosphere (the MAGTHOMSCATT code) with the vacuum birefringence effect included and excluded.
The phase-averaged polarization degree in the 2–8 keV band is 46±4%, and in the soft band 2–3 keV it reaches 59±5%, a record among the six magnetars observed by IXPE. In phase-resolved analysis, the polarization in the 2–4 keV band rises to 74±11%, and in 2–3 keV to 82±15%. Polarization drops sharply from 2 to 4 keV: from 59±5% to 37±5%. Modeling shows that without vacuum birefringence the Q/I and U/I curves exhibit strong oscillations (χ²/dof = 106.8/4 and 95.6/4), while including it dramatically improves the fit (χ²/dof = 19.0/4 and 10.9/4).
Unlike previous work, where high polarization was attributed to a condensed surface or purely atmospheric effects, here we observe polarization that cannot be reproduced without magnetospheric vacuum birefringence. This sets 1E 1547.0-5408 apart from other magnetars and makes it a natural laboratory for testing QED in strong fields. The work also shows that the sharp decline in polarization between 2 and 4 keV is consistent with the expected influence of a vacuum resonance in the atmosphere.
To definitively confirm the effect, observations in a softer X-ray band (0.5–1 keV) are needed, where models predict polarization above 80%. Future missions such as GoSOX could provide such sensitivity. Deeper IXPE observations are also required to refine the polarization behavior at 4–8 keV and to test the role of the vacuum resonance.
The results will impact strong-field physics, neutron star astrophysics, and quantum electrodynamics. They will also set a standard for interpreting polarimetric data from future X-ray missions.
Proposals for additional IXPE observations are planned to accumulate statistics in the harder part of the band. Models incorporating the vacuum resonance in the atmosphere are being developed to fully describe the energy dependence of polarization.
The contribution of the vacuum resonance to depolarization at 3–4 keV remains an open question. It is also unclear how universal vacuum birefringence is among magnetars, or whether it manifests only under certain geometries and surface temperatures.
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What the work does
This work presents polarimetric observations of the magnetar 1E 1547.0-5408 using IXPE, NICER, and Parkes. A record polarization degree of up to 59% was measured in the 2–3 keV range, with phase-resolved values reaching 82%. Radiative transfer modeling shows that the data are consistent with the model only when vacuum birefringence in the magnetosphere is included, making this the most compelling evidence for a QED effect in astrophysics to date.
Where its strength is
The strength of the work lies in obtaining phase-resolved Stokes curves with high statistical significance that cannot be explained without vacuum birefringence. This opens a path to direct tests of QED in strong fields.
Where it could go next
Worth trying
Why this may matter
Confirming vacuum birefringence in magnetars would be the first observational test of QED in strong fields, which is important for fundamental physics.
Nearby works in our archive
The closest work in the archive sits at 0.64 by meaning — the usual level for our corpus.
The magnetic field of magnetar 1E 1547.0-5408 is so strong that at a distance of 1000 km from the star it still exceeds the field of the most powerful laboratory magnets by millions of times.
In Stanislaw Lem's novel "Fiasco," stars with extreme magnetic fields that affect the properties of vacuum are mentioned. The idea that emptiness can behave like a crystal resonates with the concept of vacuum birefringence.