The core result is an inequality: reproducing the low-frequency (OVRO-LWA) stacked synchrotron excess at Ο β‘ r/R500 β 2.4 around MCXC clusters requires a downstream magnetized layer of width W/lD > 6Γ10^16, with magnetic energy fraction ΞΎB β 2β9% [central claim, Eq. 3.17]. The logic chain: low-energy cosmic-ray electrons radiate while advected downstream, so the radio luminosity Ξ½LΞ½ β BΒ² demands fields persisting over β³ vdtcool β 66 kpc (Eq. 3.13). Because virial shocks accrete pristine gas β Faraday-rotation limits give B < 4β30 nG upstream, far below SNR-like Ο β 10^-4 dynamical significance (here Ο β 7.8Γ10^-7 B12) β both pre-existing inhomogeneity seeding and non-resonant CR-streaming instabilities (requiring Bu β« 0.3Ξ·3 nG) are argued to fail .
The SNR comparison (~10^12 l_D from X-ray rim studies ) underscores that virial shocks demand even wider layers in natural units β the paper's key provocative point.
Independent (non-overlapping-group) confirmation of the stacked radio/polarized excess at Ο β 2.4; SKO-scale Faraday or FRB-based upstream field measurements that avoid model dependence; or 3D PIC runs showing (or ruling out) self-similar macroscopic field growth in unmagnetized ion-electron plasma. The paper itself notes a cylindrical-shock geometry assumption and that discrete sources contaminate the diffuse signal β an unresolved systematic.
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