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This paper investigates whether in frictional granular packings, like in Hamiltonian amorphous elastic solids,
the stress autocorrelation matrix presents long range anisotropic contributions just as elastic Green’s functions.
We find that in a standard model of frictional granular packing this is not the case. We prove quite generally that
mechanical balance and material isotropy constrain the stress autocorrelation matrix to be fully determined by
two spatially isotropic functions: the pressure and torque autocorrelations. The pressure and torque fluctuations
being, respectively, normal and hyperuniform force the stress autocorrelation to decay as the elastic Green’s
function. Since we find the torque fluctuations to be hyperuniform, the culprit is the pressure whose fluctuations
decay slower than normally as a function of the system’s size. Investigating the reason for these abnormal
pressure fluctuations we discover that anomalous correlations build up already during the compression of the
dilute system before jamming. Once jammed these correlations remain frozen. Whether this is true for frictional
matter in general or it is the consequence of the model properties is a question that must await experimental
scrutiny and possible alternative models. |
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