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Independent contact shifts retain a positive mean fourth-order beta power term on shared bipolar edges in eight SEEG recordings

We compared two contact control models in public SEEG data from eight patients. Each patient supplied six fixed 20-second samples. On shared-contact bipolar edges, independent time shifts gave a mean normalized cross fourth cumulant of 0.128. Independent Fourier phases gave -0.002. The mean patient contrast was 0.131, with a descriptive bootstrap 95% interval of [0.086, 0.182]. All eight contrasts were positive. The exact two-sided sign-flip P value was 0.00781, under independent patient effects and sign symmetry at zero. A fourth-moment formula predicted the pooled control draws. Time shifts preserve contact burst shapes; independent phases change those shapes. Thus, a shared contact can retain a fourth-order power term under an independent-contact model. This benchmark does not identify neural coupling. The package contains code, spectra, source versions, hashes, results, and reproduction instructions.

SEEG · power correlation · fourth cumulant · beta band · bipolar montage · contact time shifts · Fourier phase controls · signal mixing

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References

6
  1. usesIndependent contact phase controls give absolute beta correlation above 0.30 on most shared-contact bipolar edges in eight SEEG recordings sci:sha256:b140aa736f880707f1f76cc167a2c578bc877c6ea56ddc6ca389a0996300da69

    We reused its 48 compact contact spectra, montage map, fixed sample plan, source metadata, and retrieval code. We retrieved the original ranges again and verified the spectra. The new endpoint is the fourth-order power term under contact shifts and contact phases, rather than the earlier voltage correlation.

  2. usesdoi:10.18112/openneuro.ds004473.v1.0.2

    The analysis used all eight patients from OpenNeuro ds004473 version 1.0.2; the recorded retrieval recipe, source hashes, and version are preserved.

  3. doi:10.1088/1741-2552%2Facae0a
  4. doi:10.1038/s42003-023-04648-x
  5. doi:10.1016/j.neuroimage.2018.02.032
  6. doi:10.1038/nn.3101

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