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pith:VMK77YLC

pith:2026:VMK77YLCWYIQWAWRWQQ7HXQ3PR
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Emergent impedance due to antiferromagnetic domain wall dynamics

Jotaro J. Nakane, Jun'ichi Ieda, Yasufumi Araki, Yuta Yamane

Antiferromagnetic domain walls generate emergent impedance through competing contributions from translational motion and internal spin canting.

arxiv:2605.16778 v1 · 2026-05-16 · cond-mat.mes-hall

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Claims

C1strongest claim

Two dynamical modes play separate roles in the emergent impedance: translational motion of the domain-wall center generates a contribution proportional to its velocity, while time-dependent canting of the sublattice magnetizations localized within the moving domain wall produces a contribution whose magnitude is inversely proportional to the antiferromagnetic exchange coupling constant; their competition determines the sign and magnitude of the imaginary part at sub-resonant frequencies.

C2weakest assumption

The combined action of spin-transfer torque and spinmotive force, previously established for spiral magnets, remains the dominant mechanism for generating emergent impedance when applied to antiferromagnetic domain walls, with no additional damping or disorder terms required to alter the derived analytical expressions.

C3one line summary

Analytical expressions for emergent impedance in antiferromagnetic domain walls show separate contributions from translational motion proportional to velocity and from time-dependent sublattice canting inversely proportional to exchange coupling, with their competition setting the imaginary part at低

References

73 extracted · 73 resolved · 0 Pith anchors

[1] L. Néel, Ann. de physique17, 5 (1932); F. Bitter, Phys. Rev.54, 79 (1938); J. H. Van Vleck, J. Chem. Phys.9, 85 (1941) 1932
[2] C. G. Shull and J. S. Smart, Phys. Rev.76, 1256 (1949); C. G. Shull, W. A. Strauser, E. O. Wollan,ibid.83, 333 (1951) 1949
[3] T. Jungwirth, X. Marti, P. Wadley, and J. Wunderlich, Antiferromagnetic spintronics, Nat. Nanotechnol.11, 231 (2016) 2016
[4] V . Baltz, A. Manchon, M. Tsoi, T. Moriyama, T. Ono, and Y . Tserkovnyak, Antiferromagnetic spintronics, Rev. Mod. Phys.90, 015005 (2018) 2018
[5] J. Železný, P. Wadley, K. Olejník, A. Hoffmann, and H. Ohno, Spin transport and spin torque in antiferromag- netic devices, Nat. Phys.14, 220 (2018) 2018

Formal links

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First computed 2026-05-20T00:03:21.533326Z
Builder pith-number-builder-2026-05-17-v1
Signature Pith Ed25519 (pith-v1-2026-05) · public key
Schema pith-number/v1.0

Canonical hash

ab15ffe162b6110b02d1b421f3de1b7c66b868421e58e19e66980b062601051e

Aliases

arxiv: 2605.16778 · arxiv_version: 2605.16778v1 · doi: 10.48550/arxiv.2605.16778 · pith_short_12: VMK77YLCWYIQ · pith_short_16: VMK77YLCWYIQWAWR · pith_short_8: VMK77YLC
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curl -sH 'Accept: application/ld+json' https://pith.science/pith/VMK77YLCWYIQWAWRWQQ7HXQ3PR \
  | jq -c '.canonical_record' \
  | python3 -c "import sys,json,hashlib; b=json.dumps(json.loads(sys.stdin.read()), sort_keys=True, separators=(',',':'), ensure_ascii=False).encode(); print(hashlib.sha256(b).hexdigest())"
# expect: ab15ffe162b6110b02d1b421f3de1b7c66b868421e58e19e66980b062601051e
Canonical record JSON
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    "submitted_at": "2026-05-16T03:19:14Z",
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