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Resolving the spinon hierarchy of the Heisenberg antiferromagnet

Abstract

A local spin fluctuation in the spin-1/2 Heisenberg antiferromagnet creates an even number of fractional spinon excitations. We resolve its zero-temperature dynamical structure factor through six spinons directly in the thermodynamic limit. Beyond the established two-spinon contribution of 72.89%, the four-spinon response gives approximately 21.90% of the integrated intensity and six spinons contribute a further 4.3%, bringing the response to about 99% of both the intensity and first-frequency-moment sum rules. We derive momentum-independent first-moment fractions in the calculated sectors and a general upper-edge law Sn∼ An(k)(ωn,u−ω)(n2−3)/2 for every even n at nonzero momentum. The rapid growth of the edge exponent explains why the expanding multiparticle bandwidth carries very little high-energy weight, while higher sectors remain appreciable within the lower-sector continua.

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BibTeX
@misc{mcculloch2026resolving,
  title = {{Resolving the spinon hierarchy of the Heisenberg antiferromagnet}},
  author = {Ian P. McCulloch and Jesse J. Osborne},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.42127},
  eprint = {2610.42127},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.42127},
}
RIS
TY  - UNPB
TI  - Resolving the spinon hierarchy of the Heisenberg antiferromagnet
AU  - Ian P. McCulloch
AU  - Jesse J. Osborne
PY  - 2026
DA  - 2026/10/30
PB  - arXiv
DO  - 10.48550/arxiv.2610.42127
UR  - https://arxiv.org/abs/2610.42127
AB  - A local spin fluctuation in the spin-1/2 Heisenberg antiferromagnet creates an even number of fractional spinon excitations. We resolve its zero-temperature dynamical structure factor through six spinons directly in the thermodynamic limit. Beyond the established two-spinon contribution of 72.89%, the four-spinon response gives approximately 21.90% of the integrated intensity and six spinons contribute a further 4.3%, bringing the response to about 99% of both the intensity and first-frequency-moment sum rules. We derive momentum-independent first-moment fractions in the calculated sectors and a general upper-edge law S_n∼ A_n(k)(ω_n,u−ω)^(n^2−3)/2 for every even n at nonzero momentum. The rapid growth of the edge exponent explains why the expanding multiparticle bandwidth carries very little high-energy weight, while higher sectors remain appreciable within the lower-sector continua.
ER  -