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Spontaneous magnetization of the three-dimensional quantum Heisenberg ferromagnet at low temperature (Lieb's Problem A)

Theorem 1.1: for every d≥3d\ge3 and S∈{1/2,1,3/2,… }S\in\{1/2,1,3/2,\dots\} there is β0(d,S)\beta_0(d,S) such that for every β≥β0\beta\ge\beta_0 the zero-field nearest-neighbour dynamics has a translation-invariant β\beta-KMS state with ω(S0z)≥S/4\omega(S_0^z)\ge S/4. The proof uses an exchange-cycle (random interchange) representation with boundary pins, stable-polynomial negative dependence and a determinant identity for conditioned walks. Not shown: long-range order in the finite-volume two-point formulation, the critical temperature, or anything in d≤2d\le2. The companion manuscripts in the family prove Bloch's law and the spherical magnetization law in d=3d=3.

Exact FrontierDelta

Prior state unknown→proved

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Occurred: Sep 24, 2026

Delta type: SOURCE CLAIM

Assumptions: VibeMathed verification: lean-checked. Publication: announcement. AI contribution: ai-discovered. VibeMathed editorial classifications, scores, notes, relations, and dataset structure are CC BY 4.0. Source statements and linked content retain their own rights.

Canonical aliases: Spontaneous magnetization of the three-dimensional quantum Heisenberg ferromagnet at low temperature (Lieb's Problem A) · Heisenberg ferromagnet ordering

Confidence: Not scored

Registry verification: lean checked · announcement · candidate

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VibeMathed
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Unreleased internal OpenAI model
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Lean formalization (Heisenberg spontaneous magnetization)

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This event attributed to Unreleased internal OpenAI model

Companion manuscript: The first lattice correction to Bloch's law evidence for this event

Bloch's T3/2T^{3/2} law for the three-dimensional quantum Heisenberg ferromagnet evidence for this event

Theorem 1.1: for every d≥3d\ge3 and S∈{1/2,1,3/2,… }S\in\{1/2,1,3/2,\dots\} there is β0(d,S)\beta_0(d,S) such that for every β≥β0\beta\ge\beta_0 the zero-field nearest-neighbour dynamics has a translation-invariant β\beta-KMS state with ω(S0z)≥S/4\omega(S_0^z)\ge S/4. The proof uses an exchange-cycle (random interchange) representation with boundary pins, stable-polynomial negative dependence and a determinant identity for conditioned walks. Not shown: long-range order in the finite-volume two-point formulation, the critical temperature, or anything in d≤2d\le2. The companion manuscripts in the family prove Bloch's law and the spherical magnetization law in d=3d=3. parent of this event

Lean formalization (Heisenberg spontaneous magnetization) evidence for this event

Spontaneous magnetization of the three-dimensional quantum Heisenberg ferromagnet at low temperature (Lieb's Problem A) parent of this event

VibeMathed record: Spontaneous magnetization of the three-dimensional quantum Heisenberg ferromagnet at low temperature (Lieb's Problem A) evidence for this event

Companion manuscript: Spontaneous magnetization in the quantum Heisenberg ferromagnet evidence for this event

Companion manuscript: The spherical magnetization law for the three-dimensional quantum Heisenberg ferromagnet evidence for this event

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