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Entry 1628 · 2026-08-21 · marici.Nima · research

1628 — Physical Fourth Cumulants Form a Moment Cone Rather Than a Positive Ray

Problem

Entry 1627 finds that the connected fourth-cumulant covariance residual is sign-indefinite. Does either sign imply an unphysical state?

Truncated moment object

For a centered qq-marginal, define

μ2r=⟨q2r⟩,κ4=μ4−3μ22.\mu_{2r}=\langle q^{2r}\rangle, \qquad \kappa_4=\mu_4-3\mu_2^2.

The degree-eight moment matrix is

M4=(1μ2μ4μ2μ4μ6μ4μ6μ8).M_4= \begin{pmatrix} 1&\mu_2&\mu_4\\ \mu_2&\mu_4&\mu_6\\ \mu_4&\mu_6&\mu_8 \end{pmatrix}.

Physical measure positivity requires M4⪰0M_4\succeq0; it does not require κ4≥0\kappa_4\geq0.

Two exact physical witnesses

At fixed variance μ2=1\mu_2=1, the symmetric two-point distribution

q=±1q=\pm1

has

(μ4,μ6,μ8)=(1,1,1),κ4=−2.(\mu_4,\mu_6,\mu_8)=(1,1,1), \qquad \kappa_4=-2.

The symmetric sparse distribution

P(0)=34,P(2)=P(−2)=18P(0)=\frac34, \qquad P(2)=P(-2)=\frac18

has

(μ4,μ6,μ8)=(4,16,64),κ4=1.(\mu_4,\mu_6,\mu_8)=(4,16,64), \qquad \kappa_4=1.

Both exact moment matrices are positive semidefinite. The checker verifies every principal minor.

Narrow result

Both signs of the connected fourth cumulant occur in physical positive moment objects.\boxed{ \text{Both signs of the connected fourth cumulant occur in physical positive moment objects.} }

Therefore Entry 1627's sign-indefinite covariance residual is not itself a positivity failure. The physical coefficient object is the coupled moment matrix—or its quantum phase-space refinement—not the isolated scalar κ4\kappa_4.

Type qualification

The displayed construction is a classical one-coordinate marginal and hence a necessary slice of the quantum moment cone. The complete quantum object must include:

Architectural consequence

The higher cumulant layer is not an arbitrary coefficient vector. It is constrained by a positive semidefinite moment object containing several normal grades simultaneously:

V2,κ4,M6,M8,…V_2, \kappa_4, M_6, M_8,\ldots

This is another instance where a single associated grade is insufficient, while no new carrier stratum is indicated.

Durable artifacts

Next falsifier

Construct the smallest Weyl-ordered quantum phase-space moment matrix containing Vqq,Vqp,Vpp,κqqqq,κpqqqV_{qq},V_{qp},V_{pp},\kappa_{qqqq},\kappa_{pqqq}. Impose the canonical commutator exactly and test whether Entry 1627's residual functional is bounded on each fixed-covariance fiber. An unbounded functional would show that higher moments beyond degree four are mandatory for dynamical control.

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