Manuscript IV@1 · IV.tex · figure · 351cb2d7

Model 3 record and controls

Model 3: scalar stress form and exterior record › The source-sensitive record · lines 3207–3242

IV@1#fig:model3-record-controls

gravitationalscalaroperator / instrumenterror / restrictionsupport / scope

\Psi_0=\Omega

\Psi_1=\operatorname{Coh}(z_*)

A^{(3)}_{\Lambda,M}=\lambda\Pi_M B_\Lambda(J_\psi)\Pi_M

J_\psi,\ z_*,\ \Lambda,\ \lambda,\ \tau,\ \theta=\pi/2

independent of

M

p^{(3)}_{+,M}(\Psi_1)-p^{(3)}_{+,M}(\Psi_0)\ge c_3-e_M^{(3)},\quad e_M^{(3)}\to 0

Positive for sufficiently large finite $M$ . $\Lambda$ and measured $M$ stay retained.

interpolation off:

\lambda=0

source off: replace

T

by zero

both give

A=0

U=I

, and

p_+(\Psi_0)=p_+(\Psi_1)=1/2

The massless scalar is not the source-off operation.

Model 3 record and controls. At a selected finite momentum cutoff, the coherent preparation has a positive curvature-pairing mean relative to the vacuum. Number-tail estimates give positive contrast for sufficiently large finite compressions. Interpolation-off and explicit source-off operations both give the exact probability $1/2$ at the chosen Ramsey phase.

Model 3 record and controls

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