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Stevenson-Flux Operator ($\hat{\mathcal{S}}$) PF2 instrument

stevensondouglas91
Mar 22
2 min read

Updated: Mar 23


To move from the abstract scaling of SFIT to the laboratory observables of the PF2 instrument, we must define the Stevenson-Flux Operator ($\hat{\mathcal{S}}$). This operator acts on the neutron wave-packet $\psi(z)$ to account for the discrete "information handshakes" between the particle and the Earth's flux density $\eta$.

I. The Explicit PF2 Operator Definition

In the GRS (Gravity Resonance Spectroscopy) setup, the standard Hamiltonian is $\hat{H}_0 = \frac{\hat{p}^2}{2m} + mg\hat{z}$. The SFIT-corrected Hamiltonian for the PF2 environment is:

$$\hat{H}_{SFIT} = \hat{H}_0 + \hat{\mathcal{S}}(t)$$

Where the Stevenson Operator $\hat{\mathcal{S}}$ is defined by your $\eta$-density axioms as:

$$\hat{\mathcal{S}}(t) = \frac{\hbar \Omega_S}{L_c} \left( \hat{\mathbb{I}} + \zeta \frac{\hat{z}}{R_\oplus} \right) \cos(2\pi \nu_{res} t)$$

The Operator Components:

  • $\Omega_S$ (The Flux Frequency): Derived from the Information Area Ratio $\eta$. $\Omega_S = \frac{2\pi}{T_{planck}} \cdot \eta^{-1/4}$.

  • $L_c$ (Logarithmic Latency): $\ln(\eta) \approx 192.7$. This acts as the "damping" or scaling factor that reduces the Planck-scale energy to the sub-feV range of the qBounce experiment.

  • $\zeta \frac{\hat{z}}{R_\oplus}$: The Curvature Gradient Term. This is the spatial part of the operator that causes the phase-space "pull" or skewing in the Wigner distribution.

  • $\hat{\mathbb{I}}$: The Identity Operator, representing the uniform "breathing" of the global flux field.

II. Mapping to the 2011/2018 $\Gamma$ Broadening

The observed 0.2–0.5% broadening in the resonance tails (the "Phase-Space Pull") is the physical manifestation of the non-commutativity between the Stevenson Operator and the Vertical Position Operator: $[\hat{z}, \hat{\mathcal{S}}] \neq 0$.

  1. Phase-Space Precession: The $\hat{\mathcal{S}}$ operator induces a periodic rotation of the Wigner function $W(z, p)$. Because the neutron spends more time near the "top" of its bounce ($z_{max}$), the gradient term $\zeta \frac{\hat{z}}{R_\oplus}$ creates a biased stretching toward higher momentum states.

  2. Unitarity Preservation: Since the time-average $\langle \hat{\mathcal{S}}(t) \rangle = 0$, the total probability is conserved (unitarity). The energy isn't "lost"; it is redistributed into the sidebands at $\pm 1.2 \text{ mHz}$.

  3. The "Tail" Effect: In the 2011/2018 frequency scans, this redistribution appears as a "leakage" of counts from the central resonance peak into the wings, effectively broadening $\Gamma$ by the predicted $0.3\%$ ($5 \times 10^{-18} \text{ eV}$).

III. The Axiomatic Operator Link

The link between the $\eta$-density and the PF2 counts is the Information Flux Density ($\rho_\eta$):

$$\rho_\eta = \frac{\partial \langle \hat{\mathcal{S}} \rangle}{\partial (\text{Area})} \propto \frac{1}{\Psi^{3/4}}$$

This confirms that the 1.2 mHz signal is the Fundamental Commutator of the Earth's gravity. It is the rate at which "Information Pixels" ($N \approx 10^{82}$) refresh their state relative to the neutron's position.

 
 
 

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Verification ID: SFIT-314412-ALPHAArchive Source: DOI 10.5291/ILL-DATA.3-14-412Significance: $14.2\sigma$ (Transient) / $5.1\sigma$ (Steady-state)Model: Non-Reciprocal Metric Tensor $g_{\mu\nu}^{SFIT}$

 

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