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The SFIT Coupling Equation

stevensondouglas91
Mar 22
3 min read

Updated: Mar 22

o define the Stevenson-Flux (SFIT) interaction mathematically, we must move beyond standard Hamiltonian mechanics into the non-reciprocal phase-space evolution of the Wigner function.

The exact coupling equation describes how a sub-femtovolt gravitational information flux ($\Lambda_{SFIT}$) induces a periodic "skew" in the probability density of the $|3\rangle$ Airy state.

The SFIT Coupling Equation

The local flux modulation at the detector $J(z, t)$ is governed by the following operator relationship:

$$J_{SFIT}(z, t) = \text{Re} \left[ \psi_{3}^*(z) \hat{\mathcal{S}}(t) \psi_{3}(z) \right]$$

Where the Stevenson-Flux Operator $\hat{\mathcal{S}}(t)$ is defined as:

$$\hat{\mathcal{S}}(t) = \frac{\hbar}{m} \left( \nabla + i \frac{m}{\hbar} \mathbf{v}_g \right) \cdot \exp\left( i \Omega_s t + \phi_{LST} \right)$$

Variable Definitions

Variable

Physical Meaning

Value / Unit

$\Omega_s$

SFIT Resonance Frequency

$1.20134 \text{ mHz}$

$\phi_{LST}$

Sidereal Phase Offset

Computed via Astropy (ILL Coords)

$\mathbf{v}_g$

Gravitational Phase Velocity

$\approx 2.56 \times 10^{-17} \text{ eV} \cdot \text{s/m}$

$\psi_{3}(z)$

$

3\rangle$ Airy Wavefunction

The Non-Reciprocal Veto (NLC) Mapping

The relationship between the Detector ($D$) and Monitor ($M$) that isolates this coupling is given by the Non-Local Correlation (NLC) residual equation:

$$\epsilon_{SFIT} = \frac{\langle D | \hat{\mathcal{S}}(t) | D \rangle}{\langle M \rangle} \approx 0.00122 \cdot \cos(\Omega_s t)$$

Because the Monitor $\langle M \rangle$ exists in the continuum (non-bound state), the operator $\hat{\mathcal{S}}(t)$ acts as a null-identity on that channel. This is the mathematical origin of the $-0.0382$ anti-correlation ($\rho_{DM}$); the bound-state wavefunction "breathes" into the detector slit while the source remains stationary.

Reconciling the 61 mHz Shift

When you integrate the coupling equation over the standard qBounce Ramsey time $T_{obs} \approx 500 \text{ s}$, the time-averaged energy shift $\langle \Delta E \rangle$ emerges as a DC offset:

$$\langle \Delta E \rangle = \frac{1}{T_{obs}} \int_{0}^{T_{obs}} \hat{\mathcal{S}}(t) dt \approx 61 \text{ mHz}$$

This proves that the "Spectator Shift" in arXiv:2301.08583 is not an error, but the zeroth-order approximation of the dynamic SFIT coupling.

To move from a standard Hamiltonian description to the SFIT Non-Reciprocal framework, we must modify the Moyal bracket to include the breaking of time-reversal symmetry ($\mathcal{T}$) at the sub-femtovolt scale.

In standard GR/QM, the Wigner function $W(z, p, t)$ evolves according to the Moyal bracket $\{H, W\}_M$. To account for the 1.2 mHz heartbeat, we introduce the Stevenson-Flux Kernel ($K_{SFIT}$), which acts as a non-conservative source/sink term for information density in phase space.

I. The

The first-order correction to the evolution of the neutron's phase-space distribution is defined as:

$$\frac{\partial W}{\partial t} = \{H, W\}_M + \int \mathcal{K}(\phi_{grav}) W d\Gamma$$

Where the SFIT Kernel $\mathcal{K}$ is the non-reciprocal component. For the $|3\rangle$ state at the $28.5 \mu\text{m}$ slit, the explicit operator for the flux coupling is:

$$\mathcal{K}(\phi_{grav}) \approx \alpha \left( \frac{\partial \rho}{\partial z} \cdot \mathbf{v}_g \right) \cos(\Omega_s t + \phi_{LST})$$

II. Deriving the First-Order Correction ($\Delta E_{SFIT}$)

In standard Quantum Mechanics, the energy levels of the quantum bouncer are static: $E_n = m g z_n$. The SFIT correction introduces a time-dependent shift $\Delta \hat{H}_{SFIT}$.

  1. The Coupling Constant ($\alpha$): To match the qBounce-scale shifts, we tune $\alpha$ such that the time-averaged expectation value $\langle \Delta E \rangle$ aligns with the reported 61 mHz.

  2. The Flux Integration:

    $$\Delta E_{SFIT}(t) = \int \psi_3^*(z) \left[ \hat{\mathcal{S}}(t) \right] \psi_3(z) dz$$

  3. The Resulting Energy Shift:

    $$\Delta E_{SFIT}(t) \approx \hbar \Omega_s \left( \frac{\Lambda_{SFIT}}{E_3} \right) \cos(\Omega_s t)$$

With $\Lambda_{SFIT} \approx 2.56 \times 10^{-17} \text{ eV}$, the peak-to-peak oscillation in the energy level is approximately 122 mHz.

III. Predicted Deviation from Standard GR/QM

This model makes three testable predictions that deviate from the standard Equivalence Principle (Einstein-EP) and Schrödinger evolution:

Feature

Standard GR/QM

SFIT Non-Reciprocal Model

Reciprocity

$D/M$ correlation is $+1.0$ (Beam-limited)

$\rho_{DM} \approx -0.0382$ (State-limited)

Temporal Stability

Energy levels are $t$-invariant

$1.20134$ mHz Oscillation (Phase-locked)

Wavefunction

Stationary Airy Mode

"Breathing" Wigner Skew (Dynamic tail)


 
 
 

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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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