Exploring Spatial Ξ-Gradients in a Modified Double Slit Experiment
Abstract
This experimental concept tests the role of spatially variable condensivity (Ξ) in electromagnetic wave propagation, using the iconic double slit framework. By introducing an asymmetric Ξ field across the slits, we propose that observable deviations in the interference pattern—such as fringe displacement, asymmetry, and coherence modulation—can emerge. These effects would signal a local structural influence on the vacuum-like medium through which photons propagate, providing a novel probe into the field-based lattice theory underlying Charge Admittance Theory.
Classical Model Assumption
In traditional wave optics, the double slit interference pattern is governed by equal propagation speeds and homogeneous vacuum characteristics. The resulting fringe pattern depends on wavelength, slit separation, and distance to the detection screen:
The medium itself plays no active role in modulation—only geometry and coherence matter.
Ξ-Based Model Assumption
In this updated model, we hypothesize a spatial condensivity function:
Where:
Ξ0 is the base condensivity of the field
α introduces an asymmetry
d is the slit separation
This variation modifies the effective wave speed:
And thus alters the phase accumulation across the slits:
Where δLΞ represents the apparent path difference due to condensivity-induced slowing of the wavefront.
Expected Observables:
Ξ Field Effect | Classical Prediction | Ξ-Based Prediction |
Fringe Center | Centered | Shifted toward lower-Ξ slit |
Fringe Spacing | Uniform | Mild asymmetry from Ξ gradient |
Coherence Visibility | Maximal | Modulated by Ξ-dependent delays |
Arrival Timing | Uniform | Ξ-dependent time-of-flight shifts |
Energy Condensation | Not applicable | Focused in high-Ξ zones (structural lensing) |
Note: on Geometry and Ξ-Induced Fringe Shift
In the classic double-slit setup, the slits are vertically aligned, so the resulting interference pattern spreads horizontally across the detection screen. The angular variable θ describes positions along this horizontal axis.
If there is a Condensivity asymmetry (i.e., one slit is in a higher-Ξ region), then the effective propagation speed differs between the two slits, causing a relative phase shift. This results in a lateral displacement of the entire fringe pattern.
The interference pattern shifts away from the slit in the lower-Ξ (faster) region, and toward the higher-Ξ (slower) region, analogous to a Michelson phase imbalance.
This introduces a subtle, testable prediction: Ξ gradients across the slit plane will bias the fringe center, even in the absence of external fields or refractive index differences.