In standard quantum mechanics, the time-dependent Schrödinger equation describes how the wave function of a particle evolves in time: i\hbar \frac{\partial \psi}{\partial t} = \hat{H}\psi
where (\psi) represents a probability amplitude — not a real field, but a statistical description of possible outcomes.
In this view, the act of observation “collapses” the wave function into one result.
Khandro Field Theory (KFT) proposes a different picture.
Here, the basic entity is not a probability wave but a real field phase (\phi_k(\mathbf{r},t)), representing continuous physical interference across space.
Its evolution equation replaces the external potential (V) with the intrinsic gradient of the field density: \hbar \frac{\partial \phi_k}{\partial t} = -\frac{\hbar^2}{2m}\nabla^2 \phi_k + \alpha (\nabla \rho_k)\phi_k
In KFT, no collapse occurs — measurement simply introduces a local phase shift within the unified field.
Photons, in this sense, “are not afraid of being watched.”
🔗 Learn more: The Khandro Field Theory (KFT): Consistency Conditions from Shapiro Delay and Constraints from Delbrück Analogues https://zenodo.org/records/17279181
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