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Published August 25, 2026 | Version v13

Quantum Feed-Forward Diverter Loop

Authors/Creators

Description

This scientific proposal outlines a unique thought experiment combining ultra-cold Rubidium atomic clouds in a negative time dwell state with quantum entanglement triggers. The framework utilizes a quantum feed-forward mechanism to route incoming photon light pulses onto an alternate path, effectively presenting a theoretical layout to bypass temporal grandfather paradoxes without inducing a system-wide wavefunction collapse.

"Update (Version 2): Added Python (Qiskit) simulation script to verify quantum state routing logic."

Implemented a 4-Case Marginal Probability Matrix simulation (Z-basis, X-basis, No-measurement, and Random-basis) to rigorously verify that the system strictly obeys the No-Signaling Theorem and preserves causality under feed-forward routing conditions.

Update (Version 4): Integrated an advanced Time-Symmetric / Post-Selected Diverter Test framework. Successfully verified a 100% quantum state correlation conditioned on future measurement outcomes while strictly preserving the global No-Signaling theorem constraint.

Version 5 Update — Temporal Wavepacket and Effective Negative Group-Delay Model

This version extends the Quantum Feed-Forward Diverter Loop thought experiment by introducing a temporal wavepacket model for the photon and an effective frequency-domain transfer function representing positive and negative group delays.

The photon is modeled as a Gaussian temporal wavepacket. Two alternative pathways are assigned effective delays, with Path-1 represented by a positive delay and Path-2 by an effective negative group delay. The resulting temporal wavepackets are numerically propagated and compared to visualize the corresponding temporal shifts.

The quantum-routing component is then combined with an entangled A–B pair, photon–B interaction, and A-controlled quantum path diversion. The simulation evaluates both the unconditional photon-path distribution and the post-selected correlation between the earlier photon path and the later B measurement outcome.

Using 20,000 simulated shots, the unconditional path probabilities were approximately:

P(Path=0) = 0.5000
P(Path=1) = 0.5000

Post-selection produced perfect conditional correlations in this circuit model:

P(Path=0 | B=0) = 1.0000
P(Path=1 | B=1) = 1.0000

These results demonstrate temporal-wavepacket shifting and strong conditional quantum correlation within the computational model. The effective negative group delay is used as a mathematical transfer-function parameter and is not interpreted as literal backward propagation of a photon or proof of retrocausality.

This version is intended as a theoretical/computational extension of the proposed Quantum Feed-Forward Diverter Loop and does not constitute an experimental demonstration of negative time, retrocausal signalling, or violation of the quantum no-signalling principle.

Version 6 Update — Coupled Temporal–Quantum Counterfactual Test
This version extends the Quantum Feed-Forward Diverter Loop by coupling the temporal wavepacket framework with the quantum A–B diverter model and introducing an explicit future-measurement-choice test.
The photon is represented as a temporal wavepacket, while the two quantum paths are associated with different effective transfer functions. Path-1 is assigned an effective negative group delay. The quantum model includes A–B entanglement, photon–B interaction, and A-controlled path diversion.
The model tests whether changing the future measurement basis of particle B can alter the earlier photon-path marginal distribution without classical communication. Four future measurement conditions were compared: Z basis, X basis, Random basis, and No measurement.
Using 20,000 simulated shots, the earlier-path probabilities were approximately:
P(Earlier Path=0):
Z basis = 0.4992
X basis = 0.4979
Random basis = 0.4979
No measurement = 0.5013
P(Earlier Path=1):
Z basis = 0.5008
X basis = 0.5021
Random basis = 0.5021
No measurement = 0.4986
The results show that the earlier photon-path marginal remains approximately 50:50 across the different future measurement choices. No controllable change in the earlier marginal distribution was observed in this computational model.
Conditional correlations between the photon path and the later B outcome remain present, demonstrating the distinction between quantum correlation and usable retrocausal signalling.
This version therefore provides a counterfactual/no-signalling test of the proposed mechanism. It does not demonstrate literal backward time, retrocausal communication, or a violation of the quantum no-signalling principle.
Important: The negative group delay remains an effective temporal transfer-function parameter and should not be interpreted as literal backward propagation of the photon.
 
Version 7 A coupled computational model combining temporal wavepacket shifts with quantum path control and future-conditioned A–B correlations was implemented. The earlier-path marginal remained approximately 50:50 in the tested configuration, while perfect conditional Path–B correlations were observed.
 
Version 8 Update — Future-Choice / Retrocausal Marginal Test
This version extends the Quantum Feed-Forward Diverter Loop computational model by testing whether an independently selected future measurement basis of qubit B can statistically alter the earlier photon-path marginal distribution.
The model retains the joint temporal-wavepacket and quantum-path framework introduced in Version 7, including:
Path-0 coupled to a positive-delay temporal wavepacket.
Path-1 coupled to an effective negative-delay temporal wavepacket.
Quantum A–B correlations and photon–B interaction.
Earlier photon-path measurement performed before the future B measurement.
Independent variation of the future B measurement choice.
Four future-choice conditions were compared: Z basis, X basis, no measurement, and random basis.
For the principal Z-versus-X comparison, the simulated results were:
P(Path=0 | future B=Z) = 0.498150
P(Path=0 | future B=X) = 0.499450
Difference = −0.001300
Z-score = −0.260001
Two-sided p-value = 0.794863
No statistically significant difference was detected between the earlier-path marginal distributions under the tested future measurement choices.
The simulation therefore provides no evidence of controllable retrocausal signalling within this computational model. Conditional correlations between the earlier path and later B outcomes may still occur, but these correlations do not by themselves demonstrate that a future measurement choice can be used to control an earlier observable.
Important limitation: the negative delay used in this model represents an effective mathematical temporal-transfer-function shift. It does not represent literal backward propagation of a photon in time.
This Version 8 should therefore be interpreted as a computational test of the no-signalling/retrocausal hypothesis, not as an experimental demonstration of backward time propagation or retrocausal communication.
Version 9 - Robustness Test
Version 10- Coupled mathematical model
Version 11 Coupled Temporal Path Quantum Model & Projective Future Measurement Test
Version 13- Mathematical Model Showing no-signalling invariance under the tested future measurement channels
Version 14/15 Computetionl test of the proposed retrocausal/causal hypothesis no controllable retrocausal signalling detected

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