John Bollinger | December 2025
Framework #6 β Coherence Telephone
Objective: Detect topology-specific, non-classical correlation between EΒ·B modulation and coherence-sensitive observables, under conditions that rule out conventional electromagnetic coupling.
Two topologically-matched systems (Chern number π=3) will exhibit a measurable correlation in response to EΒ·B modulation that is absent when their topologies are mismatched.
The kill shot: Same signal for matched AND mismatched = classical leakage (theory fails).
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β SINGLE DILUTION REFRIGERATOR β
β (Base T < 20 mK) β
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β β
β βββββββββββββββββββ βββββββββββββββββββ β
β β SOURCE NODE β β DETECTOR NODE β β
β β (A) β SHIELDED β (B) β β
β β β BARRIER β β β
β β βββββββββββββ β β β βββββββββββββ β β
β β β π = 3 β β β β β π = 3 β β β
β β β Array β β β β β Array β β β
β β βββββββ¬ββββββ β β β βββββββ¬ββββββ β β
β β β β β β β β β
β β βββββββΌββββββ β β β βββββββΌββββββ β β
β β β Microwave β β β β β Readout β β β
β β β Cavity β β β β β Qubit β β β
β β βββββββ¬ββββββ β β β βββββββ¬ββββββ β β
β β β β β β β β β
β β βββββββΌββββββ β β β βββββββΌββββββ β β
β β βEΒ·B Drive β β β β β Resonator β β β
β β β (Ο_d, ΞΈβ) β β β β β (Readout) β β β
β β βββββββββββββ β β β βββββββββββββ β β
β β β β β β β
β ββββββββββ¬βββββββββ β ββββββββββ¬βββββββββ β
β β β β β
β βββββββββββββββββ«βββββββββββββββββ β
β β β
β βββββββββΌββββββββ β
β β CONTROL & β β
β β DATA β β
β β ACQUISITION β β
β βββββββββββββββββ β
β β
ββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββ
Key Design Principle: Both nodes in separately shielded compartments within the same cryostat. Millikelvin temperatures with precise isolation control.
| Parameter | Specification | Notes |
|---|---|---|
| Platform | Superconducting qubit array | Google Sycamore / Quantinuum H2 techniques |
| Topology | Tunable Chern insulator | In-situ tunable to π = 2, 3, 4 |
| Verification | Quantized Hall conductance | Confirms topological phase |
| Coherence | Tβ* > 50 ΞΌs | State-of-the-art transmon |
Critical requirement: Arrays must be tunable in-situ between Chern numbers for control experiments.
| Component | Specification | Purpose |
|---|---|---|
| Cavity | High-Q 3D microwave, Ο_c/2Ο ~ 6-8 GHz | Resonant enhancement |
| EΒ·B Modulator | Orthogonal antenna/coil pair | Crossed E and B fields |
| Drive signal | Coherent tone at Ο_d | δθ(t) = ΞΈβ cos(Ο_d t) |
| Control knob | ΞΈβ amplitude | Primary experimental variable |
| Component | Specification | Purpose |
|---|---|---|
| Readout qubit | High-coherence transmon (Tβ* > 50 ΞΌs) | Frequency shift sensor |
| Coupling | Dispersive to π=3 array | Coherence field β qubit shift |
| Resonator | Standard readout circuit | QND measurement |
| Measurement | Ramsey interferometry | Precise frequency determination |
| System | Specification | Purpose |
|---|---|---|
| Cryostat | Dilution refrigerator, T < 20 mK | Quantum coherence |
| Magnetic shield | Cryoperm + superconducting Al | Field isolation |
| RF shield | Separate enclosures per node | EM isolation |
| Control | Phase-locked ΞΌW generators | Timing precision |
| DAQ | Ultra-low-noise digitizers | Signal acquisition |
βββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββ
β 1.1 Cool system to base temperature (< 20 mK) β
β 1.2 Tune BOTH arrays to π = 3 β
β 1.3 Verify topology via transport or spectroscopy β
β 1.4 Calibrate EΒ·B drive amplitude ΞΈβ (radians) β
β 1.5 Calibrate dispersive shift Οβ (qubit + array ground) β
β 1.6 Measure noise floor (no drive) β
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Configuration: Source π = 3, Detector π = 3 (MATCHED)
For shot i = 1 to N_shot:
2.1 INITIALIZE
ββ Prepare both arrays in ground state
ββ Reset readout qubit
2.2 MODULATE
ββ Apply EΒ·B drive δθ(t) = ΞΈβ cos(Ο_d t) at Node A
ββ Duration: T_pulse = 1-10 ΞΌs
2.3 MEASURE
ββ Ramsey sequence on readout qubit (Node B)
ββ Extract frequency shift Οα΅’
2.4 RECORD
ββ Store (timestamp, ΞΈ(t), Οα΅’)
Accumulate N_shot = 10β΄ to 10βΆ measurements
Configuration: Source π = 2, Detector π = 3 (MISMATCHED)
3.1 Re-tune Source Node A to π = 2
ββ Detector Node B remains at π = 3
3.2 Repeat EXACTLY the same sequence as Step 2
3.3 Expected result (if hypothesis correct):
ββ Correlated shift Ο(t) β ZERO (noise floor only)
| Control | Procedure | Purpose |
|---|---|---|
| 4.1 RF Shunting | Disconnect all ΞΌW lines to Node B during modulation | Rule out EM crosstalk |
| 4.2 Frequency Detuning | Set Ο_d far off any resonance | Rule out cavity coupling |
| 4.3 Thermal Test | Replace coherent drive with heating pulse | Rule out thermal effects |
| 4.4 Time Reversal | Swap source/detector roles | Verify symmetry |
Data matrix D[i, t]:
i = shot index (1 to N_shot)
t = time bin
D[i, t] = {
ΞΈ(t) : Drive envelope at time t
Οα΅’(t) : Measured frequency shift
config: Topology configuration (3-3 or 2-3)
}
Compute cross-correlation between drive and response:
Predicted outcomes:
| Configuration | C(0) Prediction | Physical Meaning |
|---|---|---|
| π=3 β π=3 (matched) | Strong peak | Topology-mediated coupling |
| π=2 β π=3 (mismatched) | Zero (noise) | No coupling (different channel) |
| Metric | Formula | Purpose |
|---|---|---|
| Selectivity ratio | S = C(0)_matched / Ο_mismatched | Topology discrimination |
| SNR | Ο_peak / Ο_noise | Detection significance |
| p-value | From null hypothesis test | Statistical confidence |
The experiment is a SUCCESS if ALL of the following are true:
| Criterion | Threshold | Meaning |
|---|---|---|
| Matched signal | p-value < 10β»β΅ (β₯ 4.4Ο) | Real correlation detected |
| Control null | p-value > 0.05 | No signal in mismatched case |
| Selectivity | S > 5 | Clear topology discrimination |
| Reproducibility | 3+ independent runs | Not a statistical fluke |
The experiment FAILS (falsifies hypothesis) if:
| Failure Mode | Observation | Interpretation |
|---|---|---|
| Classical leakage | Equal signal in matched AND mismatched | EM crosstalk, not topology |
| Null result | No signal in either condition | Coupling too weak or mechanism wrong |
| Inconsistent | Non-reproducible results | Systematic error |
| Matched (3-3) | Mismatched (2-3) | Interpretation | Next Step |
|---|---|---|---|
| β Strong | β Zero | HYPOTHESIS SUPPORTED | Proceed to Phase 2 |
| β Strong | β Strong | CLASSICAL LEAKAGE | Improve shielding or abandon |
| β Zero | β Zero | NULL RESULT | Increase sensitivity or abandon |
| β Zero | β Strong | ANOMALOUS | Investigate systematic error |
| Role | Responsibility | FTE |
|---|---|---|
| PI (Theorist) | Framework, analysis, interpretation | 0.5 |
| Experimentalist | Cryogenics, qubit fabrication, measurement | 1.0 |
| Technician | Fabrication, cooldown support | 0.5 |
| Postdoc/Student | Data acquisition, analysis | 1.0 |
Month 1-3: DESIGN & PROCUREMENT
ββ Finalize component specs
ββ Procure/fabricate arrays and cavities
ββ Prepare control software
Month 4-6: INTEGRATION & CALIBRATION
ββ Cooldown and system characterization
ββ Tune arrays to target Chern numbers
ββ Calibrate all drives and readout
Month 7-9: DATA COLLECTION
ββ Primary matched-topology experiment
ββ Control experiments (mismatched, shunted, etc.)
ββ Statistical accumulation
Month 10-12: ANALYSIS & PUBLICATION
ββ Data analysis and interpretation
ββ Manuscript preparation
ββ Peer review submission
| Requirement | Specification | Potential Sites |
|---|---|---|
| Dilution refrigerator | < 20 mK base, advanced ΞΌW control | University labs, NHMFL |
| Qubit fabrication | Transmon + tunable arrays | IBM, Google, academic fabs |
| Shielding | Multi-layer magnetic + RF | Standard cryogenic practice |
| Risk | Probability | Impact | Mitigation |
|---|---|---|---|
| Insufficient isolation | Medium | High | Multiple shielding layers, separate enclosures |
| Topology not tunable | Low | Critical | Pre-characterize arrays before cooldown |
| Signal below noise | Medium | High | Optimize photon number n, integration time |
| Qubit decoherence | Low | Medium | Use state-of-the-art fabrication |
| Systematic errors | Medium | Medium | Extensive control experiments |
Dataset: Cross-correlation C(0) for matched vs. mismatched topology configurations, with full statistical analysis.
Title: "Search for Topology-Mediated Coherence Field Coupling in a Tunable Chern Insulator Array"
Structure:
- Introduction: Coherence field hypothesis and predictions
- Theory: Signal formula Ο = (Ξ±/2Ο)(gβΒ²/Ξ)(gΞΈβ/m)n
- Methods: This protocol
- Results: Cross-correlation analysis
- Discussion: Interpretation and implications
- Conclusion: Support/refutation of hypothesis
Phase 2 objective: Increase spatial separation to separate cryostats (meters apart) while maintaining millikelvin temperatures.
Phase 3 objective: Earth-Moon test for faster-than-light correlation (the ultimate kill shot).
This protocol tests the predictions from PREDICTIONS_SIGNAL_STRENGTH.md:
| Prediction | Protocol Test | Success Criterion |
|---|---|---|
| P1: Topology addressing | Step 2 vs Step 3 | Signal only in matched case |
| P2: Linear scaling | Vary ΞΈβ | Ο β ΞΈβ |
| P3: Resonance | Sweep Ο_d | Peak at Ο_d = m |
| P5: CΒ² scaling | Vary Chern number | Signal β πΒ² |
Modulate EΒ·B at a π=3 source, measure qubit frequency shift at a π=3 detector, and verify the signal vanishes when source is changed to π=2.
Strong correlation for matched topology (>4.4Ο), zero correlation for mismatched topology (>5Γ selectivity).
Equal signal in both configurations = classical leakage = theory falsified.
| Parameter | Symbol | Typical Value | Units |
|---|---|---|---|
| Fine structure constant | Ξ± | 1/137 | β |
| Vacuum Rabi coupling | gβ/2Ο | 50-200 | MHz |
| Qubit-cavity detuning | Ξ/2Ο | 1-5 | GHz |
| Drive amplitude | ΞΈβ | 0.1-0.5 | rad |
| Photon number | n | 10Β³-10βΆ | β |
| Qubit dephasing time | Tβ* | >50 | ΞΌs |
| Base temperature | T | <20 | mK |
| Chern number (matched) | π | 3 | β |
| Chern number (control) | π | 2 | β |
From PREDICTIONS_SIGNAL_STRENGTH.md:
| g/m (radβ»ΒΉ) | Ο (Hz) | Integration | Feasibility |
|---|---|---|---|
| 10β»Β³ | 290 | ~120 ms | β Easy |
| 10β»β΄ | 29 | ~12 s | β Feasible |
| 10β»β΅ | 2.9 | ~20 min | β Doable |
| 10β»βΆ | 0.29 | ~1.4 days | |
| 10β»βΉ | β | β | β Falsified |
"This protocol turns equations into measurements. If it works, we've found something real. If it fails cleanly, we've learned something true."
β John Bollinger, December 2025