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Strong coupling between propagating spin waves and microwave photons in superconducting resonator-magnetic thin film hybrid circuits. Design methodology for hybrid magnonic quantum systems using YIG-on-substrate integration.
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| name | spin-wave-superconducting-coupling |
| description | Strong coupling between propagating spin waves and microwave photons in superconducting resonator-magnetic thin film hybrid circuits. Design methodology for hybrid magnonic quantum systems using YIG-on-substrate integration. |
| tags | ["quantum","magnonics","spin-wave","superconducting-resonator","hybrid-systems","YIG","microwave-photon","cavity-magnonics","nonreciprocity","Damon-Eshbach","quantum-information"] |
| trigger_words | spin wave coupling, superconducting magnon, YIG resonator, propagating spin wave, microwave photon coupling, Damon-Eshbach mode, backward-volume spin wave, hybrid magnonic system, cavity magnonics, nonreciprocal spin wave, rare-earth-free substrate |
Design methodology for achieving strong coupling between propagating spin wave (magnon) modes and microwave photons in superconducting resonator-magnetic thin film hybrid circuits. Enables integration of spin-wave magnonics with cavity magnonics for quantum information science applications.
Based on: "Strong coupling between propagating spin wave and microwave photons in a superconducting resonator" (arXiv:2606.27279)
The system achieves strong coupling when:
g > κ_m, κ_c, γ
Where:
Strong coupling enables:
┌─────────────────────────────────┐
│ Superconducting Resonator │ ← Nb/Al superconducting film
├─────────────────────────────────┤
│ YIG Thin Film (Y₃Fe₅O₁₂) │ ← Magnetically active layer
├─────────────────────────────────┤
│ Y₃Sc₂Ga₃O₁₂ (YSGO) Substrate │ ← Rare-earth-free, lattice-matched
└─────────────────────────────────┘
| Mode Type | Propagation | Coupling Characteristics |
|---|---|---|
| Damon-Eshbach (DE) | Surface wave, unidirectional | Strongest coupling, exhibits nonreciprocity |
| Backward-Volume (BV) | Volume wave, bidirectional | Weaker coupling but broader bandwidth |
| Magnetostatic Forward Volume | Bulk propagation | Intermediate characteristics |
In the Damon-Eshbach configuration:
g ∝ √(N_magnons) × γ_magnon-photon × √(ω_cavity)
| Loss Channel | Typical Value | Mitigation |
|---|---|---|
| Magnon damping (κ_m/2π) | ~1 MHz | High-quality YIG, surface passivation |
| Cavity loss (κ_c/2π) | ~0.1 MHz | Superconducting materials, geometric optimization |
| Spin wave propagation loss | ~1 dB/mm | Film thickness, surface roughness control |
| Two-level system (TLS) loss | ~0.01-0.1 MHz | Substrate cleaning, interface optimization |
| Application | Configuration | Key Metric |
|---|---|---|
| Quantum memory | DE mode coupling | Coherence time > 1 μs |
| Quantum transducer | BV mode + optical conversion | Conversion efficiency > 1% |
| Quantum isolator | DE nonreciprocity | Isolation > 20 dB |
| Magnonic quantum processor | Multi-mode coupling | Mode count > 10, g/2π > 10 MHz |
| Hybrid quantum network | Spin wave bus | Propagation distance > 1 mm |
quantum-network-transduction - Quantum signal conversionnon-hermitian-cv-quantum-control - Non-Hermitian control methodsquantum-hybrid-neural-computing - Hybrid quantum systemsKeywords: spin wave coupling, superconducting magnon, YIG resonator, propagating spin wave, microwave photon coupling, Damon-Eshbach mode, backward-volume spin wave, hybrid magnonic system, cavity magnonics, nonreciprocal spin wave, rare-earth-free substrate, YSGO substrate