Resonator & Coupling¶
Resonator & Coupling Parameters: Readout and bus resonator characteristics plus qubit-resonator coupling extracted via EPR
Resonator Properties
Parameter |
Symbol |
Unit |
Description |
Optimal / Best Value |
Good Range |
Acceptable Range |
Poor / Worst Value |
Physical Significance |
|---|---|---|---|---|---|---|---|---|
Resonator Frequency |
omega_r / 2pi |
GHz |
Bare resonator frequency; should be detuned from qubit to remain in dispersive regime. |
6.5 – 8.5 GHz |
5 – 10 GHz |
3 – 5 GHz |
< 2 GHz |
Must satisfy |Δ| = |ω_q - ω_r| > > g for dispersive approximation; EPR gives bare frequency. |
Resonator Internal Q |
Q_int |
dimensionless |
Internal (material-limited) quality factor of the readout resonator. |
> 10⁵ |
10⁴ – 10⁵ |
10³ – 10⁴ |
< 500 |
Low Q_int adds photon loss increasing measurement back-action and reducing readout SNR. |
Resonator External Q |
Q_ext |
dimensionless |
External quality factor set by coupling to transmission line; determines measurement bandwidth. |
10³ – 10⁴ (fast readout) |
500 – 2×10⁴ |
50 – 499 |
< 50 |
Too high → slow readout; too low → Purcell-enhanced qubit decay. Optimized with Purcell filter. |
Resonator–Qubit Detuning |Δ| |
|Δ|/2π |
GHz |
Frequency detuning between qubit and resonator; must be large compared to coupling g. |
1.0 – 3.0 GHz |
0.5 – 4.0 GHz |
0.1 – 0.5 GHz |
< 0.05 GHz |
Small detuning violates dispersive approximation; EPR hybridization factor chi tracks this. |
Purcell Decay Rate |
γ_P/2π |
kHz |
Qubit decay rate via resonator Purcell channel; κ * (g/Δ)². Must be < < 1/T1_target. |
< 1 kHz |
1 – 10 kHz |
10 – 100 kHz |
> 500 kHz |
Dominant T_1 limit in many designs without Purcell filter; directly predicted by EPR p_J^res. |
Coupling Strengths
Parameter |
Symbol |
Unit |
Description |
Optimal / Best Value |
Good Range |
Acceptable Range |
Poor / Worst Value |
Physical Significance |
|---|---|---|---|---|---|---|---|---|
Transverse Coupling g / 2pi |
g / 2pi |
MHz |
Qubit-resonator coupling strength (Jaynes-Cummings); extracted from EPR as g = √(p_J^res * ω_r * ω_q / 2). |
50 – 150 MHz |
20 – 200 MHz |
5 – 19 MHz |
< 2 MHz |
Sets χ and readout speed; g/|Δ| < 0.1 required for dispersive regime. |
Dispersive Coupling g/Δ ratio |
g/|Δ| |
dimensionless |
Dimensionless ratio quantifying proximity to strong-coupling limit; must be < < 1 for dispersive readout. |
0.01 – 0.05 |
0.005 – 0.09 |
0.09 – 0.15 |
> 0.20 |
Ratio > 0.1 causes photon-number-dependent qubit dephasing and higher-order dispersive corrections. |
Bus Coupler Coupling (2Q) |
J / 2pi |
MHz |
Exchange coupling between two qubits via bus resonator or direct capacitance. |
5 – 20 MHz |
2 – 30 MHz |
0.5 – 1.9 MHz |
< 0.1 MHz |
Too weak → slow two-qubit gates; too strong → residual ZZ. EPR predicts J from geometry. |
Residual ZZ (static) |
zeta_ZZ / 2pi |
kHz |
Always-on longitudinal (ZZ) qubit–qubit interaction; source of conditional phase errors. |
< 10 kHz |
< 100 kHz |
100 – 500 kHz |
> 1 MHz |
Limits two-qubit gate fidelity via conditional phase accumulation; minimized by tunable couplers. |
Stray Coupling (nearest-neighbor) |
J_stray / 2pi |
kHz |
Unintended coupling between non-adjacent qubits; extracted from full-chip EPR simulation. |
< 10 kHz |
< 50 kHz |
50 – 200 kHz |
> 500 kHz |
Degrades multi-qubit gate fidelity; EPR full-chip simulation essential to identify stray modes. |