Qubit Performance Metrics¶
HFSS-derived qubit checks for frequency, anharmonicity, energy scales, coherence, Purcell decay, and gate fidelity.
# |
VER ID |
Parameter |
Severity |
Design Rule / Constraint |
Ideal / Optimal Value |
Acceptable Range |
Good |
Bad |
Why It Matters |
|---|---|---|---|---|---|---|---|---|---|
26 |
HFSS-Q-001 |
Anharmonicity α |
Critical |
|α|/2π ≥ 150 MHz (|α| = |ω₁₂ − ω₀₁|) |
−200 to −300 MHz |
−100 to −500 MHz |
|α| 200–300 MHz: DRAG gates < 30 ns with leakage < 0.01%; selective driving |
|α| < 50 MHz: must slow gates to > 200 ns; leakage to |2⟩ > 1% |
Frequency gap between 0→1 and 1→2 transitions. Must exceed pulse bandwidth for selective driving without leakage. |
27 |
HFSS-Q-002 |
Qubit Frequency f_q |
Critical |
4.0 GHz ≤ f_q ≤ 6.0 GHz (transmon sweet spot) |
4 – 6 GHz |
3 – 8 GHz |
4–6 GHz: kT/hf < 0.001 at 20 mK; standard microwave hardware |
< 1 GHz: thermal population > 1%; > 10 GHz: substrate loss increases |
Qubit transition frequency. Must be well above thermal energy (kT/h ≈ 400 MHz at 20 mK) and away from substrate TLS resonances. |
28 |
HFSS-Q-003 |
Josephson Energy E_J |
Critical |
10 GHz ≤ E_J/h ≤ 40 GHz; E_J/E_C ≥ 50 |
15 – 30 GHz |
5 – 60 GHz |
15–30 GHz: f_q on target; charge insensitive; junction reproducible within ±5% |
< 1 GHz: qubit below 2 GHz; thermally excited; E_J/E_C < 10: charge sensitive |
Josephson tunneling energy sets qubit frequency and E_J/E_C ratio. Extracted in HFSS via junction inductance L_J = Φ₀²/E_J. |
29 |
HFSS-Q-004 |
Charging Energy E_C |
Critical |
200 MHz ≤ E_C/h ≤ 350 MHz |
200 – 350 MHz |
100 – 500 MHz |
200–350 MHz: anharmonicity ~−E_C; charge noise suppressed; qubit addressable |
< 50 MHz: near-harmonic oscillator; > 1000 MHz: Cooper-pair box regime |
Single-electron charging energy set by shunt capacitance. E_C = e²/2C_Σ; defines anharmonicity and charge sensitivity. |
30 |
HFSS-Q-005 |
Purcell Decay Rate γ_P |
Critical |
γ_P/2π < 1 kHz (without filter); < 100 Hz (with) |
< 500 Hz |
< 10 kHz |
< 500 Hz: Purcell T₁ contribution > 2 ms; does not limit qubit T₁ budget |
> 100 kHz: Purcell T₁ < 10 µs; qubit lifetime dominated by readout line |
Qubit decay rate into transmission line via off-resonant resonator. γ_P = (g/Δ)²κ. Limits T₁ without Purcell filter. |
31 |
HFSS-Q-006 |
Predicted T₁ |
Critical |
T₁ > 100 µs (planar 2D); > 1 ms (3D cavity) |
> 500 µs (3D) / > 100 µs (2D) |
50 – 500 µs |
> 100 µs: supports > 1000 gate depth within coherence envelope (10 ns gates) |
< 10 µs: < 100 gates within T₁; fault-tolerant computation infeasible |
Predicted energy relaxation time from HFSS loss model: 1/T₁ = Σ(pᵢ × ωᵢ × tan δᵢ) + γ_Purcell + γ_radiation. |
32 |
HFSS-Q-007 |
Predicted T₂ |
Critical |
T₂ > 50 µs; ideally T₂ ≈ 2T₁ (pure dephasing limited) |
> 100 µs |
20 – 300 µs |
T₂ ≈ 2T₁: pure dephasing negligible; charge and flux noise well-suppressed |
T₂ ≪ T₁: strong 1/f dephasing; substrate charge traps or flux noise dominant |
Pure dephasing time. Gap between T₂ and 2T₁ quantifies 1/f noise from TLS charge noise and flux noise in junctions. |
33 |
HFSS-Q-008 |
1Q Gate Fidelity F₁Q |
Critical |
F₁Q ≥ 99.9% (randomised benchmarking) |
> 99.9 % |
99 – 99.99 % |
> 99.9%: below surface-code fault-tolerance threshold (~99.4%); QEC viable |
< 99%: error rate exceeds fault-tolerance threshold; errors cascade in QEC |
Single-qubit gate fidelity estimated from T₁, T₂, anharmonicity, and leakage. Must exceed fault-tolerant threshold ~99.5%. |
34 |
HFSS-Q-009 |
2Q Gate Fidelity F₂Q |
Critical |
F₂Q ≥ 99.5% (CZ or iSWAP gate) |
> 99.5 % |
98 – 99.9 % |
> 99.5%: viable for surface code with standard overhead; ZZ residual < 10 kHz |
< 97%: excessive error rate; 2Q errors dominate total circuit error budget |
Two-qubit gate fidelity. More sensitive to residual ZZ coupling, leakage, coupler calibration, and neighbouring qubit crosstalk. |