Loss & Dissipation¶
Loss & Dissipation Parameters: Dielectric, surface, radiation, and junction loss channels identified and weighted by EPR participations
Dielectric Loss (Bulk & Surface)
Parameter |
Symbol |
Unit |
Description |
Optimal / Best Value |
Good Range |
Acceptable Range |
Poor / Worst Value |
Physical Significance |
|---|---|---|---|---|---|---|---|---|
Bulk Substrate Loss Tangent |
tan delta_bulk |
dimensionless |
Intrinsic dielectric loss of the substrate material (Si, sapphire, SiO2); weighted by bulk EPR participation. |
< 1×10⁻⁷ (Si, sapphire) |
< 1×10⁻⁶ |
1×10⁻⁶ – 1×10⁻⁵ |
> 1×10⁻⁴ |
Silicon and sapphire are preferred substrates; amorphous SiO2 has tan δ ~ 10⁻³ (very poor). |
Metal-Substrate Interface Loss |
tan delta_MS |
dimensionless |
Effective loss tangent of metal–substrate (MS) two-level system (TLS) interface layer. |
< 1×10⁻³ |
< 3×10⁻³ |
3×10⁻³ – 1×10⁻² |
> 5×10⁻² |
MS interface is typically 2–5 nm thick oxide layer; dominant loss in many planar qubits. |
Substrate-Air Interface Loss |
tan delta_SA |
dimensionless |
Effective loss tangent of substrate–air (SA) interface; due to adsorbed surface oxides and organics. |
< 3×10⁻³ |
< 1×10⁻² |
1×10⁻² – 5×10⁻² |
> 0.1 |
Cleaning and surface passivation reduce SA loss; participation ratio from EPR isolates this channel. |
Metal-Air Interface Loss |
tan delta_MA |
dimensionless |
Effective loss tangent of metal–air (MA) interface; native oxide on superconducting film top surface. |
< 3×10⁻³ |
< 1×10⁻² |
1×10⁻² – 5×10⁻² |
> 0.1 |
Nb and Al form native oxides; replacing top surface with clean metal reduces MA loss. |
Surface Participation Ratio (MS) |
p_MS |
dimensionless |
Fraction of electric field energy in metal-substrate interface region; computed from EPR E-field. |
< 5×10⁻⁴ |
< 2×10⁻³ |
2×10⁻³ – 1×10⁻² |
> 5×10⁻² |
Thinner gaps increase p_MS; EPR identifies geometry changes to reduce interface participation. |
TLS-Limited Quality Factor (1/f) |
Q_TLS |
dimensionless |
Quality factor limited by two-level system (TLS) bath; power- and temperature-dependent. |
> 3×10⁶ |
10⁶ – 3×10⁶ |
10⁵ – 10⁶ |
< 10⁴ |
Q_TLS improves with high drive power (TLS saturation); EPR participations give TLS contribution breakdown. |
Radiation & Geometry Loss
Parameter |
Symbol |
Unit |
Description |
Optimal / Best Value |
Good Range |
Acceptable Range |
Poor / Worst Value |
Physical Significance |
|---|---|---|---|---|---|---|---|---|
Radiation Loss Rate |
gamma_rad / 2pi |
kHz |
Energy loss due to electromagnetic radiation from non-closed geometry; computed by EPR from far-field. |
< 1 kHz |
< 10 kHz |
10 – 100 kHz |
> 500 kHz |
Open transmission line stubs or poorly designed ground planes lead to radiation loss. |
Seam Loss (3D cavities) |
gamma_seam / 2pi |
kHz |
Loss at mechanical seam between cavity halves; critical for 3D transmon and fluxonium devices. |
< 1 kHz |
< 5 kHz |
5 – 50 kHz |
> 200 kHz |
EPR current participation at seam predicts seam loss; improved by indium bonding or tight tolerances. |
Quasiparticle Loss Rate |
gamma_qp / 2pi |
kHz |
Qubit decay due to nonequilibrium quasiparticles tunneling across junction. |
< 2 kHz |
< 20 kHz |
20 – 100 kHz |
> 500 kHz |
Quasiparticle poisoning is stochastic; mitigated by gap engineering and quasiparticle traps. |
Vortex Loss (in-field operation) |
gamma_vortex / 2pi |
kHz |
Loss from magnetic vortices in superconducting film when operated in residual magnetic field. |
< 1 kHz (< 1 µT shield) |
< 10 kHz |
10 – 100 kHz |
> 500 kHz |
Mitigated by magnetic shielding and moat structures; EPR current maps identify vortex-sensitive areas. |
Conductor (Ohmic) Loss |
gamma_ohm / 2pi |
kHz |
Residual ohmic loss from non-superconducting regions or above Tc contributions; usually negligible in Al. |
< 0.1 kHz |
< 1 kHz |
1 – 10 kHz |
> 100 kHz |
Typically negligible at mK temperatures; relevant for normal-metal contacts or resistive wirebonds. |