Substrate & Dielectric Loss =============================== Substrate and dielectric-loss outputs explain how material selection and surface participation affect T_1. .. list-table:: :header-rows: 1 * - # - Parameter - Symbol / Unit - Extraction Method - Typical Q3D Value - Ideal / Optimal - Good Range - Worst Case - Why It Matters - Key Design Note * - 40 - Substrate Bulk Loss Tangent - tan delta_bulk - Q3D dielectric loss tangent input; resonator Q fitting vs power - < 10⁻⁶ (HR-Si, 4K) - < 10⁻⁶ - 10⁻⁶ – 10⁻⁵ - > 10⁻⁴ - Bulk dielectric loss sets floor on 1/Q_int from substrate volume; sapphire < 5×10⁻⁷ - tan δ improves by 10–100× on cooling from 300K to 4K due to reduced phonon and TLS population * - 41 - Metal-Air Interface Loss (tan delta_MA) - tan delta_MA - Surface participation ratio (SPR) from Q3D E-field + measured Q factor - ~10⁻³ - < 10⁻³ (passivated Al₂O₃) - 10⁻³ – 5×10⁻³ - > 10⁻² - TLS loss at metal-air interface is the dominant T₁ source in planar transmon designs - Etching native oxide before Al deposition reduces tan delta_MA by up to 10×; HF vapor clean * - 42 - Substrate-Air Interface Loss (tan delta_SA) - tan delta_SA - SPR analysis from Q3D E-field distribution - ~5×10⁻⁴ - < 5×10⁻⁴ (HF-etched Si) - 5×10⁻⁴ – 5×10⁻³ - > 10⁻² - TLS at substrate exposed surface; addressed by passivation, UV ozone clean, or dry etching - Hydrogen-passivated Si surface (HF dip) shows 5× lower tan delta_SA vs untreated Si * - 43 - Metal-Substrate Interface Loss (tan delta_MS) - tan delta_MS - EELS/TEM interface composition + Q3D SPR calculation - ~5×10⁻³ - < 5×10⁻³ - 5×10⁻³ – 10⁻² - > 5×10⁻² - TLS at Al–Si or Nb–Si interface; reduced by HF dip substrate prep before metal deposition - Amorphous interfacial SiOx layer of 1–2 nm is the primary TLS host; substrate HF clean removes it * - 44 - Surface Participation Ratio (SPR) - p_MA / ppm - Q3D E-field energy integral on metal-air interface: p = ∫_MA ε\|E\|²dV / ∫_all ε\|E\|²dV - 5 – 50 ppm - < 5 ppm - 5 – 50 ppm - > 200 ppm - p × tan δ contributes directly to 1/Q; minimise by thick metal, wider gap, no sharp corners. For planar transmons, p_MA can reach 100–1000 ppm without geometry optimisation. - 1/Q_TLS = Σ p_i × tan δ_i; SPR is the design lever; tan δ is the material lever. <5 ppm ideal is achievable in optimised 3D cavity or large-gap planar designs; planar CPW without optimisation may be 100–1000 ppm.