boron doped epi

In-Situ Doped Epitaxy is the epitaxial growth process where dopant gases are introduced simultaneously with silicon or silicon-germanium precursors during source/drain or channel growth — allowing precisely controlled, electrically active dopant profiles to be incorporated directly into the epitaxial film without requiring a subsequent ion implantation step. In-situ doped epi enables dopant concentrations above solid solubility limits, abrupt junction profiles, and eliminates implant-induced crystal damage in the active device region.

Why In-Situ Doping Is Preferred

  • Traditional approach: Grow epi → then implant dopant into epi → anneal → activation.
  • Problem: Implant damages the epi crystal → increased defects → higher junction leakage.
  • In-situ solution: Dopants incorporated during growth → substitutionally placed → no damage → immediate activation → low junction leakage.
  • Benefit: Abrupt junction profiles achievable with epi thickness control (1–2 nm precision) rather than implant straggle.

Common Doped Epi Systems

Epi SystemDopantApplicationDopant Gas
Si:B (Boron-doped Si)BPMOS S/D (planar)B₂H₆ (diborane)
SiGe:BBPMOS FinFET/GAA S/DB₂H₆ + GeH₄
Si:P (Phosphorus-doped Si)PNMOS S/DPH₃ (phosphine)
Si:AsAsNMOS contact layerAsH₃ (arsine)
SiGe:C:BB, CPMOS — C suppresses B diffusionB₂H₆ + CH₃SiH₃
SiGe:PPNMOS — high-mobility Ge:PPH₃

Dopant Incorporation Mechanism

  • Dopant molecules (e.g., B₂H₆) decompose on the Si surface during CVD growth.
  • B atoms incorporate substitutionally at Si lattice sites → electrically active immediately.
  • Maximum active concentration: Exceeds solid solubility when grown by low-temperature epi (≤600°C) — kinetically frozen.
  • Typical peak concentrations: B in SiGe: 3–5 × 10²⁰ cm⁻³; P in Si: 2–4 × 10²¹ cm⁻³.

Carbon in SiGe:C:B (B-Diffusion Suppression)

  • Boron diffuses rapidly in SiGe during subsequent high-T steps → junction moves deeper → PMOS short-channel degraded.
  • Adding C (0.5–1.5% atomic) to SiGe reduces B diffusivity 10–100× by trapping vacancies.
  • SiGe:C:B epi: Compressive strain (from Ge) enhances hole mobility + C pins boron in place.
  • Used in SiGe HBT base layers for precise base doping control.

Selective vs. Blanket Epi

  • Selective epitaxy: Growth only on exposed Si surfaces (S/D regions) — no growth on SiO₂ or SiN.
  • Selectivity achieved by: HCl in growth gas (etches SiGe nuclei on oxide before they can grow).
  • Critical for S/D epi in FinFET/GAA: Must grow SiGe:B (PMOS) or Si:P (NMOS) only in recessed S/D trenches.

FinFET S/D Epi Process

1. S/D recess etch: Remove Si fin in S/D regions (~10–20 nm deep)
2. Pre-clean: HF-last clean to remove native oxide from Si surfaces
3. Epi load into CVD reactor (reduced pressure, 550–650°C)
4. Selective SiGe:B growth (PMOS) or Si:P growth (NMOS)
5. Multiple epi layers: Buffer + doped layer + cap (optimize shape and doping profile)
6. Merge between adjacent fins → creates continuous S/D region
7. No implant needed → clean crystal, abrupt junction

Metrology for Doped Epi

  • SIMS: Measures dopant concentration vs. depth — verifies peak dopant level and junction depth.
  • SRP (Spreading Resistance Profile): Electrical measurement of carrier concentration vs. depth.
  • TEM/EDX: Verifies Ge% and layer structure.
  • Rs (sheet resistance): Monitors activation and dopant incorporation uniformity.

In-situ doped epitaxy is the clean, crystallographically perfect alternative to implanting dopants into active device regions — by incorporating electrically active B and P during crystal growth rather than by damage-inducing ion bombardment, in-situ epi delivers the high carrier concentrations, abrupt junctions, and low defect densities that make PMOS and NMOS source-drain contacts at 5nm and below meet their drive current and reliability targets.

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