40nm BSI CMOS Image SensorPreview

HKD/AR1 AlO deposition

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HKD/AR2 TaO deposition

BPMD SiO Deposition
298Oxide hard mask deposition299Pre Litho Cleaning300Backside Passivation Implant Mask Lithography301Back Passivation Ion Implantation302Ashing & Strip/Clean303Oxide hard mask etch304Vacuum Bake305Rapid Thermal Processing306RF Plasma307HKD/AR1 AlO deposition308HKD/AR2 TaO deposition309BPMD SiO Deposition

Process Cross-Section

ISP WaferCIS Wafer · BacksideBKPAS · K11 · HKD/AR2 TaO DepositionTaOAlOP+ implanted regionSiCESLSiO2CuTaAlSiN

Step highlight

The deposition is typically executed via Atomic Layer Deposition (ALD), leveraging surface self-limiting chemical reactions where each cycle forms only a sub-monolayer, enabling atomic-level thickness control .

In depth

In Backside Illuminated (BSI) CMOS Image Sensors, photons enter through the thinned ba

ckside silicon surface, making interface reflection a primary source of optical loss . To maximize optical quantum efficiency, a multi-layer Anti-Reflective Coating (ARC) is required to bridge the refractive index gap between the silicon substrate and the external environment . The HKD/AR2 Tantalum Oxide (TaO) deposition immediately follows the AlO (AR1) layer and precedes the SiO (BPMD) deposition . This specific ordering of dielectric layers with strongly differing refractive indices actively controls the phase and energy of reflected light to suppress Fresnel reflections at the interfaces . Furthermore, high-k dielectrics like TaO contribute to structural passivation, complementing the field-effect passivation provided by the underlying AlO layer . The core mechanism of this step relies on thin-film optics and phase cancellation . When light crosses media with differing refractive indices, multiple reflections generate interference phenomena . By precisely controlling the physical thickness and refractive index of the TaO film, the light reflected from the TaO interfaces acquires a 180° phase difference relative to other reflected waves, producing destructive interference . The deposition is typically executed via Atomic Layer Deposition (ALD), leveraging surface self-limiting chemical reactions where each cycle forms only a sub-monolayer, enabling atomic-level thickness control . This extreme conformality ensures uniform optical path lengths across the entire wafer, which is critical because production tolerances and thickness non-uniformities drastically alter the optical quantum efficiency for different wavelengths . TaO is selected for the AR2 layer primarily due to its high refractive index and transparency in the visible spectrum, which are essential properties for optical coatings . Additionally, TaO is a well-characterized high-k dielectric material known for its superior bulk dielectric properties . In a multi-layer ARC stack, tuning the process gas ratios and deposition temperature directly modulates the film's density, which in turn defines its refractive index (n) and extinction coefficient (k) . These optical constants must be rigorously optimized to achieve a minimum reflectivity across the wide spectrum of visible light absorbed by the underlying silicon photodiodes . The use of a purely deposition-based ALD approach, rather than plasma-heavy techniques, significantly reduces high-energy ion bombardment damage to functional interfaces . At the 40nm BSI node, pixel sizes are highly scaled, demanding exceptional photon capture efficiency because the physical area available for light absorption is minimized . Maintaining low interface state density is paramount, as defects act as recombination centers or thermal generation sites that manifest as dark current . By utilizing highly conformal, low-damage deposition techniques, the process preserves the structural integrity of the active pixel regions . The combination of AlO, TaO, and SiO provides a tailored optical index gradient that mitigates the severe standing waves and transmission losses that occur in sub-wavelength photonics .

Risks & Challenges

  • [High] Optical Thickness Mismatch: Drift in deposition cycle rates alters the physical thickness of the TaO layer, disrupting the quarter-wave phase cancellation condition . This failure causes constructive rather than destructive interference, sharply increasing interface reflectivity and degrading the sensor's optical quantum efficiency .
  • [Medium] Impurity-Induced Optical Absorption: Incomplete surface reactions during the ALD process leave precursor ligands trapped within the TaO film . These impurities create defect states that alter the material's extinction coefficient (k), leading to parasitic optical absorption and reduced photon transmission .
  • [Medium] Interfacial Layer Formation: If the thermal budget is too high, the TaO layer may react with adjacent materials to form uncontrolled interfacial silicate layers . This unintended interfacial layer changes the effective optical stack, inducing wavelength-dependent reflection variations across the wafer .
  • [Low] Plasma Damage to Passivation: If an assisting plasma is used during deposition, excessive power can cause high-energy ion bombardment damage to the underlying functional layers . This damage generates interface states that increase subthreshold leakage and dark current in the highly scaled photodiodes .

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Related steps

  • Oxide hard mask deposition
  • Pre Litho Cleaning
  • Backside Passivation Implant Mask Lithography
  • Back Passivation Ion Implantation
  • Ashing & Strip/Clean
  • Oxide hard mask etch