Thick gate oxide growth forms a dense Si–O network at the fin surface, reducing electric field stress .
The Thick Gate Oxide Growth step is inserted after fin definition and post‑etch cleaning to establish a robust electrical and chemical isolation layer between the fin channel and the subsequent dummy gate structure in a 7 nm HKMG FinFET flow . This step creates a deliberately thicker dielectric than the core logic gate oxide to support devices t
hat experience higher electric field stress, such as I/O or protection transistors, while also serving as a sacrificial or protective oxide during dummy gate integration . By performing this step before dummy gate amorphous silicon deposition, the process ensures that the fin sidewalls and top surfaces are uniformly passivated, which stabilizes subsequent gate patterning, CMP, and replacement gate steps . From a flow‑integration perspective, this oxide acts as a structural and electrical buffer that decouples fin surface conditions from the mechanical and chemical stresses introduced during dummy gate deposition and planarization . The preceding post‑etch clean removes native oxide and etch residues, enabling controlled re‑oxidation or deposition with predictable interfacial chemistry, which is essential for threshold and reliability uniformity across fins . Unlike later Dual Gate Oxide Lithography steps that locally tailor oxide thickness by patterning, this step establishes a baseline thick oxide over the entire active region, making it foundational rather than selective .
The fundamental mechanism of thick gate oxide formation in advanced FinFETs relies on controlled oxidation or deposited oxide growth that passivates silicon dangling bonds and forms a dense Si–O network at the fin surface . In deposition‑based implementations such as ALD SiO₂, self‑limiting surface reactions sequentially saturate available hydroxyl or dangling bond sites, leading to uniform coverage on three‑dimensional fin sidewalls and STI corners . This surface‑reaction‑limited regime explains why conformality is preserved even in high‑aspect‑ratio FinFET geometries, unlike gas‑phase‑reaction‑limited CVD processes . From a device‑physics standpoint, increasing the physical thickness of the gate oxide reduces the electric field for a given applied voltage according to the relation E = V/t, thereby suppressing defect generation and time‑dependent dielectric breakdown (TDDB) under high‑field operation . The oxide quality is therefore governed not only by thickness but also by interfacial defect density, since interface traps modulate surface potential control and accelerate breakdown through trap‑assisted tunneling mechanisms . Post‑growth or in‑situ treatments such as nitridation further modify the chemical bonding environment by replacing weaker Si–O bonds or oxygen vacancies with stronger Si–N bonds, directly reducing trap generation rates under electrical stress .
Deposited oxides, particularly ALD SiO₂, are favored over purely thermal oxidation for thick gate applications in FinFETs because they avoid excessive consumption of the fin channel material and maintain fin geometry integrity . This consideration is especially critical when alternative channels such as SiGe are present, since thermal oxidation would preferentially oxidize Ge and degrade strain and mobility, a failure mode documented in advanced fin structures . The high conformality and atomic‑scale thickness control inherent to ALD directly address the three‑dimensional topology of 7 nm fins, ensuring that oxide thickness variations do not translate into local electric‑field hotspots . Process parameters interact primarily through surface chemistry and defect physics rather than simple thickness scaling, as higher deposition or oxidation aggressiveness generally improves film density but can also enhance impurity incorporation or interfacial layer regrowth . Similarly, nitridation strength and thermal budget trade off interface state reduction against potential fixed charge introduction, which in turn shifts flat‑band and threshold voltages as described by MOS electrostatics . The chosen method therefore reflects a balance between dielectric robustness, interface quality, and downstream compatibility with high‑k/metal gate stacks, where an interfacial SiO₂‑like layer is still required for mobility and reliability reasons .
At the 7 nm node, the fin width and height amplify sensitivity to any non‑uniform oxide growth, making conformality and interface control far more critical than in planar technologies . The presence of HKMG integration further constrains this step, since oxygen redistribution during later high‑k and metal gate processing can regrow or modify the interfacial oxide if its initial quality is poor, directly impacting equivalent oxide thickness and threshold stability . As a result, the thick gate oxide grown at this stage must be chemically stable and defect‑lean to survive subsequent thermal cycles without excessive interfacial layer evolution, a requirement that differentiates it from simpler pad oxide growth earlier in the flow . In contrast to Pad Oxide Growth, which primarily serves as an etch buffer and stress relief layer during STI formation, this Thick Gate Oxide Growth step is electrically functional and directly tied to gate reliability and device operation . It also differs from Dual Gate Oxide Lithography steps, which selectively thin or thicken oxides for multi‑Vt or I/O differentiation, whereas this step establishes the uniform foundational dielectric needed before any gate patterning occurs .
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