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ILD0 DED First Deposition

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150ILD0 DED First Deposition
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Process Cross-Section

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Step highlight

The ILD0 DED First Deposition forms a conformal dielectric layer on nitride and silicon surfaces, filling recesses and partially leveling topography to enable subsequent contact etching without exposing underlying structures .

In depth

Device Context and Integration Logic

The ILD0 DED First Deposition step introduces the first interlayer dielectric immediately after CESL nitride formation, creating a mechanically continuous and electrically insulating matrix that embeds the contact-level topograp

hy generated in earlier MOL steps . This step exists at this position in the flow because the CESL nitride defines stress and etch-stop functionality, while the subsequent ILD0 DED etch requires a sacrificial dielectric volume that can be selectively patterned to define contact openings without exposing or damaging the underlying CESL and transistor structures . By depositing this initial dielectric before any contact patterning, the process establishes a controlled vertical separation between active devices and forthcoming metal contacts, which is essential for managing parasitic capacitance and preventing electrical shorts . This deposition also prepares the surface for the following ILD0 DED Etch by smoothing high-frequency topography left from gate, spacer, and CESL steps, thereby enabling more uniform etch front propagation and reducing local electric-field enhancement at contact edges . In contrast to the later ILD0 HARP deposition, which primarily serves gap-fill and global planarization purposes, the DED First Deposition is integration-driven and sacrificial in nature, designed to be partially removed and re-shaped during contact definition .

Physical and Chemical Mechanisms

Physically, the ILD0 DED First Deposition operates by forming a conformal dielectric network that nucleates on nitride and silicon-based surfaces, followed by volumetric growth that fills surface recesses and partially levels topography . The deposition chemistry promotes the formation of a silicon–oxygen backbone through gas-phase precursor dissociation and surface reactions, producing an amorphous dielectric whose insulating behavior arises from its wide bandgap and low free-carrier density . As the film grows, surface diffusion and re-emission processes redistribute arriving species, which determines sidewall coverage and local density variations, directly influencing how the film will later respond to anisotropic etching . From a device-physics perspective, the dielectric electrically decouples the transistor terminals from future metal contacts, reducing capacitive coupling and leakage paths in accordance with MOS electrostatic principles . The quality of this dielectric, particularly its defect density and bonding structure, influences local electric-field distribution around contact vias, which in turn affects breakdown reliability and time-dependent dielectric degradation in later operation .

Material and Method Selection with Parameter Interactions

The dielectric material used in ILD0 DED First Deposition is selected for its moderate density, etch tunability, and compatibility with both nitride etch stops and subsequent high-density gap-fill oxides, following integration concepts demonstrated in multilayer dielectric stacks . A deposition method favoring directional control and film uniformity is chosen so that increasing deposition energy or plasma activation generally enhances film density while simultaneously reducing etch rate in later patterning steps, illustrating a key trade-off managed during integration . Conversely, higher precursor reactivity improves step coverage but can increase hydrogen incorporation, which raises the risk of moisture uptake and dielectric instability during downstream thermal exposure . The interaction between deposition conformality and CESL topography is particularly critical, as excessive overhang formation at spacer corners can lead to contact etch pinch-off, while insufficient coverage can expose nitride edges and create localized field crowding after metallization . Therefore, this step is tuned not in isolation but in anticipation of the subsequent ILD0 DED Etch and the final ILD0 HARP deposition, which together complete the contact dielectric stack .

Node-Specific Considerations for 28nm Planar Technology

At the 28nm planar node, contact pitch scaling intensifies sensitivity to dielectric thickness uniformity and sidewall integrity, making the initial ILD0 DED First Deposition more critical than in older nodes with larger geometries . Shorter gate lengths and higher device densities increase the impact of parasitic capacitance and leakage, so the dielectric’s microstructure must support aggressive contact etching without compromising electrical isolation . Additionally, mechanical stress transmitted through the CESL into the channel can be partially modulated by the overlying ILD0 dielectric, linking this deposition step indirectly to strain engineering effects that influence carrier mobility at advanced planar nodes .

Risks & Challenges

  • [High] Contact Etch Pinch-Off: Non-uniform deposition or excessive overhang at spacer and CESL corners can cause local narrowing during the subsequent ILD0 DED Etch, leading to incomplete via opening and high contact resistance, driven by geometric shadowing and differential etch rates .
  • [Medium] Dielectric Defect-Induced Leakage: Hydrogen-related defects or weakly bonded regions in the deposited dielectric can form trap-assisted conduction paths under high electric field, increasing leakage and degrading breakdown reliability in contact regions .
  • [Medium] Etch Selectivity Loss to CESL: If the deposited dielectric has density or composition too similar to the underlying nitride, the chemical contrast during etching is reduced, increasing the risk of CESL erosion and unintended exposure of device features .
  • [Low] Stress-Induced Cracking or Delamination: Mismatch in intrinsic film stress between the ILD0 DED dielectric and CESL nitride can concentrate mechanical stress at interfaces, potentially causing micro-cracks that later propagate during thermal cycling (Engineering Practice).

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