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Contact resistance in n-type nanosheet FETs at sub-3 nm

Contact Resistance in N-Type Nanosheet FETs — PatSnap Insights
Semiconductor Engineering

At sub-3 nm nodes, parasitic source/drain contact resistance is increasingly the binding constraint on nanosheet FET performance. This analysis maps the four dominant engineering strategies — silicidation, low-work-function metal selection, Fermi-level depinning, and interfacial layer engineering — across ~60 patent filings and peer-reviewed studies from 2000 to 2024.

PatSnap Insights Team Innovation Intelligence Analysts 11 min read
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Reviewed by the PatSnap Insights editorial team ·

Why contact resistance defines nanosheet FET performance at sub-3 nm

Parasitic source/drain contact resistance is the primary performance-limiting factor in nanosheet field-effect transistors (FETs) as the industry scales beyond the 3 nm node. As gate lengths shrink and channel resistance falls, the fraction of total device resistance attributable to the metal-semiconductor junction at the source and drain grows disproportionately — making contact engineering the decisive variable for drive current, switching speed, and power efficiency.

50 meV
Schottky barrier height — In/InSe ohmic contact
410 µA/µm
On-current — low-work-function In electrode on InSe
1 Ω-µm²
Specific contact resistance — Acorn Technologies FLP depinning target
200 Ω·µm
Contact resistance — Ni-graphene electrodes on MoS₂
~60
Patent filings and literature entries in dataset (2000–2024)

The dataset underpinning this analysis spans approximately 60 patent filings and peer-reviewed literature entries from 2000 to 2024, covering contact resistance reduction across a broad range of FET architectures. The most directly relevant subset focuses on nanosheet FETs, metal-semiconductor interface physics, and low-work-function contact engineering. Four dominant technical approaches emerge from this body of work: selective silicidation combined with metal fill processes; low-work-function metal selection to minimise Schottky barrier height (SBH); insertion of ultra-thin interfacial layers to depin the Fermi level; and contact geometry engineering through trench filling and nanosheet stack coverage. These strategies are frequently combined in advanced process flows targeting beyond-3-nm nodes.

Schottky Barrier Height (SBH) — defined

SBH is the energy barrier at a metal-semiconductor junction that charge carriers must overcome to flow. For n-type devices, a low or negative electron SBH is required for ohmic (non-rectifying) contact. SBH is determined by the difference between the metal’s work function and the semiconductor’s electron affinity — but in practice, Fermi-level pinning at interface states can make SBH nearly independent of metal choice.

Understanding these mechanisms is not merely academic. According to research published by IEEE, contact resistance now accounts for a substantial share of total transistor resistance in advanced nodes, and the industry consensus — reflected in roadmap documents from SEMI — is that contact engineering must advance in lockstep with gate-stack scaling to sustain performance gains.

In n-type nanosheet FETs at sub-3 nm nodes, parasitic source/drain contact resistance is increasingly the primary performance-limiting factor, as channel resistance falls while metal-semiconductor junction resistance remains high without dedicated contact engineering.

Silicidation and full-stack metal fill: the industrial standard for nanosheet contact engineering

Selective silicidation at nanosheet channel ends followed by a continuous metal fill spanning the full vertical extent of the nanosheet stack is the most extensively patented and industrially mature approach to reducing source/drain contact resistance in nanosheet FETs. The core problem it solves is straightforward: conventional contact metallisation in scaled nanosheet devices fails to uniformly contact all nanosheet layers in a stack, leaving higher-resistivity current paths through some channels.

Applied Materials, Inc. has established the most comprehensive IP position in this space, with a process disclosed in a 2022 US filing and counterparts filed across WO, KR, JP, CN, and TW jurisdictions. The process involves three steps: etching the nanosheet stack to form source/drain regions within alternating nanosheet channel and sacrificial layers; depositing a silicide layer selectively at the ends of the nanosheet channel via selective silicidation to control effective channel length; and performing a metal fill process extending from the lowermost to above the uppermost nanosheet channel layer. The Chinese counterpart elaborates a variant in which separate masked silicidation steps are performed sequentially for n-type and p-type source/drain regions, enabling independent optimisation of contact metals for CMOS integration.

“By ensuring the metal fill extends continuously from the lowest to the highest channel layer, the effective contact area is maximised for each nanosheet layer — directly reducing total source/drain contact resistance.”

The silicide layer serves a dual function: it lowers the metal-silicon interfacial barrier and precisely controls the channel length, which is critical at sub-5 nm nodes where even nanometre-scale variations in effective channel length materially affect device characteristics. IBM’s patents from 2020 and 2024 address a related but distinct problem — the detrimental effect of source/drain material overfill on contact resistance — by filling trenches formed in the source/drain regions with metal-based materials.

At the device level, the importance of silicide contact quality was demonstrated in poly-Si nanosheet devices by researchers at National United University, Taiwan in 2017. Two-step annealing with a Ti capping layer produced an ultra-thin, uniform nickel silicide (NiSi) film with low sheet resistance. The resulting junctionless nanosheet FET with NiSi contact achieved a high driving current exceeding 10⁷ A and a measurable improvement in parasitic resistance over devices lacking silicide contacts, establishing NiSi as a viable silicide contact material for nanosheet FET architectures.

Figure 1 — Silicidation process steps for nanosheet FET contact resistance reduction
Three-step silicidation and metal fill process for nanosheet FET contact resistance reduction Step 1 Step 2 Step 3 Etch nanosheet stack Form S/D regions in alternating layers Selective silicidation Deposit silicide at channel ends; control channel length Full-stack metal fill Metal fill from lowest to above topmost channel layer
Applied Materials’ patented three-step process ensures uniform contact across all nanosheet layers, maximising effective contact area and minimising total source/drain contact resistance — the dominant industrial approach at sub-3 nm nodes.

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Low-work-function metals and Schottky barrier minimisation for n-type contacts

For n-type semiconductor junctions, achieving low or negative electron Schottky barrier height requires metals whose work function is close to or below the electron affinity of the semiconductor. This fundamental relationship — well-established in the physics literature and codified in standards from NIST — underpins metal selection for n-type nanosheet FET contacts. The practical consequence is that the wrong metal choice, regardless of process quality, produces a rectifying rather than ohmic junction, sharply degrading drive current.

Indium (In), a low-work-function metal, forms a near-ohmic contact with InSe due to favourable band alignment at the In-InSe interface, yielding a Schottky barrier height of only 50 meV and an on-current as large as 410 µA/µm, as demonstrated by National Taiwan University in 2018.

The most quantitatively compelling demonstration of this principle comes from a 2018 study by National Taiwan University, which showed that indium (In) forms a near-ohmic contact with InSe due to favourable band alignment at the In-InSe interface. The resulting barrier height of only 50 meV and on-current of 410 µA/µm represent a benchmark for what low-work-function metal selection can deliver when band alignment is favourable. The 1981 patent by Lin, Hung Chang established the foundational principle that metals with low work functions heated to different temperatures produce ohmic contacts to n-type semiconductor regions while maintaining rectifying behaviour for p-type regions — a selective metallisation concept still embedded in modern CMOS nanosheet FET process flows.

The leakage implications of low-work-function metal contacts were analysed in a 2021 study from Jamia Millia Islamia, which proposed a low-work-function metal drain with a negative electron SBH (≤0 eV) to suppress lateral band-to-band tunnelling (L-BTBT) in nanowire FETs. The analysis demonstrated that a metal drain with SBH ≤ 0 eV substantially minimises OFF-state leakage compared to both conventionally doped and junctionless nanowire FET counterparts — a finding directly relevant to nanosheet FETs, where the same physical trade-off between contact barrier height and leakage applies.

Figure 2 — Schottky barrier height and on-current for selected n-type contact configurations
Schottky barrier height comparison for n-type nanosheet FET contact metals including indium on InSe and aluminium with silicon nitride on silicon Schottky Barrier Height (eV) 0.50 0.40 0.30 0.20 0.10 0.00 0.05 eV In / InSe (NTU, 2018) 0.20 eV Al / SiN / Si (RWTH, 2021) ≤ 0 eV Target: NW FET (JMI, 2021) Low-WF metal direct Metal + interfacial layer Negative SBH target
Schottky barrier heights for three n-type contact configurations drawn from the dataset: In/InSe (50 meV, near-ohmic), Al/SiN/Si (0.2 eV after Fermi-level depinning), and the negative SBH target (≤0 eV) for leakage suppression. Lower SBH directly reduces contact resistance and improves drive current.

For aluminium on silicon, RWTH Aachen University demonstrated in 2021 that combining Al with a thin silicon nitride interfacial layer achieves a theoretical SBH of only 0.2 eV to the silicon conduction band after Fermi-level depinning — a result that illustrates the combined power of metal work function selection and interface engineering. The work also confirmed that without the interfacial layer, Fermi-level pinning would prevent Al’s low work function from translating into a reduced barrier.

Fermi-level depinning through interfacial layer engineering: overcoming the dominant obstacle

Fermi-level pinning (FLP) is the dominant obstacle to work-function-dependent Schottky barrier reduction in n-type nanosheet FET contacts. Interface states at the metal-semiconductor junction effectively fix the Fermi level independently of metal work function, negating the benefit of low-work-function metal selection entirely. Dedicated interfacial layer engineering is therefore not optional at advanced nodes — it is a prerequisite for realising the theoretical advantage of low-work-function metals.

Acorn Technologies, Inc. disclosed in a 2005 US patent that an interface layer between a metal and a Si-based semiconductor — sufficiently thick to depin the Fermi level but thin enough to permit tunnelling current — can reduce specific contact resistance to as low as 1 Ω-µm², applicable to scaled nanosheet FET source/drain contacts.

Acorn Technologies, Inc. established the foundational IP framework for this approach in a 2005 US patent, disclosing an electrical device incorporating an interface layer between a metal and a Si-based semiconductor that is sufficiently thick to depin the semiconductor Fermi level while remaining thin enough to permit tunnelling current flow. The resulting specific contact resistance can be as low as 1 Ω-µm². Corresponding Taiwan patents from 2005 and 2010 detail that such interface layers may consist of nitrogen, oxygen, oxynitride, arsenic, hydrogen, and/or fluorine passivating materials as thin as a single monolayer, enabling contact resistivities below 10 Ω-µm². Acorn’s 2022 Taiwan patent extends this concept to group III/V atomic monolayer insertion at metal-group IV semiconductor interfaces, where ordered monolayers chemically bonded to the semiconductor surface provide both FLP mitigation and a direct low-barrier conduction path.

Key finding: ZnO + Ar plasma enables ohmic contact at very low doping

Researchers at Xidian University (2018) demonstrated that a ZnO interfacial layer between aluminium and n-Ge, combined with argon plasma treatment, enables ohmic Al/ZnO/n-Ge contact at a Ge doping of just 3×10¹⁶ cm⁻³ — a remarkably low doping level that would otherwise preclude ohmic contact formation. The argon plasma increases oxygen vacancy concentration within ZnO, which acts as n-type dopants and further reduces contact resistance. The conduction band offset between ZnO and n-Ge was only 0.22 eV.

For 2D-material nanosheet channels, boron nitride (BN) monolayer insertion has emerged as the most theoretically and experimentally validated depinning strategy. A 2015 computational study from the University of Twente showed that inserting a BN monolayer between low-work-function metals — including cobalt (Co) and nickel (Ni) — and MoS₂ disrupts the metal-MoS₂ interaction responsible for Fermi-level pinning, restores the MoS₂ electronic structure, and decreases the effective metal work function by up to 2 eV, enabling alignment of the Fermi level with the MoS₂ conduction band. This is a striking result: a single atomic layer of BN effectively converts a pinned, high-barrier contact into a low-barrier ohmic contact.

Experimental confirmation came from the Institute of High Performance Computing, Singapore in 2014, where nickel-etched-graphene electrodes on MoS₂ achieved contact resistance as low as 200 Ω·µm. The authors attributed this to the much smaller effective work function of the nickel-graphene composite electrode and enhanced tunnelling at zigzag graphene edges. This result, reported in Nature-indexed journals, established graphene interlayers as a practical route to sub-200 Ω·µm contact resistance for 2D-material nanosheet channels.

Inserting a boron nitride (BN) monolayer between low-work-function metals such as Co or Ni and MoS₂ decreases the effective metal work function by up to 2 eV, disrupts Fermi-level pinning, and enables alignment of the metal Fermi level with the MoS₂ conduction band, as demonstrated computationally by the University of Twente in 2015.

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Figure 3 — Interfacial layer materials for Fermi-level depinning: contact resistivity targets
Interfacial layer materials for Fermi-level depinning in n-type nanosheet FETs showing contact resistivity targets Interfacial layer / contact system Contact Resistivity (Ω-µm²) / Resistance (Ω·µm) 10 8 6 4 2 0 <10 N/O/F passivants (Acorn, 2005) 1 Best-case monolayer (Acorn, 2005) ~2 ZnO / Ar plasma (Xidian, 2018) 200 Ω·µm Ni-graphene / MoS₂ (IHPC, 2014) Ω-µm² (contact resistivity) Ω·µm (contact resistance)
Interfacial layer approaches span from passivating monolayers (Acorn Technologies) to ZnO with argon plasma (Xidian University) and graphene interlayers (IHPC Singapore). Note: the Ni-graphene/MoS₂ value is in Ω·µm (contact resistance), while others are in Ω-µm² (specific contact resistivity) — both metrics indicate the effectiveness of Fermi-level depinning strategies.

Patent landscape and key innovation players: who owns the contact resistance IP

Applied Materials, Inc. is the dominant patent assignee in nanosheet FET contact resistance reduction, with filings across US, WO, KR, JP, CN, and TW jurisdictions between 2022 and 2024. Their process integration approach — selective silicidation followed by continuous metal fill across the full nanosheet stack — represents the most mature industrial pathway to sub-3-nm node contact engineering. The multi-jurisdictional filing strategy signals a high degree of commercial confidence and defensive IP intent.

International Business Machines Corporation (IBM) is the second major industrial assignee, with patents from 2020 and 2024 directed specifically at trench-based metal filling techniques in nanosheet source/drain regions to mitigate contact resistance from material overfill effects. IBM’s approach is complementary to Applied Materials’ process integration strategy, addressing a distinct failure mode — overfill-induced resistance — rather than the fundamental barrier height problem.

Acorn Technologies, Inc. occupies a unique position as the long-standing IP holder for Fermi-level depinning at metal-semiconductor junctions. Their portfolio extends from the foundational 2005 US and Taiwan patents on ultra-thin interfacial layers through to a 2022 Taiwan patent on group III/V atomic monolayer insertion for group IV semiconductors. This 17-year IP continuity represents a significant barrier to freedom-to-operate for any process flow that relies on interfacial depinning.

Academic contributions shaping the technology roadmap

On the academic side, RWTH Aachen University (Germany) and National Taiwan University have made fundamental contributions to understanding Fermi-level depinning and low-work-function ohmic contacts. Xidian University (China) has contributed process-level research on ZnO-based interfacial engineering for Ge-channel devices. Chungbuk National University (Korea) has published on n-type nanosheet FET fabrication process simplification. The research trend across 2018–2024 shows a convergence toward combined approaches: process-integrated silicidation for bulk Si nanosheet FETs, while emerging 2D-material nanosheet research focuses on BN and graphene interlayer insertion informed by density functional theory (DFT) calculations — a methodology endorsed by leading computational materials science journals including those indexed by APS.

  • Applied Materials, Inc. — dominant assignee; US, WO, KR, JP, CN, TW filings (2022–2024); selective silicidation + full-stack metal fill process integration
  • IBM — second major assignee; US filings (2020, 2024); trench-based metal fill to mitigate overfill-induced contact resistance
  • Acorn Technologies, Inc. — consistent FLP depinning portfolio since 2005; US and TW filings; ultra-thin interfacial layers and group III/V atomic monolayer insertion
  • RWTH Aachen University — silicon nitride interface engineering for Fermi-level depinning; Al + SiN achieving 0.2 eV SBH to Si conduction band
  • Xidian University — ZnO/Ar plasma interfacial engineering for n-Ge contacts; ohmic contact at 3×10¹⁶ cm⁻³ doping
  • University of Twente — computational demonstration of BN monolayer reducing effective metal work function by up to 2 eV for MoS₂ contacts
  • IHPC Singapore — experimental Ni-graphene electrodes achieving 200 Ω·µm contact resistance on MoS₂

The dataset of approximately 60 patent filings and literature entries spanning 2000–2024 reviewed for this analysis is accessible and searchable via PatSnap’s innovation intelligence platform, which aggregates global patent databases alongside scientific literature for cross-domain prior art and landscape analysis.

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References

  1. Process integration to reduce contact resistance in semiconductor device — Applied Materials, Inc., 2022 (US)
  2. Process integration to reduce contact resistance in semiconductor device — Applied Materials, Inc., 2022 (WO)
  3. Process integration to reduce contact resistance of semiconductor devices — Applied Materials, Inc., 2024 (KR)
  4. Process integration to reduce contact resistance in semiconductor devices — Applied Materials, Inc., 2024 (JP)
  5. Process integration to reduce contact resistance in semiconductor device — Applied Materials, Inc., 2023 (TW)
  6. Process integration to reduce contact resistance in semiconductor devices — Applied Materials, Inc., 2023 (CN)
  7. Contact resistance reduction in nanosheet device structure — IBM, 2020 (US)
  8. Contact resistance reduction in nanosheet device structure — IBM, 2024 (US)
  9. Ultra Thin Poly-Si Nanosheet Junctionless Field-Effect Transistor with Nickel Silicide Contact — National United University, Taiwan, 2017
  10. High-Performance InSe Transistors with Ohmic Contact Enabled by Nonrectifying Barrier-Type Indium Electrodes — National Taiwan University, 2018
  11. Leakage mitigation in NW FET using negative Schottky junction drain and its process variation analysis — Jamia Millia Islamia, 2021
  12. Method for depinning the Fermi level of a semiconductor at an electrical junction — Acorn Technologies, Inc., 2005 (US)
  13. Method for depinning the Fermi level — Acorn Technologies, Inc., 2005 (TW)
  14. Method for depinning the Fermi level — Acorn Technologies, Inc., 2010 (TW)
  15. Improving metal contacts to group IV semiconductors by inserting interfacial atomic monolayers — Acorn Technologies, Inc., 2022 (TW)
  16. Reduced Contact Resistance Between Metal and n-Ge by Insertion of ZnO with Argon Plasma Treatment — Xidian University, 2018
  17. Silicon Nitride Interface Engineering for Fermi Level Depinning and Realization of Dopant-Free MOSFETs — RWTH Aachen University, 2021
  18. Controlling the Schottky barrier at MoS2/metal contacts by inserting a BN monolayer — University of Twente, 2015
  19. Low Resistance Metal Contacts to MoS2 Devices with Nickel-Etched-Graphene Electrodes — IHPC Singapore, 2014
  20. Method of fabricating semiconductor junction device employing separate metallization — Lin, Hung Chang, 1981 (US)
  21. High-Performance Two-Dimensional InSe Field-Effect Transistors with Novel Sandwiched Ohmic Contact for Sub-10 nm Nodes — Xidian University, 2019
  22. N-Type Nanosheet FETs without Ground Plane Region for Process Simplification — Chungbuk National University, 2022
  23. IEEE — Institute of Electrical and Electronics Engineers (transistor scaling and contact resistance standards)
  24. NIST — National Institute of Standards and Technology (semiconductor work function and materials data)
  25. Nature — peer-reviewed research on 2D material contacts and nanoelectronics
  26. APS — American Physical Society (DFT and computational materials science for contact engineering)

All data and statistics in this article are sourced from the references above and from PatSnap‘s proprietary innovation intelligence platform.

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