Medium Current Ion Implanter
Medium Current Ion Implanter
Operating
Model: MC3-II/GP
Function: Up to 8-inch, 3–960 keV; Implantation available for B, BF₂, P, As, Ar
Engineer: Li / +86-21- 34206126-6012 / litq@1
Location: East Area, Epitaxy/Ion Implantation Zone
Equipment ID: EEI0MCI01
  • Basic Equipment Information
  • Operating Principle
  • Typical Application Case
Main Applications

It is used for doping semiconductor materials to modify their electrical properties, such as adjusting the threshold voltage, forming shallow junctions/resistors, and fabricating CMOS wells.

 

Process / Testing Capabilities

Implantation available for B, BF₂, As, P, Ar; Dissociation Energy > 50; Energy Error < 1%; Dose Error < 1%; Angular Error < 0.2°; Repeatability & Uniformity < 0.5%

 

Technical Specifications

Dose Range: 1E12 ~ 1E16 atoms/cm²;Tilt Angle Range: 0–60°, Minimum Adjustment Precision: 0.1°;Twist Angle Range: 0–360°, Minimum Adjustment Precision: 0.1°;Beam Parallelism: ≤±0.5°;Wafer Alignment Precision: ≤±0.2°;Temperature: < 100°C;Particle Addition: < 30 ea (≥0.12 μm, 3 mm wafer edge exclusion)

Ion implanters are critical precision equipment in the semiconductor manufacturing process, primarily used to implant ions of specific elements into semiconductor wafers (e.g., silicon wafers), thereby modifying the electrical properties of local wafer regions (e.g., doping concentration, conductivity type, etc.). Their working principle can be summarized into five core steps: ion generation → ion extraction and acceleration → mass analysis and filtration → ion beam transmission and scanning → ion implantation into wafers.

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I. Ion Generation (Ion Source)

Principle: Convert the elements to be implanted (e.g., B, P, As, Ar, etc.) into an ionic state through an ionization process.

Methods: Thermal Ionization: Heat the solid material to cause its evaporation, followed by ionization via electron bombardment.

Gas Ionization: Perform electron bombardment on gaseous substances (e.g., BF₃, PH₃) to ionize gas molecules into corresponding ions (e.g., BF₂⁺, P⁺).

 

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II. Ion Extraction and Acceleration (Accelerating Electric Field)

Principle: The ions generated by the ion source are extracted and imparted with a specific kinetic energy by means of electric field acceleration.

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III. Mass Analysis and Filtration (Magnetic Analyzer)

Principle: The target ions are screened out by utilizing the principle of magnetic field deflection (e.g., to exclude impurity ions or different isotopes of the same element).

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IV. Ion Beam Transmission and Scanning (Beam Current Control)

Principle: The shape, direction and position of the ion beam are controlled by electromagnetic lenses and scanning systems to ensure its uniform coverage of the entire wafer surface.

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V. Ion Implantation into Wafers (Target Chamber and Wafer Stage)

Principle: The ion beam, after filtration and scanning, ultimately bombards the wafer surface, and the ions penetrate into the wafer interior through kinetic energy deposition to form a doped layer.

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Through the full-process control of ion generation → acceleration → mass filtration → scanning → implantation, the ion implanter achieves precise doping of semiconductor wafers, and it is an irreplaceable key equipment in integrated circuit manufacturing. Its technical challenges lie in high energy precision, high beam current purity, high-uniformity scanning, and the integration of complex vacuum and control systems.

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Boron (B) - Acceptor Impurity (P-type)
  1. Core Doping for PMOS Source/Drain (P⁺ Region) in CMOS Logic Chips: Low-energy ion implantation (e.g., 5~20 keV) forms shallow junctions (<10 nm), used in advanced processes below 7 nm to suppress the short-channel effect.
  2. P-well Formation: High-energy implantation (100~500 keV) creates deep P-wells (junction depth 1~3 μm) in silicon substrates to isolate NMOS devices, with a doping dose of approximately 1e13~1e14 ions/cm².
  3. Threshold Voltage Regulation for NAND Flash Floating Gate Cells in Memory Chips: Boron implantation is used to adjust the threshold voltage distribution of memory cells.
  4. DRAM Channel Doping: Light boron doping (dose ~1e12 ions/cm²) modulates the MOSFET threshold voltage and reduces standby leakage current.

Phosphorus (P) - Donor Impurity (N-type)

  1. NMOS Source/Drain (N⁺ Region): Medium-energy implantation (20~50 keV) forms conductive channels with a doping concentration up to 1e20 cm⁻³, which requires rapid thermal annealing for activation.
  2. Source of Power MOSFETs: High-energy implantation (>100 keV) forms low-resistance N⁺ sources in Si or SiC substrates to reduce on-resistance.
  3. Buried Word Line (WL) in DRAM: Phosphorus diffusion forms N-type buried layers to improve word line conductivity, suitable for high-capacity memory chips (e.g., 14 nm DDR5).
  4. Emitter of Bipolar Junction Transistors (BJTs): Phosphorus diffusion forms N⁺ emitters, which form PN junctions with the base region (boron-doped) and are used in radio frequency (RF) amplification or power switch devices.

Arsenic (As) - Donor Impurity (N-type)

  1. NMOS Source/Drain Extension (SDE) in Advanced Processes: Low-energy implantation (<10 keV) forms ultra-shallow junctions (junction depth <5 nm), used in FinFET/GAA devices below 3 nm to suppress source-drain punch-through.
  2. Buried Layer Doping for High-Speed Logic Chips: Arsenic implantation in silicon substrates forms deep N-type layers (e.g., beneath the buried oxide layer of SOI substrates), used for isolation or conductive layers in RF devices.
  3. Source/Drain of InGaAs Devices: Arsenic implantation in InGaAs substrates forms N⁺ contacts, which utilize its lattice matching with III-V materials to reduce contact resistance (e.g., 5G millimeter-wave chips).

Fluorine (F) - Interface Modulation

  1. FinFET/GAA Gate Engineering: Fluoride ion implantation (energy ~1 keV, dose ~1e14 ions/cm²) beneath metal gates neutralizes interface trap charges and optimizes threshold voltage uniformity (e.g., Intel's 10 nm process).
  2. In addition, BF₂ implantation can be used to achieve ultra-shallow junction implantation of B.
Samples containing metals, powders or liquefiable substances are prohibited. Both front and back sides of the sample must be kept clean. The size of wafer samples shall not exceed 8 inches; small-sized regular samples are processable. 
The list below shows FAQs (click a question to view the answer). If your question is not listed, you can leave a message using the link.
FAQs
  • 01
    能否进行超大剂量注入如1E16级别?

    平台使用机型为中电流机型,能量范围广,但电流中等,因此加工大剂量条件需要花费较长时间。平台最大支持1e16 级别剂量,且需要进行多次注入,具体细节请与工艺老师确认。

  • 02
    Tilt 角度和Twist 角度有什么区别,怎么应用?

    Tilt 指的是离子束与晶圆垂直角度的夹角,可理解为入射角度,垂直入射为0°,一般使用Tilt7°来避免沟道效应。Twist 指晶圆以圆心逆时针旋转的角度,同样是为了避免沟道效应,一般设置Twist22°。

  • 03
    已知掺杂浓度和深度,怎么确认离子注入条件?

    需要借助仿真软件进行模拟,平台暂时仅支持加工服务。

  • 04
    预约离子注入工艺,需要向工艺老师提供哪些需求?

    1.样品信息:样品是否符合加工规范,是否需要贴片。

    2.条件信息:包含注入元素,能量,剂量,角度等参数。

  • 05
    除B, BF2, P, As,Ar这些元素,是否支持其他元素注入?

    暂时仅支持以上元素注入,后续视需求逐步拓展Ge,Si,In,等元素注入.

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