Target Material Technology: A Comprehensive Analysis from Fundamental Principles to Cutting-Edge Applications


Release time:

2025-06-11

As the core material in Physical Vapor Deposition (PVD) technology, the target material essentially serves as a "material source" where atomic-level material transfer is achieved through high-energy particle bombardment. In the sputtering process, the target material acts as the target for high-energy ions (such as argon ions). When ions bombard the target surface with energy of 3-5 keV, the target atoms gain sufficient kinetic energy to escape the lattice, migrating to the substrate in the gas phase and depositing as a film.

I. Core Concepts and Mechanisms of Target Materials

1. Essential Definition and Functional Positioning of Target Materials

As the core material in Physical Vapor Deposition (PVD) technology, target materials are essentially a "material source" that achieves atomic-level material transfer through high-energy particle bombardment. In the sputtering process, the target material acts as the target for high-energy ions (such as argon ions). When ions bombard the target material surface with energy of 3-5 keV, the target material atoms gain sufficient kinetic energy to leave the lattice and migrate to the substrate in the gas phase to deposit a film. This material transfer process is highly controllable, and the composition, structure, and purity of the target material directly determine the electrical, optical, and mechanical properties of the film. For example, in semiconductor chip manufacturing, the resistivity of the interconnect layer formed by magnetron sputtering of copper target material needs to be controlled below 1.8μΩ·cm, which requires the target material purity to be above 99.999% (5N), and the content of impurity atoms (such as iron and zinc) needs to be below 10ppm; otherwise, it will lead to increased electron scattering and an increase in chip signal transmission delay of more than 15%.

2. Physical Basis of Sputtering Process

(1) Four-Stage Model of the Sputtering Process

  • Gas Ionization Argon gas is introduced into the vacuum chamber and a high-frequency electric field (13.56MHz) is applied. Argon atoms are ionized into Ar⁺ ions and free electrons, forming plasma;
  • Ion Acceleration Under the action of the electric field, Ar⁺ gains kinetic energy and bombards the target material surface with energy of 200-1000eV;
  • Atom Ejection Target material atoms obtain sufficient energy through "cascade collisions" to overcome lattice constraints and form sputtered particles (90% neutral atoms, 10% ions);
  • Film Deposition Sputtered particles migrate to the substrate at a speed of 300-1000m/s, forming a dense film through surface diffusion and atomic rearrangement.

(2) Mechanism of Target Material's Influence on Film Properties

  • Chemical Matching The ratio of indium to tin atoms in ITO (Indium Tin Oxide) target material must be strictly controlled at 9:1. A deviation exceeding ±0.5% will cause the sheet resistance of the film to increase by 20%, affecting the touch sensitivity of the touch screen;
  • Microstructure Consistency The grain size of the target material needs to be controlled at 5-10μm and the orientation needs to be uniform; otherwise, anisotropy during sputtering will cause the film thickness deviation to exceed ±3%;
  • Thermal Stability The temperature of tantalum targets used in semiconductors can reach 300℃ during sputtering. Hot isostatic pressing (HIP) treatment is required to eliminate internal stress and avoid cracking of the target material due to inconsistent thermal expansion coefficients.

3. Performance Evaluation System of Target Materials

Index Category Semiconductor Grade Requirements Display Panel Grade Requirements Photovoltaic Grade Requirements
Purity ≥5N (metal impurities <1ppm) ≥4N (metal impurities <10ppm) ≥3N (metal impurities <50ppm)
Density ≥99.5% theoretical density ≥98% theoretical density ≥95% theoretical density
Impurity Distribution Uniformity <5ppm spatial fluctuation Uniformity <20ppm spatial fluctuation Uniformity <50ppm spatial fluctuation
Grain Size 5-15μm (single crystal target material <1μm) 10-30μm 20-50μm

II. Classification System and Characteristic Comparison of Target Materials

1. Fine Classification by Material Composition

(1) Metal Target Materials: The "Conductive Foundation" of the Electronics Industry

  • High-purity Aluminum Target (Purity ≥5N): Used for the first layer of metal wiring in semiconductor chips, requiring iron and silicon impurities <5ppm; otherwise, Al-Fe-Si precipitates will form, reducing the electromigration resistance of the wiring by 50%. In TSMC's 7nm process, high-purity aluminum targets with grain sizes <5μm are used to increase the electromigration lifetime of the copper interconnect layer to over 1000 hours.
  • Titanium Tungsten Alloy Target (Ti:W=7:3): As a barrier layer material, the oxygen content needs to be controlled <200ppm; otherwise, TiO₂ impurities will cause the barrier layer resistance to increase by 30%, affecting chip reliability.

(2) Ceramic Target Materials: "Functional Carriers" in the Optoelectronic Field

  • ITO Target Material (In₂O₃:SnO₂=9:1): Key indicators include:
    • Resistivity <1.5×10⁻⁴Ω·cm (ensuring touch screen response speed <5ms);
    • Visible light transmittance >85% (400-700nm band);
    • Particle size <0.5μm (avoiding film surface roughness >1nm).
      BOE's 10.5-generation line uses G8.5 size ITO targets, which require hot isostatic pressing (HIP) treatment to achieve a density of 99.8% to ensure that the resistance uniformity deviation of large-area display panels is <5%.

(3) Composite target materials: An "integrated solution" with multi-dimensional performance

  • CIGS (copper indium gallium selenide) target materials Through gradient composition design (Cu/(In+Ga)=0.85-0.95, Ga/(In+Ga)=0.2-0.3), the photoelectric conversion efficiency of thin-film solar cells exceeds 23%. Würth Solar in Germany uses a three-layer structure (Cu-In/Ga-Se) for its CIGS target materials, achieving atomic-level compositional uniformity control through simultaneous magnetron sputtering deposition.

2. In-depth analysis by application scenario

(1) Semiconductor manufacturing: "Material engraving" with nanometer-level precision

In 3D NAND flash memory manufacturing, tungsten target materials are used to deposit high aspect ratio (>30:1) via-fill layers. The target material requires an oxygen content of <100ppm; otherwise, WO₃ impurities will form at the bottom of the vias, increasing the contact resistance by 10 times. Samsung's 128-layer 3D NAND uses ultra-fine crystalline tungsten targets (grain size <2μm), increasing the via-fill yield from 85% to 98%.

(2) Display panels: The "ultimate challenge" of large-area uniformity

Micro-LED display silver target materials must meet:


 

  • Purity ≥5N (Ag≥99.999%);
  • Target size ≥1.5m×1.8m (matching G8.5 substrate);
  • Surface roughness Ra<0.2μm (to avoid poor thin film step coverage).
    The large-size silver target developed by Nippon Mining & Metals in Japan, through powder metallurgy + hot isostatic pressing process, achieved 99.9% density and ±2% compositional uniformity, enabling Micro-LED electrode linewidth control within 5μm.

(3) New energy field: The "balance of art" between efficiency and cost

Barium titanate target materials for perovskite solar cells require precise control of oxygen vacancy concentration (2-5%) during sputtering to optimize carrier transport performance. Research by ETH Zurich in Switzerland shows that barium titanate films with an oxygen vacancy concentration of 3.2% can increase the battery open-circuit voltage to 1.2V and achieve a fill factor of 78%.

III. Technical barriers and process innovations in target material preparation

1. Purification revolution of high-purity materials

(1) Metal target material purification technology

  • Zone melting method Through 10-20 zone melting operations, the purity of copper target materials can be increased from 99.99% to 99.9999% (6N), with iron and nickel impurity content <0.1ppm. Honeywell's 6N copper target uses this technology for copper interconnect layers in processes below 14nm, increasing the current density of the chip to 1×10⁶A/cm².
  • Electrorefining method When used for aluminum target purification, high-purity graphite anodes and titanium cathodes are used for electrolysis in an organic electrolyte, reducing sodium and magnesium impurities in aluminum to <1ppm. JX Nippon Mining & Metals' 5N aluminum target uses this process to meet the wiring needs of advanced logic chips.

(2) Ceramic target material synthesis technology

  • Sol-gel method When preparing ITO target materials, hydrolysis-polycondensation reaction of indium tin alkoxides can obtain precursor powder with a particle size of <10nm. After sintering at 1400℃, the density reaches 99.5%, which is 3% higher than that of target materials prepared by the traditional solid-state method, and the sputtering rate is increased by 15%.

2. Precision breakthrough in forming process

(1) Powder metallurgy process

  • Cold isostatic pressing (CIP) + vacuum sintering When preparing aluminum nitride target materials, molding is performed under a pressure of 200MPa, and then vacuum sintering at 1800℃ can obtain target materials with thermal conductivity >280W/(m・K), meeting the heat dissipation requirements of high-power chips. CoorsTek's aluminum nitride target materials use this process, with thermal conductivity increased by 20% compared to traditional processes.

(2) Hot isostatic pressing (HIP) technology

  • Treating the target material at 150MPa argon pressure and 1200℃ can eliminate internal microcracks and pores, increasing the density of tantalum targets from 98% to 99.9%, and the target material utilization rate during sputtering from 30% to 50%. Jiangfeng Electronics' HIP-treated tantalum targets have passed SMIC certification and are used for the deposition of barrier layers in the 14nm process.

3. Microscopic control of surface treatment

The sputtering surface of the target material needs atomic-level polishing, with a roughness Ra<0.1μm; otherwise, the surface particle contamination (>0.5μm particles) of the thin film will increase by 10 times. For molybdenum ruthenium target materials used in EUV lithography, the surface needs to be polished by ion beam polishing (IBP) to achieve Ra<0.05μm to avoid scattering loss on the mirror surface and ensure that the reflectivity of EUV light is >70%.

IV. Frontier exploration and future trends of target material applications

1. Target material innovation in advanced processes

In the 3nm FinFET process, ruthenium target materials, as the work function adjustment layer of the gate-all-around structure, need to control the grain size <50nm and the orientation is consistent (<5° deviation) to achieve uniform threshold voltage control (deviation <5mV). TSMC has adopted the nanocrystalline ruthenium target from Tosoh Corporation in Japan, reducing the leakage current of 3nm chips by 30%.

2. Target Material Breakthroughs in Flexible Electronics

Silver nanowire targets for flexible OLED displays. A 20nm thick silver film is deposited on a PI substrate via magnetron sputtering. The following requirements must be met:
 
  • Sheet resistance < 10Ω/□ (traditional ITO film is 15Ω/□);
  • Resistance change rate < 5% when bending radius < 5mm;
  • Visible light transmittance > 88%.

3. Three Major Development Directions of Target Material Technology

  • Ultimate Purity Development of 7N (99.99999%) grade high-purity target materials for superconducting thin film deposition in quantum computing chips. Shin-Etsu Chemical in Japan has already achieved small-batch production of 7N aluminum targets;
  • Intelligent Design Optimizing target material composition through machine learning, such as using Gaussian process regression models to design the copper-indium-gallium ratio of CIGS target materials, resulting in a solar cell efficiency prediction error < 0.3%;
  • Green Manufacturing Promoting the hydrothermal synthesis method for preparing ceramic target materials, reducing energy consumption by 40% compared to traditional sintering processes and reducing nitrogen oxide emissions by 50%.

Strategic Value of Target Material Technology

From nanoscale chips to hundreds-of-meter-scale photovoltaic components, target materials serve as an "atomic-level bridge" for material transformation. Technological advancements directly drive the continuation of Moore's Law and breakthroughs in new energy efficiency. Driven by both the need for independent and controllable semiconductors and the dual-carbon goals, the target material industry is upgrading from material supply to collaborative innovation in "materials - processes - equipment". In the future, with the development of cutting-edge fields such as quantum computing and flexible electronics, target materials will become a key indicator of a nation's high-end manufacturing capabilities. Technological breakthroughs will not only affect industrial competitiveness but also the strategic foundation of scientific and technological self-reliance.

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