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Method Article

An Integrated Multimethod Simulation Framework for Tin Debris Control in Extreme Ultraviolet Lithography

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DOI:

10.3791/69818

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March 27th, 2026

In This Article

Summary

This protocol aims to guide users through an integrated simulation framework to achieve tin debris control in extreme ultraviolet (EUV) and emerging Blue-X lithography, integrating kinetic modeling, the Boltzmann transport equation (BTE), and density functional theory (DFT)–based methods to evaluate ion interactions and hydrogen-assisted cleaning.

Abstract

This protocol is a conceptual, integrated modeling framework illustrated with representative results and instructs users on combining the Boltzmann transport equation (BTE), particle-in-cell (PIC), and kinetic simulations to investigate tin (Sn) debris mitigation in extreme ultraviolet (EUV) lithography. The protocol includes the reflectivity of Mo/Si multilayer mirrors (MLM), sputtering yield, implantation depth, kinetic modeling, and BTE computation. BTE and PIC simulations are used to resolve the electron energy distribution function (EEDF) of hydrogen plasmas and analyze the generation and acceleration of energetic Sn ions under different plasma conditions. The influence of hydrogen flow on ion slowing and radiation efficiency is also quantified. Based on the ionization cross sections and dissociation channels of SnxHy species, the interaction potentials for Sn-H collision are computed using the density functional theory (DFT) method, which are used to calculate the implantation depth. In addition, the MLM reflectivity and sputtering yield from the interaction between Sn debris and the Ru coating on the MLM are calculated using a semi-empirical formula. By following this protocol, users can obtain key physical parameters relevant to Sn debris control, including sputtering yields, implantation depths, MLM reflectivity, and SH4 formation under various hydrogen plasma EEDFs. These outputs enable systematic evaluation of contamination, cleaning, and detection processes in EUV lithography systems.

Introduction

Extreme-ultraviolet lithography (EUVL) is the state-of-the-art technology for advancing integrated circuit miniaturization, enabling patterning of features smaller than 2 nm. In a typical EUV source, a tin (Sn) microdroplet is first vaporized and ionized by a prepulse from a Nd:YAG laser, and the resulting plasma cloud is reheated by a CO2 laser operating at 10.6 µm, thereby generating EUV radiation, which is collected by Mo/Si multilayer mirrors (MLM)1,2. For commercial systems such as those developed by ASML, source power has reached levels sufficient for mass production. Nevertheless, ongoin....

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Protocol

NOTE: The overall workflow, including the integration of fluid, kinetic, and quantum-chemical approaches. The workflow is illustrated in Figure 1 (highlighted in the red box).

Magnetic hydrodynamic code diagram showing plasma parameters and kinetic code integration process.
Figure 1. Schematic of the integrated simulation framework for extreme ultraviolet lithography. Abbreviatio....

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Results

Sputtering yield calibration and validation
Calculate the sputtering yield of Ar atoms in Ru as a calibration step. These sputtering yields represent output from protocol step 2.1 (Yamamura model). The results are shown in Figure 5 (left). Experimental data reported by Wu et al.26 and Laegreid et al.27 are largely consistent. The theoretical results from the present model show good agreement with experimental measurements a.......

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Discussion

The integrated methodology that combines the Boltzmann transport equation (BTE), particle-in-cell (PIC), and kinetic simulations establishes a unified framework for investigating tin (Sn) debris mitigation in extreme ultraviolet (EUV) lithography. Specifically, the fluid simulation yields the plasma parameters—density and temperature, which can be integrated into a PIC program to obtain the spatiotemporal distribution of SnxHy molecules. By coupling these PIC results with reaction rates obtain.......

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Disclosures

The authors have no conflicts of interest to disclose.

Acknowledgements

We acknowledge support from the National Natural Science Foundation of China Grant No.12374231.

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Materials

List of materials used in this article
NameCompanyCatalog NumberComments
BOLSIG+Laboratory Plasma et Conversion d'Energie, University Paul SabatierThe version updated on April 24, 2025
GaussianGaussian Inc.Gaussian 16
RustBCADepartment of Nuclear, Plasma, and Radiological Engineering, University of Illinois at Urbana-Champaign1.2.0

References

  1. O’Sullivan, G., et al. Spectroscopy of highly charged ions and its relevance to EUV and soft X-ray source development. J Phys B At Mol Opt Phys. 48, 144025(2015).
  2. Versolato, O. O. Physics of laser-driven tin p....

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Tags

EUV LithographyBoltzmann Transport EquationParticle-In-Cell SimulationKinetic ModelingHydrogen PlasmaSputtering YieldImplantation DepthMLM ReflectivityDensity Functional Theory