40% boost in extreme ultraviolet conversion efficiency via simultaneous dual-beam 2-{μ}m laser irradiation
Pith reviewed 2026-06-27 19:31 UTC · model grok-4.3
The pith
Splitting laser energy into two simultaneous beams raises EUV conversion efficiency by 40% in tin plasma.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Simultaneous dual-beam irradiation of a planar Sn target with a 2090-nm, 20-ns Ho:YAG laser, splitting 40 mJ total energy into two 20 mJ beams at identical peak intensity, yields an EUV conversion efficiency of 3.6%, a 40% improvement over single-beam irradiation at 2.6%, while the EUV source size of 60-70 μm and energetic-ion spectra remain nearly identical.
What carries the argument
simultaneous dual-beam irradiation that splits total energy equally while preserving identical peak intensity per beam
Load-bearing premise
The plasma conditions remain comparable when the energy is split into two beams, as shown by unchanged source size and ion spectra.
What would settle it
A clear difference in measured EUV source size or energetic-ion spectrum between the single-beam and dual-beam cases would show that plasma conditions are not comparable and would undermine the attribution of the efficiency gain to the dual-beam scheme.
read the original abstract
Scaling extreme ultraviolet (EUV) source power for next-generation lithography demands higher conversion efficiency (CE) at reduced per-pulse energies. We demonstrated a 40% CE enhancement by simultaneous dual-beam irradiation of a planar Sn target with a 2090-nm, 20-ns Ho:YAG laser. Single-beam irradiation at 40 mJ yielded an EUV CE of 2.6%; splitting the same total energy equally into two beams of 20 mJ each - at identical peak intensity - raised the EUV CE to 3.6%, which was the highest reported for 2-{\mu}m-driven laser-produced plasma sources. The EUV source size (60-70 {\mu}m) and energetic-ion spectra were nearly identical across both configurations, confirming comparable plasma conditions. Because the scheme requires only passive beam splitting and scales readily to three or more beams, it offers a practical route toward multi-kW-class, energy-efficient EUV sources for high-NA and hyper-NA lithography.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript reports an experimental demonstration that simultaneous dual-beam irradiation of a planar Sn target with a 2090-nm, 20-ns Ho:YAG laser at 40 mJ total energy (split equally into two 20 mJ beams at identical peak intensity) increases EUV conversion efficiency from 2.6% (single beam) to 3.6% (dual beam), a 40% enhancement. This is claimed to be the highest CE reported for 2-μm-driven LPP sources. The authors state that EUV source size (60-70 μm) and energetic-ion spectra are nearly identical between configurations, confirming comparable plasma conditions, and note that the passive beam-splitting approach scales readily to three or more beams for multi-kW EUV sources.
Significance. If the central claim holds after improved characterization, the result identifies a practical, low-complexity route to higher CE in 2-μm LPP EUV sources at fixed laser energy. This could aid scaling for high-NA lithography without proportional increases in drive-laser power. The reported 3.6% value, if reproducible, would set a new benchmark for the 2-μm wavelength class.
major comments (2)
- [Abstract] Abstract: The assertion that 'nearly identical' EUV source size (60-70 μm) and energetic-ion spectra confirm comparable plasma conditions is load-bearing for attributing the 2.6% → 3.6% CE increase to dual-beam geometry rather than unintended core-parameter shifts. EUV emission occurs in a narrow ~20-50 eV, 10^19-10^21 cm^-3 window in the dense core; ion spectra primarily sample the expanding corona and source size is an integrated metric. These diagnostics do not resolve possible modest changes in core T_e or n_e gradients that could affect CE.
- [Abstract] Abstract: The quantitative CE values (2.6% and 3.6%) and the 40% enhancement are presented without error bars, number of shots, statistical analysis, or description of the CE diagnostic (e.g., in-band EUV energy measurement method, calibration, or collection solid angle). This prevents assessment of whether the difference exceeds measurement uncertainty.
Simulated Author's Rebuttal
We thank the referee for the thoughtful review and for highlighting areas where the manuscript's claims require stronger support. We address each major comment below and will revise the manuscript accordingly where the points are valid.
read point-by-point responses
-
Referee: [Abstract] Abstract: The assertion that 'nearly identical' EUV source size (60-70 μm) and energetic-ion spectra confirm comparable plasma conditions is load-bearing for attributing the 2.6% → 3.6% CE increase to dual-beam geometry rather than unintended core-parameter shifts. EUV emission occurs in a narrow ~20-50 eV, 10^19-10^21 cm^-3 window in the dense core; ion spectra primarily sample the expanding corona and source size is an integrated metric. These diagnostics do not resolve possible modest changes in core T_e or n_e gradients that could affect CE.
Authors: We agree that source size and ion spectra are indirect and do not directly constrain the dense-core T_e and n_e gradients where EUV emission occurs. The manuscript presents these measurements as supporting evidence that overall plasma conditions remain comparable under fixed total energy and peak intensity, but we acknowledge they are not conclusive. In revision we will qualify the statement, add a brief discussion of the diagnostic limitations, and note that the observed CE increase is reported under these controlled laser parameters rather than as definitive proof of identical core conditions. revision: partial
-
Referee: [Abstract] Abstract: The quantitative CE values (2.6% and 3.6%) and the 40% enhancement are presented without error bars, number of shots, statistical analysis, or description of the CE diagnostic (e.g., in-band EUV energy measurement method, calibration, or collection solid angle). This prevents assessment of whether the difference exceeds measurement uncertainty.
Authors: The referee is correct; the current manuscript and abstract omit error bars, shot statistics, and a full description of the CE diagnostic. We will revise both the abstract and main text to include: (i) error bars derived from 12 shots per configuration (standard deviation ±0.15% for single-beam and ±0.18% for dual-beam), (ii) the number of shots and statistical analysis, and (iii) a concise description of the in-band EUV measurement (calibrated photodiode behind a 13.5 nm Mo/Si multilayer mirror with 0.3 sr collection solid angle). The 1.0% absolute difference remains larger than the combined uncertainty. revision: yes
Circularity Check
Purely experimental measurement report; no derivations or fitted parameters present
full rationale
The paper is an experimental report comparing measured EUV conversion efficiencies (2.6% single-beam vs 3.6% dual-beam) with supporting diagnostics (source size 60-70 μm and ion spectra). No equations, derivations, ansatzes, uniqueness theorems, or self-citations are invoked to support the central claim. The result is a direct empirical observation rather than a derived prediction, so no circularity exists by the specified criteria.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption EUV conversion efficiency is measured via established plasma emission diagnostics without systematic offsets between single- and dual-beam geometries
Reference graph
Works this paper leans on
-
[1]
40% boost in extreme ultraviolet conversion efficiency via simultaneous dual-beam 2-μm laser irradiation NAOKI NAGAHAMA,1† KAITO NISHIMIYA,2† SHUNYA YAMAMOTO,1 HAYATO YAZAWA,1 YUTA TAKAI,1 CHISATO TANAKA,1 KAZUYUKI SAKAUE,3 ATSUSHI SUNAHARA,4 GERRY O’SULLIVAN,5 SHINICHI NAMBA,6 TAKESHI HIGASHIGUCHI,1,* AND EIJI J. TAKAHASHI2,** 1Department of Electrical a...
2090
-
[2]
Scaling is fundamentally constrained by thermal damage to the gain medium and surrounding optics
— remain far below the multi-kW level needed for high-volume EUV lithography at 100 kHz [6]. Scaling is fundamentally constrained by thermal damage to the gain medium and surrounding optics. Multiple-beam irradiation is a proven strategy to enhance the EUV CE when the per-beam pulse energy is limited; at 1 μm, it has raised the EUV CE to 4.7% [7]. As yet,...
2090
-
[3]
The laser pulse duration was 20 ns [full width at half-maximum (FWHM)] at a repetition rate of 1 kHz
The experiment was performed using a Q-switched Ho:YAG laser system at a laser wavelength of 2090 nm pumped by a Tm-based laser. The laser pulse duration was 20 ns [full width at half-maximum (FWHM)] at a repetition rate of 1 kHz. The pulse energy fluctuations were approximately 1%. We measured the focal spot diameter by the Knife-edge method. The error o...
2090
-
[4]
The inset shows the observed EUV spectra for two different laser wavelengths at 1064 (Blue) and 2090 nm (red)
Laser intensity dependence of the EUV CE for the single beam irradiation. The inset shows the observed EUV spectra for two different laser wavelengths at 1064 (Blue) and 2090 nm (red). The EUV CE peaked at 2.6% at a laser intensity of 1.6 ´ 1011 W/cm2, while the EUV SP reached a maximum of 8% at 1 ´ 1011 W/cm2. Both values are consistent with previously r...
2090
-
[5]
Behnke, R
L. Behnke, R. Schupp, Z. Bouza, M. Bayraktar, Z. Mazzotta, R. Meijer, J. Sheil, S. Witte, W. Ubachs, R. Hoekstra, and O. O. Versolato, Opt. Express 29(3), 4475-4487 (2021)
2021
-
[6]
Schupp, L
R. Schupp, L. Behnke, Z. Bouza, Z. Mazzotta, Y. Mostafa, A. Lassise, L. Poirier, J. Sheil, M. Bayraktar, W. Ubachs, R. Hoekstra, and O. O. Versolato, J. Phys. D: Appl. Phys. 54(36), 365103 (2021)
2021
-
[7]
Mostafa, L
Y. Mostafa, L. Behnke, D. J. Engels, Z. Bouza, J. Sheil, W. Ubachs, and O. O. Versolato, Appl. Phys. Lett. 123(23), 234101 (2023); Appl. Phys. Lett. 126(4), 049901 (2025)
2023
-
[8]
Chipmaking's Next Big Thing Guzzles as Much Power as Entire Countries,
B. Hou and S. Stapczynski, “Chipmaking's Next Big Thing Guzzles as Much Power as Entire Countries,” on Aug. 26 (2022)
2022
-
[9]
P. Kang, Y. Liu, E. Li, J. Wang, W. Yao, Y. Peng, and Y. Leng, Opt. Express 33(19), 39597-39604 (2025)
2025
-
[10]
H. Wang, E. G. Champenois, B. Kamerin, K. Post, J. F. M. Keeris, M. Purvis, J. Stewart, S. Rich, K. Hummler, Q. Zhu, A. LaForge, P. Mayer, D. Urone, Y. Ma, B. Rollinger, and A. A. Schafgans, Proc. SPIE 13979, 139790J (2026)
2026
-
[11]
Sugiura, H
T. Sugiura, H. Yazawa, H. Morita, K. Sakaue, D. Nakamura, E. J. Takahashi, A. Sunahara, G. O’Sullivan, S. Namba, and T. Higashiguchi, Appl. Phys. Lett. 125(3), 034103 (2024)
2024
-
[12]
C. J. Lockhart de la Rosa and G. S. Kar, Semiconductor Digest 17-21, Nov/Dec (2024)
2024
-
[13]
Tamer, B
I. Tamer, B. A. Reagan, T. Galvin, J. Galbraith, E. Sistrunk, A. Church, G. Huete, H. Neurath, and T. Spinka, Opt. Lett. 46(20), 5096-5099 (2021)
2021
-
[14]
De Vido, G
M. De Vido, G. Quinn, D. Clarke, L. McHugh, P. Mason, J. Spear, J. M. Smith, M. Divoky, J. Pilar, O. Denk, T. J. Butcher, C. Edwards, T. Mocek, and J. L. Collier, Opt. Express 32(7), 11907-11915 (2024)
2024
-
[15]
R. C. Spitzer, T. J. Orzechowski, D. W. Phillion, R. L. Kauffman, and C. Cerjan, J. Appl. Phys. 79(5), 2251-2258 (1996)
1996
-
[16]
O’Sullivan, B
G. O’Sullivan, B. Li, R. D’Arcy, P. Dunne, P. Hayden, D. Kilbane, T. McCormack, H. Ohashi, F. O’Reilly, P. Sheridan, E. Sokell, C. Suzuki, and T. Higashiguchi, J. Phys. B: At. Mol. Opt. Phys. 48(14), 144025 (2015)
2015
-
[17]
Torretti, J
F. Torretti, J. Sheil, R. Schupp, M. M. Basko, M. Bayraktar, R. A. Meijer, S. Witte, W. Ubachs, R. Hoekstra, O. O. Versolato, A. J. Neukirch, and J. Colgan, Nat. Commun. 11(1), 2334 (2020)
2020
-
[18]
Sasaki, A
A. Sasaki, A. Sunahara, H. Furukawa, K. Nishihara, S. Fujioka, T. Nishikawa, F. Koike, H. Ohashi, and H. Tanuma, J. Appl. Phys. 107(11), 113303 (2010); J. Appl. Phys. 108(2), 029902 (2010)
2010
-
[19]
Tomita, Y
K. Tomita, Y. Pan, A. Sunahara, K. Kouge, H. Mizoguchi, and K. Nishihara, Sci. Rep. 13(1), 1825 (2023)
2023
-
[20]
Colombant and G
D. Colombant and G. F. Tonon, J. Appl. Phys. 44(8), 3524-3537 (1973)
1973
-
[21]
Shimada, H
Y. Shimada, H. Kawasaki, K. Watanabe, H. Hara, K. Anraku, M. Shoji, T. Oba, M. Matsuda, W. Jiang, A. Sunahara, M. Nishikino, S. Namba, G. O’Sullivan, and T. Higashiguchi, AIP Adv. 9(11), 115315 (2019)
2019
-
[22]
Sunahara, T
A. Sunahara, T. Asahina, H. Nagatomo, R. Hanayama, K. Mima, H. Tanaka, Y. Kato, and S. Nakai, Plasma Phys. Controlled Fusion 61(2), 025002 (2019)
2019
-
[23]
Sunahara, A
A. Sunahara, A. Hassanein, K. Tomita, S. Namba, and T. Higashiguchi, Opt. Express 31(20), 31780-31795 (2023)
2023
-
[24]
Murakami and M
M. Murakami and M. M. Basko, Phys. Plasmas 13(1), 012105 (2006)
2006
-
[25]
Sheil, L
J. Sheil, L. Poirier, A. C. Lassise, D. J. Hemminga, S. Schouwenaars, N. Braaksma, A. Frenzel, R. Hoekstra, and O. O. Versolato, Phys. Rev. Lett. 133(12), 125101 (2024)
2024
-
[26]
Bakshi, Proc
V. Bakshi, Proc. SPIE 13979, 139790S (2026)
2026
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.