Cited by 111Laser-Ablation Synthesis of NanoparticlesLaser-induced spectroscopy and plasmaLaser Material Processing Techniques

Liquid-phase laser ablation

Open access
Sasaki, Koichi, Takada, Noriharu·2010·Pure and Applied Chemistry

Abstract

The irradiation of an intense laser pulse onto a solid target immersed in liquid produces dense plasma. The plasma produced by liquid-phase laser ablation has unique features at high pressure and temperature, which are never realized by liquid-phase discharges. Another unique characteristic of liquid-phase laser ablation is the formation of a cavitation bubble. This article reports the fundamental aspects of liquid-phase laser-ablation plasmas, cavitation bubbles, and the formation processes of nanoparticles, together with some applications of liquid-phase laser ablation.

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Crossref · 10.1351/pac-con-09-10-23

Cites

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  • When laser-induced photonic energy strikes metal surface, inverse bremsstrahlung occurs, where radiation absorption results in vibration of electrons, which are ejected because of formation of superheated plasma at temperatures of 4000-6000 K and explosive solid-vapor phase transition.

    “When laser-induced photonic energy strikes the metal surface, inverse bremsstrahlung (IB) [78] occurs, where radiation absorption results in the vibration of the electrons, which are ejected because of the formation of superheated plasma at temperatures of 4000–6000 K [79] and explosive solid–vapor phase transition.”

    From Influence of Laser Process Parameters, Liquid Medium, and External Field on the Synthesis of Colloidal Metal Nanoparticles Using Pulsed Laser Ablation in Liquid: A Review (2022) · cites this paper as [79]

    Split into 2 atoms — 0 confirmed, 1 partially supported, 0 disputed, 0 misattributed, 1 unverifiable. Expand the claim to see per-atom verdicts.

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  • Recently, research has applied external magnetic, electric, and temperature fields to examine impact of light-matter interaction and achieve shape control on various types of nanocrystals.

    “Recently [73,74,75,76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96], research has taken a further step, which involved the application of external magnetic, electric, and temperature fields to examine the impact of light–matter interaction and to achieve shape control on various types of nanocrystals.”

    From Influence of Laser Process Parameters, Liquid Medium, and External Field on the Synthesis of Colloidal Metal Nanoparticles Using Pulsed Laser Ablation in Liquid: A Review (2022) · cites this paper as [79]

    The Control of Liquid-Phase Laser Ablation section (pp. 1324–1325) describes investigating pressure and temperature as physical controls, but reports results for changing water pressure. It does not report applying magnetic or electric fields, or achieving nanocrystal shape control with those fields. (LLM, conf=0.84)

    Experimental — accuracy not yet measured
  • Ablation of materials in water generates plasma plumes with a temperature in the range of 4000-8000 K.

    “The ablation of materials in water is reported to generate plasma plumes with a temperature in the range of 4000-8000 K. 132,133,135,137”

    From Green nanoparticle synthesis at scale: a perspective on overcoming the limits of pulsed laser ablation in liquids for high-throughput production (2023) · cites this paper as [135]

    The “Estimations of Plasma Pressure and Temperature” section describes laser ablation of a graphite target in water producing plasma, and the Figure 2 caption says its temperature was evaluated from emission spectra. However, the Conclusions report a temperature of 10⁴ K, not the attributed range of 4000–8000 K. The cited paper supports plasma generation in water but not that numerical range. (LLM, conf=0.88)

    Experimental — accuracy not yet measured
  • A cavitation bubble lifetime is approximately 0.1-1 ms, while persistent microbubbles can stay as long as seconds.

    “While a cavitation bubble lifetime is approximately 0.1-1 ms, 145 persistent microbubbles can stay even as long as seconds.135”

    From Green nanoparticle synthesis at scale: a perspective on overcoming the limits of pulsed laser ablation in liquids for high-throughput production (2023) · cites this paper as [135]

    The citation to this source follows the claim that persistent microbubbles can last for seconds. The Dynamics of Cavitation Bubble section describes a bubble observed at 2.4 ms that then remained stationary, but gives no duration in seconds. Searches for persistent microbubbles and seconds found no passage establishing the claimed lifetime. (LLM, conf=0.72)

    Experimental — accuracy not yet measured

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Cites

Flagged first, then by citations

Research works printed but not linked: 19

  1. [1]1. O. Takai. Pure Appl. Chem. 80, 2003 (2008).
  2. [2]2. F. Mafune, J. Kohno, Y. Takeda, T. Kondow, H. Sawabe. J. Phys. Chem. B 104, 9111 (2000).
  3. [3]3. F. Mafune, J. Kohno, Y. Takeda, T. Kondow, H. Sawabe. J. Phys. Chem. B 105, 5114 (2001).
  4. [4]4. C. H. Liang, Y. Shimizu, T. Sasaki, N. Koshizaki. Appl. Phys. A 80, 819 (2005).
  5. [5]5. T. Tsuji, M. Watanabe, M. Tsuji. Appl. Surf. Sci. 211, 189 (2003).
  6. [6]6. T. Sakka, K. Saito, Y. H. Ogata. Appl. Surf. Sci. 197-198, 246 (2002).
  7. [7]7. Y. Yasui, H. Niino, Y. Kawaguchi, A. Yabe. Appl. Surf. Sci. 186, 552 (2002).
  8. [8]8. G. W. Yang, J. B. Wang, Q. X. Liu. J. Phys.: Condens. Matter 10, 7923 (1998).
  9. [9]9. P. Liu, Y. L. Cao, H. Cui, X. Y. Chen, G. W. Yang. Chem. Mater. 20, 494 (2008).
  10. [10]10. X. Y. Chen, H. Cui, P. Liu, G. W. Yang. Chem. Mater. 20, 2035 (2008).
  11. [11]11. H. Ushida, N. Takada, K. Sasaki. J. Phys. Conf. Series 59, 563 (2007).
  12. [12]12. N. Takada, T. Nakano, K. Sasaki. Appl. Surf. Sci. 255, 9572 (2009).
  13. [13]13. R. Fabbro, J. Fournier, P. Ballard, D. Devaux, J. Virmont. J. Appl. Phys. 68, 775 (1990).
  14. [14]14. K. Sasaki, T. Nakano, W. Soliman, N. Takada. Appl. Phys. Express 2, 046501 (2009).
  15. [15]15. T. Nakano, W. Soliman, N. Takada, K. Sasaki. Technical Digest of 6 th International Conference on Photo-Excited Processes and Applications, p. 72, Sapporo, Japan (2008).
  16. [17]17. W. Soliman, T. Nakano, N. Takada, K. Sasaki. Technical Digest of 6 th International Conference on Photo-Excited Processes and Applications, p. 73, Sapporo, Japan (2008).
  17. [19]19. W. Soliman, N. Takada, K. Sasaki. Appl. Phys. Express 3, 035201 (2010).
  18. [20]20. N. Takada, T. Sasaki, K. Sasaki. Appl. Phys. A 93, 833 (2008).
  19. [21]21. N. Takada, H. Ushida, K. Sasaki. J. Phys. Conf. Series 59, 40 (2007).

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Authors
Sasaki, K., & Takada, N.
Affiliations
  • Hokkaido University (JP)
  • Nagoya University (JP)
Venue
Pure and Applied Chemistry
Published
2010-05-02
Volume
82
Issue
6
Pages
1317-1327
ISSN
  • 0033-4545 (ISSN-L)
  • 1365-3075
OpenAlex
W2150997291
Cited by
111
References
18
Citations by year
2026: 1 · 2024: 5 · 2023: 5 · 2022: 10 · 2021: 7 · 2020: 5 · 2019: 7 · 2018: 6 · 2017: 11 · 2016: 8 · 2015: 4 · 2014: 5 · 2013: 13 · 2012: 17
FWCI
6.99
Type
journal article
Language
en
Open access
Locations
Pure and Applied Chemistry (publishedVersion)
Funders
  • Ministry of Education, Culture, Sports, Science and Technology
  • Japan Society for the Promotion of Science (21510114)
Topics
  • Physical Sciences › Engineering › Biomedical Engineering › Laser-Ablation Synthesis of Nanoparticles
  • Physical Sciences › Engineering › Mechanics of Materials › Laser-induced spectroscopy and plasma
  • Physical Sciences › Engineering › Computational Mechanics › Laser Material Processing Techniques
Keywords
laser-produced plasma, cavitation bubbles, nanoparticle formation, high-pressure plasma, laser-matter interaction

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