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Underwater acoustic signals induced by intense ultrashort laser pulse
1. K. Plamann, F. Aptel, C. L. Arnold, A. Courjaud, C. Crotti, F. Deloison, F. Druon, P. Georges, M. Hanna, J.-M. Legeais, F. Morin, E. Mottay, V. Nuzzo, D. A. Peyrot, and M. Savoldelli, “ Ultrashort pulse laser surgery of the cornea and the sclera,” J. Opt. 12, 084002 (2010).
2. A. Vogel, N. Linz, S. Freidank, and G. Paltauf, “ Femtosecond-laser-induced nanocavitation in water: Implications for optical breakdown threshold and cell surgery,” Phys. Rev. Lett. 100, 038102 (2008).
3. J. Woodworth, I. Molina, D. Nelson, J. Maenchen, G. Sarkisov, J. Blickem, R. Starbird, F. Wilkins, D. Van DeValde, and D. Johnson, “ Green-laser-triggered water switching at 1.6 MV,” IEEE Trans. Dielecr. Electr. Insul. 14, 951–957 (2007).
4. T. G. Jones, A. Ting, J. Penano, P. Sprangle, and G. DiComo, “ Remote underwater ultrashort pulse laser acoustic source,” in CThA1, Conference on Lasers and Electro-Optics/Conference on Quantum Electronics and Laser Science 2006 (2006).
5. W. Lauterborn and A. Vogel, Bubble Dynamics and Shock Waves, SHOCKWAVES 8, edited by C. F. Delale ( Springer-Verlag, Berlin, 2013), pp. 67–103.
6. F. Blackmon and L. Antonelli, “ Experimental demonstration of multiple pulse nonlinear optoacoustic signal generation and control,” Appl. Opt. 44, 103–112 (2005).
7. A. Vogel and W. Lauterborn, “ Acoustic transient generation by laser-produced cavitation bubbles near solid boundaries,” J. Acoust. Soc. Am. 84, 719–731 (1988).
9. S. Sreeja, C. Leela, V. R. Kumar, S. Bagchi, T. S. Prashant, P. Radhakrishnan, S. P. Tewari, S. V. Rao, and P. P. Kiran, “ Dynamics of tightly focused femtosecond laser pulses in water,” Laser Phys. 23, 106002 (2013).
10. M. H. Helle, T. G. Jones, J. R. Penano, D. Kaganovich, and A. Ting, “ Formation and propagation of meter-scale laser filaments in water,” Appl. Phys. Lett. 103, 121101 (2013).
12. D. W. Tang, B. L. Zhou, H. Cao, and G. H. He, “ Dynamic thermal expansion under transient laser-pulse heating,” Appl. Phys. Lett. 59, 3113–3114 (1991).
13. J. Noack and A. Vogel, “ Laser-induced plasma formation in water at nanosecond to femtosecond time scales: Calculation of thresholds, absorption coefficients, and energy density,” IEEE J. Quant. Electron. 35, 1156–1167 (1999).
14. A. Vogel, J. Noack, K. Nahen, D. Theisen, S. Busch, U. Parlitz, D. X. Hammer, G. D. Noojin, B. A. Rockwell, and R. Birngruber, “ Energy balance of optical breakdown in water at nanosecond to femtosecond time scales,” Appl. Phys. B 68, 271–280 (1999).
16. T. G. Jones, A. Ting, J. Penano, P. Sprangle, and L. D. Bibee, “ Remote intense laser acoustic source,” NRL Rev. 2007, 121–123.
17. R. T. Beyer, Nonlinear Acoustics ( Department of the Navy, Sea Systems Command, Washington, DC, 1974).
18.A secundary acoustic source generated at the air/water surface was also detected when the geometric focus of the lens gets closer to the interface (i.e., for h large).
19. G. Point, Y. Brelet, A. Houard, V. Jukna, C. Milián, J. Carbonnel, Y. Liu, A. Couairon, and A. Mysyrowicz, “ Superfilamentation in air,” Phys. Rev. Lett. 112, 223902 (2014).
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generated in water by terawatt (TW) laser pulses undergoing filamentation are studied. The acoustic signal has a very broad spectrum, spanning from 0.1 to 10 MHz and is confined in the plane perpendicular to the laser direction. Such a source appears to be promising for the development of remote laser based acoustic applications.
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