2012
DOI: 10.1063/1.4747486
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Publisher’s Note: “Estimating the pressure of laser-induced plasma shockwave by stimulated Raman shift of lattice translational modes” [Appl. Phys. Lett. 101, 021908 (2012)]

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Cited by 5 publications
(10 citation statements)
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“…In addition to filamentation, laserinduced plasma launches a shock wave in the medium because of high pressure and temperature gradients leading to phase transitions of stable molecules [4][5][6][7][8][9][10]. In this Letter, we present (a) the onset of ice VII phase of liquid water detected by a forward SRS signal, and (b) the role of filamentation in SRS, during propagation of a 30 ps pulse through liquid water.Typically, ns laser pulses were employed to create high pressures leading to phase transformations detected by SRS signals in both forward and backward directions [3][4][5][6]9,10]. Recently, the phase transformation of liquid water to ice VII and ice X because of a high shock pressure of 62 GPa generated at the focal volume using high energy nanosecond (12 ns, 532 nm, 360 mJ) laser produced plasma (LPP) is reported [4].…”
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confidence: 95%
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“…In addition to filamentation, laserinduced plasma launches a shock wave in the medium because of high pressure and temperature gradients leading to phase transitions of stable molecules [4][5][6][7][8][9][10]. In this Letter, we present (a) the onset of ice VII phase of liquid water detected by a forward SRS signal, and (b) the role of filamentation in SRS, during propagation of a 30 ps pulse through liquid water.Typically, ns laser pulses were employed to create high pressures leading to phase transformations detected by SRS signals in both forward and backward directions [3][4][5][6]9,10]. Recently, the phase transformation of liquid water to ice VII and ice X because of a high shock pressure of 62 GPa generated at the focal volume using high energy nanosecond (12 ns, 532 nm, 360 mJ) laser produced plasma (LPP) is reported [4].…”
mentioning
confidence: 95%
“…Recently, the phase transformation of liquid water to ice VII and ice X because of a high shock pressure of 62 GPa generated at the focal volume using high energy nanosecond (12 ns, 532 nm, 360 mJ) laser produced plasma (LPP) is reported [4]. The high pressure phases of liquid water such as ice VII, protonated ice VIII, and cuprite ice X were identified with the help of an SRS signal during nanosecond laser pulse excitation [3][4][5]9,10] which have established SRS as an essential tool to estimate the pressure in the medium during phase transitions. Though several studies reported the formation of dynamic states of water excited by ns laser pulses [3][4][5] observation of phase transitions because of optical breakdown using ps [6] and fs pulses, which invoke self-action effects such as filamentation [12][13][14], is sparse.…”
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confidence: 99%
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