TY - JOUR
T1 - Wavelength dependence of nanosecond infrared laser-induced breakdown in water
T2 - Evidence for multiphoton initiation via an intermediate state
AU - Linz, Norbert
AU - Freidank, Sebastian
AU - Liang, Xiao Xuan
AU - Vogelmann, Hannes
AU - Trickl, Thomas
AU - Vogel, Alfred
PY - 2015/4/29
Y1 - 2015/4/29
N2 - Investigation of the wavelength dependence (725-1025 nm) of the threshold for nanosecond optical breakdown in water revealed steps consistent with breakdown initiation by multiphoton ionization, with an initiation energy of about 6.6 eV. This value is considerably smaller than the autoionization threshold of about 9.5 eV, which can be regarded as band gap relevant for avalanche ionization. Breakdown initiation is likely to occur via excitation of a valence band electron into a solvated state, followed by rapid excitation into the conduction band. Theoretical analysis based on these assumptions suggests that the seed electron density required for initiating avalanche ionization amounts to 2.5×1015cm-3 at 725nm and drops to 1.1×1012cm-3 at 1025 nm. These results demand changes of future breakdown modeling for water, including the use of a larger band gap than previously employed, the introduction of an intermediate energy level for initiation, and consideration of the wavelength dependence of seed electron density.
AB - Investigation of the wavelength dependence (725-1025 nm) of the threshold for nanosecond optical breakdown in water revealed steps consistent with breakdown initiation by multiphoton ionization, with an initiation energy of about 6.6 eV. This value is considerably smaller than the autoionization threshold of about 9.5 eV, which can be regarded as band gap relevant for avalanche ionization. Breakdown initiation is likely to occur via excitation of a valence band electron into a solvated state, followed by rapid excitation into the conduction band. Theoretical analysis based on these assumptions suggests that the seed electron density required for initiating avalanche ionization amounts to 2.5×1015cm-3 at 725nm and drops to 1.1×1012cm-3 at 1025 nm. These results demand changes of future breakdown modeling for water, including the use of a larger band gap than previously employed, the introduction of an intermediate energy level for initiation, and consideration of the wavelength dependence of seed electron density.
UR - http://www.scopus.com/inward/record.url?scp=84928819396&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.91.134114
DO - 10.1103/PhysRevB.91.134114
M3 - Journal articles
AN - SCOPUS:84928819396
SN - 1098-0121
VL - 91
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 13
M1 - 134114
ER -