TY - JOUR
T1 - Energy deposition of explosive materials under femtosecond-laser irradiation
AU - Li, Junjian
AU - Wu, Junying
AU - Yang, Lijun
AU - Shang, Yiping
AU - Yao, Yule
AU - Wang, Jianyu
AU - Zheng, Fude
AU - Chen, Lang
N1 - Publisher Copyright:
© 2025
PY - 2025/3
Y1 - 2025/3
N2 - The absorption of femtosecond-laser energy by energy material is influenced by the material's optical absorption coefficients. To study the energy deposition of a 810-nm near-infrared femtosecond laser in explosive materials, we calculated their reflection coefficient, linear absorption coefficient, and two- and three-photon absorption coefficients using a first-principles method. The materials studied were HMX, TATB, RDX, PETN, and TNT. We obtained the energy deposition at two intensities (1013 and 1014 W/cm2). The results showed that the reflection coefficients differ among the different explosives, decreasing in the order of TATB > TNT > RDX > PETN > HMX, and the linear absorption coefficient decrease in the order of TATB > TNT > RDX > HMX > PETN. Thus, the strongest laser absorption was observed for TATB. For near infrared laser with a wavelength of 810 nm, TATB and TNT have a weak two-photon absorption effect and a strong three-photon absorption effect, whereas HMX, RDX, and PETN have almost no two-photon absorption effect and only a very weak three-photon absorption effect. A higher laser power density corresponds to a stronger ability of explosives to absorb laser energy through the multiphoton effect. For a given laser energy, the ablation depth of explosives increases in the order of TATB < TNT < RDX < HMX < PETN.
AB - The absorption of femtosecond-laser energy by energy material is influenced by the material's optical absorption coefficients. To study the energy deposition of a 810-nm near-infrared femtosecond laser in explosive materials, we calculated their reflection coefficient, linear absorption coefficient, and two- and three-photon absorption coefficients using a first-principles method. The materials studied were HMX, TATB, RDX, PETN, and TNT. We obtained the energy deposition at two intensities (1013 and 1014 W/cm2). The results showed that the reflection coefficients differ among the different explosives, decreasing in the order of TATB > TNT > RDX > PETN > HMX, and the linear absorption coefficient decrease in the order of TATB > TNT > RDX > HMX > PETN. Thus, the strongest laser absorption was observed for TATB. For near infrared laser with a wavelength of 810 nm, TATB and TNT have a weak two-photon absorption effect and a strong three-photon absorption effect, whereas HMX, RDX, and PETN have almost no two-photon absorption effect and only a very weak three-photon absorption effect. A higher laser power density corresponds to a stronger ability of explosives to absorb laser energy through the multiphoton effect. For a given laser energy, the ablation depth of explosives increases in the order of TATB < TNT < RDX < HMX < PETN.
KW - Absorption coefficient
KW - Femtosecond laser
KW - First-principles calculations
KW - Multiphoton absorption effect
KW - Reflection coefficient
UR - http://www.scopus.com/inward/record.url?scp=85218450628&partnerID=8YFLogxK
U2 - 10.1016/j.mtcomm.2025.111980
DO - 10.1016/j.mtcomm.2025.111980
M3 - Article
AN - SCOPUS:85218450628
SN - 2352-4928
VL - 44
JO - Materials Today Communications
JF - Materials Today Communications
M1 - 111980
ER -