pulse laser irradiation
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2021 ◽  
Vol 11 (22) ◽  
pp. 10555
Author(s):  
Yao Ma ◽  
Qiang Huang ◽  
Yixin Yu ◽  
Yuan Dong ◽  
Hui Li ◽  
...  

Carbon fiber reinforced polymers (CFRP) are a widely used composite material applied in both commercial and industrial utilization. Based on the heat conduction theory, a theoretical model for the temperature rise of braided CFRP irradiated by long pulse laser is established in this work, and the time required for the maximum temperature rise of CFRP (with different thicknesses) to be acted by long pulse laser with different energy densities and pulse widths is simulated. At the same time, the temperature rise experiment and damage morphology of a long pulse laser with braided CFRP were carried out. The theoretical simulation results are in good agreement with the experimental results, which verifies the correctness of the theoretical model. The results of this paper will provide a theoretical basis for laser processing of CFRP.


2021 ◽  
pp. 117270
Author(s):  
Vladimir Ya. Shur ◽  
Mikhail S. Kosobokov ◽  
Andrey V. Makaev ◽  
Dmitry K. Kuznetsov ◽  
Maxim S. Nebogatikov ◽  
...  

2021 ◽  
Vol 11 (1) ◽  
Author(s):  
Michiko Sasaki ◽  
Masahiro Goto

AbstractThe fabrication of functional conductive polymer nanowires (CPNWs), including ultrahigh-sensitive flexible nanosensors has attracted considerable attention in field of the Internet of Things. However, the controllable and space-selective growth of CPNWs remains challenging, and a novel synthetic technique is required. Herein, we demonstrate the synthesis of space-selective CPNWs that include quantum dots (QDs) with changeable optical properties via single-pulse laser irradiation in air at atmospheric pressure. Time-resolved shadowgraphy was applied to monitor the synthetic process of the CPNWs and optimise the process conditions. The electrical conductivity of the CPNWs with QDs (QD-CPNWs) was analysed in the presence and absence of light irradiation and was found to change drastically (over six times) under light irradiation. QD-CPNW synthesis under laser irradiation shows great potential for fabricating highly photosensitive functional nanomaterials and is expected to be applied in the production of ultrahigh-sensitive photosensors in the future.


Author(s):  
John Lopez ◽  
Kévin Gaudfrin ◽  
Konstantin Mishchik ◽  
Martin Delaigue ◽  
Clemens Hönninger ◽  
...  

Author(s):  
Vanessa Harumi Kiyan ◽  
Flávia Pires Rodrigues ◽  
Ricardo Elgul Samad ◽  
Denise Maria Zezell ◽  
Marco Antonio Bottino ◽  
...  

2020 ◽  
Vol 10 (19) ◽  
pp. 6642 ◽  
Author(s):  
Mingjun Chen ◽  
Wenyu Ding ◽  
Jian Cheng ◽  
Hao Yang ◽  
Qi Liu

As a hard and brittle material, KDP crystal is easily damaged by the irradiation of laser in a laser-driven inertial confinement fusion device due to various factors, which will also affect the quality of subsequent incident laser. Thus, the mechanism of laser-induced damage is essentially helpful for increasing the laser-induced damage threshold and the value of optical crystal elements. The intrinsic damage mechanism of crystal materials under laser irradiation of different pulse duration is reviewed in detail. The process from the initiation to finalization of laser-induced damage has been divided into three stages (i.e., energy deposition, damage initiation, and damage forming) to ensure the understanding of laser-induced damage mechanism. It is clear that defects have a great impact on damage under short-pulse laser irradiation. The burst damage accounts for the majority of whole damage morphology, while the melting pit are more likely to appear under high-fluence laser. The three stages of damage are complementary and the multi-physics coupling technology needs to be fully applied to ensure the intuitive prediction of damage thresholds for various initial forms of KDP crystals. The improved laser-induced damage threshold prediction can provide support for improving the resistance of materials to various types of laser-induced damage.


2020 ◽  
Vol 27 (8) ◽  
pp. 083518 ◽  
Author(s):  
Kavya H. Rao ◽  
N. Smijesh ◽  
D. Chetty ◽  
I. V. Litvinyuk ◽  
R. T. Sang

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