• High Power Laser and Particle Beams
  • Vol. 34, Issue 1, 011009 (2022)
Weimin Hu1、3, Xiaojun Wang1、*, Changyong Tian1, Jing Yang1, Ke Liu1, and Qinjun Peng1、2
Author Affiliations
  • 1Key Laboratory of Solid State Lasers, Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing 100190, China
  • 2Key Laboratory of Functional Crystals and Laser Technology, Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing 100190, China
  • 3University of Chinese Academy of Sciences, Beijing 100049, China
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    DOI: 10.11884/HPLPB202234.210321 Cite this Article
    Weimin Hu, Xiaojun Wang, Changyong Tian, Jing Yang, Ke Liu, Qinjun Peng. Influence of mid-infrared laser pulse width on in-band damage threshold of HgCdTe[J]. High Power Laser and Particle Beams, 2022, 34(1): 011009 Copy Citation Text show less

    Abstract

    To study the influence of pulse width on the damage threshold of HgCdTe material irradiated by mid-infrared in-band laser pulse, a one-dimensional model named self-consistent model is established. Some parameters including number density of carrier, carrier and energy current, temperature of carrier and lattice are calculated in the whole process. Damage thresholds of in-band single pulsed laser, whose wavelength is 2.85 μm and pulse width ranges from 30 ps to 10 ns, are obtained. The results show that, damage threshold rauge of in-band laser is 200-500 mJ/cm2. Among them, the damage threshold of 300 ps to 3 ns laser pulses is about 200 mJ/cm2, which is lower than that of other pulsed lasers. The validity of simulation model is verified by setting up the experimental devices and carrying out relevant experiments. Using a single pulsed laser with wavelength of 2.85 μm and pulse width of 300 ps as the light source, the damage threshold is about 200 mJ/cm2. Under the same conditions, when 10 ns single laser pulse is used, the damage threshold is greater than 474 mJ/cm2. The damage process of the HgCdTe material destroyed by hundred-picosecond pulsed laser combines thermal and optical breakdown effects, and its unique mechanism aggravates the destruction of material.
    $ \frac{{\partial n}}{{\partial t}} = \frac{{\alpha I(x,t)}}{{h\nu }} + \frac{{\beta {I^2}(x,t)}}{{h\nu }} - \gamma {n^3} + \theta n - \nabla \cdot {\boldsymbol{J}} $(1)

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    $ {c_{\rm{l}}}{\rho _{\rm{l}}}\frac{{\partial {T_{\rm{l}}}}}{{\partial t}} = \frac{{{c_{{\rm{e}} - {\rm{h}}}}}}{{{\tau _{\rm{e}}}}}({T_{\rm{e}}} - {T_{\rm{l}}}) $(2)

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    $ {c_{{\rm{e}} - {\rm{h}}}}\frac{{\partial {T_{\rm{e}}}}}{{\partial t}} = \left( {\alpha + {\mathit{\Theta}} n} \right)I\left( {x,t} \right) + \beta {I^2}\left( {x,t} \right) - \nabla \cdot {\boldsymbol{W}} - \frac{{{c_{{\rm{e}} - {\rm{h}}}}}}{{{\tau _{\rm{e}}}}}\left( {{T_{\rm{l}}} - {T_{\rm{e}}}} \right) - \frac{{\partial n}}{{\partial t}}\left[ {{E_{\rm{g}}} + 3{k_{\rm{B}}}{T_{\rm{l}}}} \right] $(3)

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    $ {\boldsymbol{J}} = - D\left( {\nabla n + \frac{{2n\nabla {T_{\rm{e}}}}}{{{T_{\rm{e}}}}}} \right) $(4)

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    $ {\boldsymbol{W}} = \left( {{E_{\rm{g}}} + 4{k_{\rm{B}}}{T_{\rm{e}}}} \right) {\boldsymbol{J}} - {k_{\rm{e}}}\nabla {T_{\rm{e}}} $(5)

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    $ I\left( {x,t} \right) = \frac{{\left( {\alpha + {\mathit{\Theta}} n} \right){I_0}{{\rm{e}}^{ - \left( {\alpha + {\mathit{\Theta}} n} \right)x}}}}{{\left( {\alpha + {\mathit{\Theta}} n} \right) + \beta {I_0}\left[ {1 - {{\rm{e}}^{ - \left( {\alpha + {\mathit{\Theta}} n} \right)x}}} \right]}} $(6)

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    $ {I_0}\left( t \right) = \sqrt {\frac{\omega }{\pi }} \frac{{\left( {1 - R} \right)\phi }}{{{t_{\rm{p}}}}}{{\rm{e}}^{ - \omega {{\left( {\tfrac{{t - {t_{\rm{m}}}}}{{{t_{\rm{p}}}}}} \right)}^2}}} $(7)

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    Weimin Hu, Xiaojun Wang, Changyong Tian, Jing Yang, Ke Liu, Qinjun Peng. Influence of mid-infrared laser pulse width on in-band damage threshold of HgCdTe[J]. High Power Laser and Particle Beams, 2022, 34(1): 011009
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