王昭, 杨军, 张敏, 刘文祥, 史国凯, 惠海龙. 石英光纤近红外波段γ辐照效应实验研究[J]. 红外与激光工程, 2024, 53(8): 20240188. DOI: 10.3788/IRLA20240188
引用本文: 王昭, 杨军, 张敏, 刘文祥, 史国凯, 惠海龙. 石英光纤近红外波段γ辐照效应实验研究[J]. 红外与激光工程, 2024, 53(8): 20240188. DOI: 10.3788/IRLA20240188
WANG Zhao, YANG Jun, ZHANG Min, LIU Wenxiang, SHI Guokai, HUI Hailong. Experimental study on γ ray radiation effect of silica optical fiber near infrared band[J]. Infrared and Laser Engineering, 2024, 53(8): 20240188. DOI: 10.3788/IRLA20240188
Citation: WANG Zhao, YANG Jun, ZHANG Min, LIU Wenxiang, SHI Guokai, HUI Hailong. Experimental study on γ ray radiation effect of silica optical fiber near infrared band[J]. Infrared and Laser Engineering, 2024, 53(8): 20240188. DOI: 10.3788/IRLA20240188

石英光纤近红外波段γ辐照效应实验研究

Experimental study on γ ray radiation effect of silica optical fiber near infrared band

  • 摘要: 为提高某光学干涉测量系统的耐辐射能力,开展耐辐射光纤选型实验。以剂量率为0.5 Gy·s−1的稳态γ射线和剂量率为5.0×109 Gy·s−1、脉冲宽度约20 ns的瞬态强γ射线为辐照源,获得掺锗、掺氟耐辐射单模光纤和常规G.652光纤在工作波长1 550 nm、注入光功率40 mW工况下的辐射感生损耗,结果表明,实验获得的在线辐射感生损耗数据真实可靠;在稳态γ射线作用下,掺锗和掺氟耐辐射光纤的性能差异不大,辐射感生损耗小于17 dB·km−1,随着辐射时间的增加,辐射损耗呈现饱和,耐辐射光纤的性能均优于常规单模G.652通信光纤;在瞬态强γ射线作用下,两个不同型号掺氟光纤的性能最优,辐射感生损耗峰值分别为471.5 dB·km−1和608.6 dB·km−1,恢复通信时长约μs量级。掺锗光纤的瞬态辐照性能最差,辐射感生损耗峰值为2 691.3 dB·km−1,在μs时间尺度维持感生损耗饱和状态。

     

    Abstract:
    Objective With the continuous development of optical fiber production technology, optical fiber sensing technology has been widely used in radiation environments such as outer space and nuclear power plants. However, under the action of radiation sources such as X-ray, γ-ray, electron and neutron, optical fiber will produce radiation induced loss especially in the intense pulse radiation field, the transient induced loss of optical fiber can reach thousands of dB, which has been widely concerned. To carry out the experimental study on the mechanical effect of radiation beam acting on materials, a set of optical fiber displacement interferometry system was established to obtain the dynamic mechanical response parameters of various materials under irradiation. In order to improve the radiation resistance of the interferometry system, it is necessary to carry out the examination experiments of various types of radiation-resistant quartz optical fibers and select the optical fibers with excellent radiation resistance.
    Methods Based on the established optical fiber displacement interferometry system, it is necessary to carry out irradiation experiments. Under the conditions of working wavelength of 1 550 nm and injected optical power of 40 mW, the online induced loss values of various radiation-resistant single-mode fibers under steady and transient irradiation are obtained, and there is no relevant data at home and abroad at present. The radiation sources selected in the experiment include 60Co radiation source and " Qiangguang-Ⅰ" γ pulse radiation source, respectively with radiation dose rates of 0.5 Gy·s−1 and 5.0×109 Gy·s−1, where the pulse width of the pulse radiation source is about 20 ns. The fiber samples selected in the experiment include Ge-doped radiation-resistant single-mode quartz fiber, F-doped radiation-resistant single-mode quartz fiber and G.652 ordinary single-mode fiber. All optical fiber samples were arranged in the radiation window, and the radiation induced loss of optical fiber in steady and transient irradiation experiments was obtained at the same time to obtain its radiation resistance.
    Results and Discussions Under the steady irradiation of 60Co with a dose rate of 0.5 Gy·s−1 and a total dose of about 2.5 kGy, the radiation-induced loss of the samples of Ge-doped and F-doped radiation-resistant fiber is less than 17 dB·km−1, and that of the corresponding 10 m optical fiber is less than 0.2 dB. With the increase of irradiation time, the radiation-induced loss is saturated. However, the radiation-induced loss of conventional G.652 single-mode fiber increases with the increase of irradiation time, and the induced loss is more than 40 dB·km−1. Under the action of intense γ pulse with a peak dose rate of 5×109 Gy·s−1 and a pulse width of about 20 ns, two different types of F-doped optical fibers have the best radiation resistance, respectively with the peak radiation-induced loss of 471.5 dB·km−1 and 608.6 dB·km−1, and the recovery time of communication is about μs. The peak radiation-induced loss of conventional G.652 single-mode fiber is 2 378.2 dB·km−1. Ge-doped fiber has the worst radiation resistance, and the peak radiation-induced loss is 2 691.3 dB·km−1, which keeps the induced loss saturated in μs time scale. Ge-doped fiber can be used in steady-state radiation environment, but not in transient radiation environment. The reason for this phenomenon is that Ge-doped fiber is easier to produce defects under irradiation, but the recovery speed of defects in this kind of fiber is relatively fast. Under transient strong radiation, the defects produced by Ge-doped fiber are more obvious, and the phenomenon of "color center" appears for a long time.
    Conclusions The experimental results of steady-state and transient irradiation can be summarized as follows: 1) The designed optical fiber irradiation experiment successfully obtained the radiation-induced loss of each optical fiber sample under steady-state and transient irradiation conditions. Especially, the introduction of reference light path not only eliminates the influence of the fluctuation of laser and photoelectric converter on the measurement, but also improves the reliability of the measurement data and plays an important role. 2) The real-time induced loss curves of Ge-doped, F-doped and G.652 single-mode fibers under the same radiation source are successfully obtained at the working wavelength of 1 550 nm, and the response differences of various types of radiation-resistant fibers are compared and analyzed. 3) Compared with others, Ge-doped radiation-resistant single-mode fiber is more sensitive to irradiation dose rate and can be used in steady-state irradiation. F-doped radiation-resistant single-mode fiber has good radiation resistance, which can be used in steady and transient intense irradiation conditions.

     

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