\begin{document}${\pi }/{2}$\end{document}. At half of the Talbot distance, the number of sub-images is the same as that of the emitters, while the spatial position of sub-image is shifted by half a cycle along the angular direction. Moreover, the sub-images with twice the number of the emitters are present in three quarters of the Talbot distance. The light intensities of the sub-images are identical and the difference in phase between adjacent sub-images is \begin{document}$- {\pi }/{2}$\end{document}. Further, the Talbot images with the same spatial and phase distribution as the emitters are generated along the angular direction at the Talbot distance. The optical profile and phase distribution of one dimensional laser array at the fractional Talbot distance are also simulated by FDTD Solutions for comparison. It is found that the edge effect of one-dimensional laser array leads to the uneven distribution of near-field light intensity, in which the intensity of light spot on the edge of array is significantly lower than that in the center of array. While the Talbot sub-images of ring laser array with identical light intensity are obtained. Therefore, We consider that the ring laser array can effectively eliminate the edge effect. The results are helpful in studying the external cavity phase locking of ring laser arrays and its applications in the field of high brightness coherent laser and quantum measurement."> - 必威体育下载

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    Li Wei, Dai Jing-Jing, Wen Cong-Yang, Zong Meng-Ya, Li Sheng-Nan, Wang Zhi-Yong
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    • Abstract views:2660
    • PDF Downloads:41
    • Cited By:0
    Publishing process
    • Received Date:20 December 2022
    • Accepted Date:11 January 2023
    • Available Online:03 February 2023
    • Published Online:05 March 2023

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