Research on potential problems of object image grating self-tiling for applications in large aperture optical systems
Zhaoyang Li, Tao Wang, Guang Xu, Dawei Li, Jianwei Yu, Weixin Ma, Jian Zhu, Lei Chen, Yaping Dai. Research on potential problems of object image grating self-tiling for applications in large aperture optical systems[J]. Collection Of theses on high power laser and plasma physics, 2013, 11(1): 0718.
[1] G. Mourou and T. Tajima, “The extreme light infrastructure: optics’ next horizon,” Opt. Photon. News 22(7), 47–51 (2011).
[2] D. Pepler, A. Boyle, J. Collier, M. Galimberti, C. Hernandez- Gomez, P. Holligan, A. Kidd, A. Lyachev, I. Musgrave, W. Shaikh, Y. Tang, and T. Winstone, “The 10 petawatt upgrade proposal for the Vulcan high-power laser,” in Proceedings of ICALEPCS 2009 (JACoW, 2009), pp. 272–274.
[3] https://lasers.llnl.gov/.
[4] http://www.lle.rochester.edu/.
[5] http://www lmj.cea.fr/.
[6] http://www.clf.rl.ac.uk/.
[7] http://www.ile.osaka u.ac.jp/.
[8] J. Qiao, A. Kalb, T. Nguyen, J. Bunkenburg, D. Canning, and J. H. Kelly, “Demonstration of large-aperture tiled-grating compressors for high-energy, petawatt-class, chirpedpulse amplification systems,” Opt. Lett. 33, 1684–1686 (2008).
[9] A. Cotel, C. Crotti, P. Audebert, C. L. Bris, and C. L. Blanc, “Tiled-grating compression of multiterawatt laser pulses,” Opt. Lett. 32, 1749–1751 (2007).
[10] G. Xu, T. Wang, Z. Li, Y. Dai, Z. Lin, Y. Gu, and J. Zhu, “1 kJ petawatt laser system for SG-II-U program,” Rev. Laser Eng. (Suppl.) 2008 1172–1175 (2008).
[11] J. Hoose, E. Loewen, R. Wiley, T. Blasiak, S. Zheleznyak, and T. Sroda, “Grand gratings: bigger is better, thanks to mosaic technology,” Photon. Spectra 29, 118–120 (1995).
[12] T. Zhang, M. Yonemura, and Y. Kato, “An array-grating compressor for high-power chirped-pulse amplification lasers,” Opt. Commun. 145, 367–376 (1998).
[13] T. J. Kessler, J. Bunkenburg, H. Huang, A. Kozlov, and D. D. Meyerhofer, “Demonstration of coherent addition of multiple gratings for high-energy chirped-pulse-amplified lasers,” Opt. Lett. 29, 635–637 (2004).
[14] Y. Hu, L. Zeng, and L. Li, “Method to mosaic gratings that relies on analysis of far-field intensity patterns in two wavelengths,” Opt. Commun. 269, 285–290 (2007).
[15] Y. Hu and L. Zeng, “Grating mosaic based on image processing for far-field diffraction intensity patterns in two wavelengths,” Appl. Opt. 46, 7018–7025 (2007).
[16] A. Cotel, M. Castaing, P. Pichon, and C. Le Blanc, “Phasedarray grating compression for high-energy chirped pulse amplification lasers,” Opt. Express 15, 2742–2752 (2007).
[17] J. Qiao, A. Kalb, M. J. Guardalben, G. King, D. Canning, and J. H. Kelly, “Large-aperture grating tiling by interferometry for petawatt chirped-pulse-amplification systems,” Opt. Express 15, 9562–9574 (2007).
[18] M. Hornung, R. B defeld, M. Siebold, M. Schnepp, J. Hein, R. Sauerbrey, and M. C. Kaluza, “Alignment of a tiled-grating compressor in a high-power chirped-pulse amplification laser system,” Appl. Opt. 46, 7432–7435 (2007).
[19] M. Hornung, R. B defeld, A. Kessler, J. Hein, and M. C. Kaluza, “Spectrally resolved and phase-sensitive far-field measurement for the coherent addition of laser pulses in a tiled grating compressor,” Opt. Lett. 35, 2073–2075 (2010).
[20] L. Zeng and L. Li, “Method of making mosaic gratings by using a two-color heterodyne interferometer containing a reference grating,” Opt. Lett. 31, 152–154 (2006).
[21] Y. Zuo, X.Wei, X.Wang, Q. Zhu, R. Ren, Z. Huang, and H. Liu, “Eliminating the longitudinal piston error between tiled gratings by angle tuning,” Opt. Lett. 32, 280–282 (2007).
[22] M. C. Rushford, J. A. Britten, C. P. J. Barty, T. Jitsuno, K. Kondo, N. Miyanaga, K. A. Tanaka, R. Kodama, and G. Xu, “Split-aperture laser pulse compressor design tolerant to alignment and line-density differences,” Opt. Lett. 33, 1902–1904 (2008).
[23] H. Habara, G. Xu, T. Jitsuno, R. Kodama, K. Suzuki, K. Sawai, K. Kondo, N. Miyanaga, K. A. Tanaka, K. Mima, M. C. Rushford, J. A. Britten, and C. P. J. Barty, “Pulse compression and beam focusing with segmented diffraction gratings in a high-power chirped-pulse amplification glass laser system,” Opt. Lett. 35, 1783–1785 (2010).
[24] N. Blanchot, E. Bar, G. Behar, C. Bellet, D. Bigourd, F. Boubault, C. Chappuis, H. Co c, C. Damiens-Dupont, O. Flour, O. Hartmann, L. Hilsz, E. Hugonnot, E. Lavastre, J. Luce, E. Mazataud, J. Neauport, S. Noailles, B. Remy, F. Sautarel, M. Sautet, and C. Rouyer, “Experimental demonstration of a synthetic aperture compression scheme for multi-petawatt high-energy lasers,” Opt. Express 18, 10088–10097 (2010).
[25] Z. Li, G. Xu, T. Wang, and Y. Dai, “Object-image-grating selftiling to achieve and maintain stable, near-ideal tiled grating conditions,” Opt. Lett. 35, 2206–2208 (2010).
[26] “Physik Instrumente,” http://www.physikinstrumente.com/en/ index.php.
[27] Y. Kitagawa, H. Fujita, R. Kodama, H. Yoshida, S. Matsuo, T. Jitsuno, T. Kawasaki, H. Kitamura, T. Kanabe, S. Sakabe, K. Shigemori, N. Miyanaga, and Y. Izawa, “Prepulse-free petawatt laser for a fast ignitor,” IEEE J. Quantum Electron. 40, 281–293 (2004).
Zhaoyang Li, Tao Wang, Guang Xu, Dawei Li, Jianwei Yu, Weixin Ma, Jian Zhu, Lei Chen, Yaping Dai. Research on potential problems of object image grating self-tiling for applications in large aperture optical systems[J]. Collection Of theses on high power laser and plasma physics, 2013, 11(1): 0718.
PDF全文
