Generation of high quality ion beams through the stable radiation pressure acceleration of the near critical density target<xref rid="cpb_26_6_065203fn1" ref-type="fn">*</xref><fn id="cpb_26_6_065203fn1"><label>*</label><p>Project supported by the National Natural Science Foundation of China (Grant Nos. 11365020, 11475026, 11565022, and 11547304), the Science and Technology Program of Gansu Province of China (Grant No. 1606RJZA090), the Fundamental Research Funds for the Higher Education Institutions of Gansu Province of China (2012), the Foundation of Northwest Normal University (Grant Nos. NWNU-LKQN-14-9 and NWNU-LKQN-16-3), and partially supported by the Fundamental Research Funds for the Central Universities of China.</p></fn>

Generation of high quality ion beams through the stable radiation pressure acceleration of the near critical density target**

Project supported by the National Natural Science Foundation of China (Grant Nos. 11365020, 11475026, 11565022, and 11547304), the Science and Technology Program of Gansu Province of China (Grant No. 1606RJZA090), the Fundamental Research Funds for the Higher Education Institutions of Gansu Province of China (2012), the Foundation of Northwest Normal University (Grant Nos. NWNU-LKQN-14-9 and NWNU-LKQN-16-3), and partially supported by the Fundamental Research Funds for the Central Universities of China.

Hong Xue-Ren¹, Zhou Wei-Jun^{1, †}, Xie Bai-Song², Yang Yang¹, Wang Li¹, Tian Jian-Min¹, Tang Rong-An¹, Duan Wen-Shan¹

(color online) The normalized density distributions of the electron and the proton in the 2D simulations. The left column is the result of the NCD target and the right column is of the HD-NCD target. Here, represents the electron density of the HD layer, and denote the densities of the electron and the proton of the NCD layer, respectively. Panels (a1) and (b1) are the results at , panels (a2) and (b2) are at , panels (a3) and (b3) are at , panels (a4) and (b4) are at .