• Acta Physica Sinica
  • Vol. 68, Issue 18, 185205-1 (2019)
Bao Du1, Hong-Bo Cai1、2、3、*, Wen-Shuai Zhang1, Jing Chen1、2、3, Shi-Yang Zou1, and Shao-Ping Zhu1、4、5、*
Author Affiliations
  • 1Institute of Applied Physics and Computational Mathematics, Beijing 100094, China
  • 2HEDPS, Center for Applied Physics and Technology, Peking University, Beijing 100871, China
  • 3IFSA Collaborative Innovation Center, Shanghai Jiao Tong University, Shanghai 200240, China
  • 4Graduate School, China Academy of Engineering Physics, Beijing 100088, China
  • 5STPPL, Research Center of Laser Fusion, China Academy of Engineering Physics, Mianyang 621900, China
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    DOI: 10.7498/aps.68.20190775 Cite this Article
    Bao Du, Hong-Bo Cai, Wen-Shuai Zhang, Jing Chen, Shi-Yang Zou, Shao-Ping Zhu. Deflection effect of electromagnetic field generated byWeibel instability on proton probe[J]. Acta Physica Sinica, 2019, 68(18): 185205-1 Copy Citation Text show less
    Schematic diagram of the proton radiography of the Weibel instabilityWeibel不稳定性的质子照相示意图
    Fig. 1. Schematic diagram of the proton radiography of the Weibel instabilityWeibel不稳定性的质子照相示意图
    Three demensional distributions of the Weibel instability generated (a) magnetic field By and (b) electric field Ex at t = 1.06 psWeibel不稳定性 (a)自生磁场By和(b)自生电场Ex在t = 1.06 ps时的三维空间分布
    Fig. 2. Three demensional distributions of the Weibel instability generated (a) magnetic field By and (b) electric field Ex at t = 1.06 ps Weibel不稳定性 (a)自生磁场By和(b)自生电场Ext = 1.06 ps时的三维空间分布
    Evolution of the energy of the Weibel instability generated magnetic and electric fields.Weibel不稳定性自生磁场和电场能量随着时间的演化
    Fig. 3. Evolution of the energy of the Weibel instability generated magnetic and electric fields.Weibel不稳定性自生磁场和电场能量随着时间的演化
    Spatial distributions of (a) the magnetic field strength |B|, (b) the electric field strength |E|, (c) the direction of B and (d) the direction of E on the z = 0 plane, (e) the y component of the magnetic field By and (f) the y component of the electric field Ey on the y = 0 plane at t = 1.06 ps.t = 1.06 ps时, z = 0平面上(a)磁场强度|B|、(b)电场强度|E|、(c)磁场方向和(d)电场方向的分布情况以及y = 0平面上(e) y向磁场By和(f) y向电场Ey的分布情况
    Fig. 4. Spatial distributions of (a) the magnetic field strength |B|, (b) the electric field strength |E|, (c) the direction of B and (d) the direction of E on the z = 0 plane, (e) the y component of the magnetic field By and (f) the y component of the electric field Ey on the y = 0 plane at t = 1.06 ps. t = 1.06 ps时, z = 0平面上(a)磁场强度|B|、(b)电场强度|E|、(c)磁场方向和(d)电场方向的分布情况以及y = 0平面上(e) y向磁场By和(f) y向电场Ey的分布情况
    Spatial distributions of (a) the magnetic field strength |B|, (b) the electric field strength |E|, (c) the direction of B and (d) the direction of E on the z = 0 plane, (e) the y component of the magnetic field By and (f) the y component of the electric field Ey on the y = 0 plane at t = 4.78 ps.t = 4.78 ps时, z = 0平面上(a)磁场强度|B|、(b)电场强度|E|、(c)磁场方向和(d)电场方向的分布情况以及y = 0平面上(e) y向磁场By和(f) y向电场Ey的分布情况
    Fig. 5. Spatial distributions of (a) the magnetic field strength |B|, (b) the electric field strength |E|, (c) the direction of B and (d) the direction of E on the z = 0 plane, (e) the y component of the magnetic field By and (f) the y component of the electric field Ey on the y = 0 plane at t = 4.78 ps. t = 4.78 ps时, z = 0平面上(a)磁场强度|B|、(b)电场强度|E|、(c)磁场方向和(d)电场方向的分布情况以及y = 0平面上(e) y向磁场By和(f) y向电场Ey的分布情况
    Proton flux density perturbations on the detection plane when (a) only the electric field is included, (b) only the magnetic field is included and (c) both the electric and magnetic fields are included at t = 1.06 ps.t = 1.06 ps时, (a)只考虑电场E、(b)只考虑磁场B以及(c)同时考虑电场E和磁场B三种情况下探测面上的质子通量密度扰动分布信息
    Fig. 6. Proton flux density perturbations on the detection plane when (a) only the electric field is included, (b) only the magnetic field is included and (c) both the electric and magnetic fields are included at t = 1.06 ps. t = 1.06 ps时, (a)只考虑电场E、(b)只考虑磁场B以及(c)同时考虑电场E和磁场B三种情况下探测面上的质子通量密度扰动分布信息
    Proton flux density perturbations on the detection plane when (a) only the electric field is included, (b) only the magnetic field is included and (c) both the electric and magnetic fields are included at t = 4.78 ps.t = 4.78 ps时(a)只考虑电场E、(b)只考虑磁场B以及(c)同时考虑电场E和磁场B三种情况下探测面上的质子通量密度扰动分布信息
    Fig. 7. Proton flux density perturbations on the detection plane when (a) only the electric field is included, (b) only the magnetic field is included and (c) both the electric and magnetic fields are included at t = 4.78 ps. t = 4.78 ps时(a)只考虑电场E、(b)只考虑磁场B以及(c)同时考虑电场E和磁场B三种情况下探测面上的质子通量密度扰动分布信息
    Bao Du, Hong-Bo Cai, Wen-Shuai Zhang, Jing Chen, Shi-Yang Zou, Shao-Ping Zhu. Deflection effect of electromagnetic field generated byWeibel instability on proton probe[J]. Acta Physica Sinica, 2019, 68(18): 185205-1
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