• High Power Laser Science and Engineering
  • Vol. 6, Issue 4, 04000e63 (2018)
F. Zhang1, Z. G. Deng1, L. Q. Shan1, Z. M. Zhang1, B. Bi1, D. X. Liu1, W. W. Wang1, Z. Q. Yuan1, C. Tian1, S. Q. Yang1, B. Zhang1, and Y. Q. Gu1、2、†,*
Author Affiliations
  • 1Science and Technology on Plasma Physics Laboratory , Laser Fusion Research Center , China Academy of Engineering Physics , Mianyang 621900 , China
  • 2IFSA Collaborative Innovation Center , Shanghai Jiao Tong University , Shanghai 200240 , China
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    DOI: 10.1017/hpl.2018.65 Cite this Article Set citation alerts
    F. Zhang, Z. G. Deng, L. Q. Shan, Z. M. Zhang, B. Bi, D. X. Liu, W. W. Wang, Z. Q. Yuan, C. Tian, S. Q. Yang, B. Zhang, Y. Q. Gu. All-optical acceleration in the laser wakefield[J]. High Power Laser Science and Engineering, 2018, 6(4): 04000e63 Copy Citation Text show less
    All-optical ‘Generator and Booster’ scheme of muon source. Muons are first generated by the Bethe–Heitler process, the ‘Generator’, via high-energy photons from Bremsstrahlung radiation of laser wakefield accelerated electrons interacting with highmaterials. After a proper collection and focusing system, muons are boosted by another laser wakefield, the ‘Booster’.
    Fig. 1. All-optical ‘Generator and Booster’ scheme of muon source. Muons are first generated by the Bethe–Heitler process, the ‘Generator’, via high-energy photons from Bremsstrahlung radiation of laser wakefield accelerated electrons interacting with high materials. After a proper collection and focusing system, muons are boosted by another laser wakefield, the ‘Booster’.
    (a) The bubble’s electron density and (b) electrostatic field in the simulation box were obtained from a two-dimensional particle-in-cell simulation code Opic2D for a plasma density. The laser pulse of wavelength, normalized peak amplitude, pulse duration 33 fs and FWHM spot sizeentered from the left of the simulation box in thedirection. A muon with critical trapping energy entered into the simulation box following the trajectory shown in (c) and the energy increasing process in (d).
    Fig. 2. (a) The bubble’s electron density and (b) electrostatic field in the simulation box were obtained from a two-dimensional particle-in-cell simulation code Opic2D for a plasma density . The laser pulse of wavelength , normalized peak amplitude , pulse duration 33 fs and FWHM spot size entered from the left of the simulation box in the direction. A muon with critical trapping energy entered into the simulation box following the trajectory shown in (c) and the energy increasing process in (d).
    (a) The estimated acceleration energy of muonsdepending on the initial energywith different positions in the rest frame of bubblefrom the one-dimensional analytical model denoted by the solid lines. Clearly trapping energy thresholds presented from the sharp peaks of the lines. The two-dimensional PIC simulations of the forward (red dots) and backward (blue dots) muons atshow well agreement with the one-dimensional estimation. (b) The inner plot shows the spectra of the forward (red lines) and backward (blue lines) muons, where dashed lines denote the initialized energy spectra and the solid lines denote the acceleration energy spectra at.
    Fig. 3. (a) The estimated acceleration energy of muons depending on the initial energy with different positions in the rest frame of bubble from the one-dimensional analytical model denoted by the solid lines. Clearly trapping energy thresholds presented from the sharp peaks of the lines. The two-dimensional PIC simulations of the forward (red dots) and backward (blue dots) muons at show well agreement with the one-dimensional estimation. (b) The inner plot shows the spectra of the forward (red lines) and backward (blue lines) muons, where dashed lines denote the initialized energy spectra and the solid lines denote the acceleration energy spectra at .
    The snapshots of the acceleration processes of forward (red dots) and backward (blue dots) muons from the two-dimensional PIC simulations in Figure 2at (a)ps, (b) 1.65 ps, (c) 16.5 ps and (d) 33 ps. (e)–(h) Theand (i)–(l)phase spaces of forward (red dots) and backward (blue dots) muons at the four snapshots are also shown, respectively.
    Fig. 4. The snapshots of the acceleration processes of forward (red dots) and backward (blue dots) muons from the two-dimensional PIC simulations in Figure  2 at (a) ps, (b) 1.65 ps, (c) 16.5 ps and (d) 33 ps. (e)–(h) The and (i)–(l) phase spaces of forward (red dots) and backward (blue dots) muons at the four snapshots are also shown, respectively.
    The extrapolated relationships of the maximum acceleration energy of muons depending on (a) the bubble’s relativistic factorand (b) the relevant trapping energy thresholdfrom the one-dimensional analytic model. The extrapolation of electrons (open circles) in the same parameters is also shown for comparison.
    Fig. 5. The extrapolated relationships of the maximum acceleration energy of muons depending on (a) the bubble’s relativistic factor and (b) the relevant trapping energy threshold from the one-dimensional analytic model. The extrapolation of electrons (open circles) in the same parameters is also shown for comparison.
    F. Zhang, Z. G. Deng, L. Q. Shan, Z. M. Zhang, B. Bi, D. X. Liu, W. W. Wang, Z. Q. Yuan, C. Tian, S. Q. Yang, B. Zhang, Y. Q. Gu. All-optical acceleration in the laser wakefield[J]. High Power Laser Science and Engineering, 2018, 6(4): 04000e63
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