<p>Based on collisions between the 100 PW laser and 8 GeV superconducting linear accelerator under construction in the Shanghai High Repetition Rate X-ray Free Electron Laser and Extreme Light Facility, the construction of GeV-level <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\gamma\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation>-ray as well as positron beams was proposed according to particle-in-cell simulations. Key processes were considered, involving the nonlinear inverse Compton scattering for <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\gamma\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation>-ray generation and the multiphoton Breit–Wheeler process for electron–positron pair production. Regardless of laser polarization, the simulations indicated that <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\gamma\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation>-ray beams achieved energies up to 8 GeV, brilliance of approximately 10<sup>27</sup> photons/(<InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\textrm{s}\cdot \textrm{mm}^{2}\cdot \textrm{mrad}^{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mtext>s</mtext> <mo>·</mo> <msup> <mtext>mm</mtext> <mn>2</mn> </msup> <mo>·</mo> <msup> <mtext>mrad</mtext> <mn>2</mn> </msup> </mrow> </math></EquationSource> </InlineEquation>), and emittance as low as 0.1 <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\textrm{mm}\cdot \textrm{mrad}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mtext>mm</mtext> <mo>·</mo> <mtext>mrad</mtext> </mrow> </math></EquationSource> </InlineEquation>, whereas positron beams attained energies up to 7 GeV, brilliance of approximately 4 <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\times\)</EquationSource> <EquationSource Format="MATHML"><math> <mo>×</mo> </math></EquationSource> </InlineEquation> 10<sup>24</sup> positrons/(<InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\textrm{s}\cdot \textrm{mm}^{2}\cdot \textrm{mrad}^{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mtext>s</mtext> <mo>·</mo> <msup> <mtext>mm</mtext> <mn>2</mn> </msup> <mo>·</mo> <msup> <mtext>mrad</mtext> <mn>2</mn> </msup> </mrow> </math></EquationSource> </InlineEquation>), and emittance as low as 0.1 <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\textrm{mm}\cdot \textrm{mrad}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mtext>mm</mtext> <mo>·</mo> <mtext>mrad</mtext> </mrow> </math></EquationSource> </InlineEquation>. Various applications could benefit from the possible high-energy <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(\gamma\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation>-ray and positron beams, which may potentially be built in SHINE, including validation of the fundamental physics of strong-field quantum electrodynamics theory, nuclear physics, nuclear astrophysics, and imaging.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

GeV-level γ-ray and positron beams produced by collisions of multi-PW laser on high-energy electron beam

  • Wan-Qing Su,
  • Chun-Wang Ma,
  • Xi-Guang Cao,
  • Guo-Qiang Zhang,
  • Yu-Ting Wang

摘要

Based on collisions between the 100 PW laser and 8 GeV superconducting linear accelerator under construction in the Shanghai High Repetition Rate X-ray Free Electron Laser and Extreme Light Facility, the construction of GeV-level \(\gamma\) γ -ray as well as positron beams was proposed according to particle-in-cell simulations. Key processes were considered, involving the nonlinear inverse Compton scattering for \(\gamma\) γ -ray generation and the multiphoton Breit–Wheeler process for electron–positron pair production. Regardless of laser polarization, the simulations indicated that \(\gamma\) γ -ray beams achieved energies up to 8 GeV, brilliance of approximately 1027 photons/( \(\textrm{s}\cdot \textrm{mm}^{2}\cdot \textrm{mrad}^{2}\) s · mm 2 · mrad 2 ), and emittance as low as 0.1 \(\textrm{mm}\cdot \textrm{mrad}\) mm · mrad , whereas positron beams attained energies up to 7 GeV, brilliance of approximately 4 \(\times\) × 1024 positrons/( \(\textrm{s}\cdot \textrm{mm}^{2}\cdot \textrm{mrad}^{2}\) s · mm 2 · mrad 2 ), and emittance as low as 0.1 \(\textrm{mm}\cdot \textrm{mrad}\) mm · mrad . Various applications could benefit from the possible high-energy \(\gamma\) γ -ray and positron beams, which may potentially be built in SHINE, including validation of the fundamental physics of strong-field quantum electrodynamics theory, nuclear physics, nuclear astrophysics, and imaging.