Introduction to Synchrotron Radiation Techniques and Applications

2023 4 17 n.w
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Discover the birth of the Synchrotron Ultraviolet Radiation Facility (SURF I) and its significance in catering to regular users of synchrotron radiation. Explore the Fokker-Planck account of damping and diffusion from incoherent emission of synchrotron radiation, along with insights on CSR-induced bunch instability. Dive into the world of synchrotron radiation with this informative presentation.

  • Synchrotron Radiation
  • SURF I
  • Fokker-Planck
  • Bunch Instabilities
  • Radiation Techniques

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  1. 2023-4-17

  2. J=1.35 0.0891, 0.0089, 0.0044, 0.0022

  3. J= 1.35 1.632.03 0.0022

  4. J=1.352.714.068.00

  5. J kR=1 m=1 30 0.0036 40 0.0037 50 0.0037 60 0.0037 100 0.0037 kR=1 m=2 30 0.0021 40 0.0022 50 0.0022 60 0.0022 100 0.0022

  6. Thus was born the Synchrotron Ultraviolet Radiation Facility (SURF I), the first to cater for regular users of synchrotron radiation.(An Introduction to Synchrotron Radiation Techniques and Applications (Philip Willmott) ) The terms on the right hand side give the Fokker-Planck account of damping and diffusion from incoherent emission of synchrotron radiation in quanta. CSR contributes an intense self-field, with wake and precursor components, which is a potential source of bunch instability beyond the effect of the machine wake (Study of Bunch Instabilities by the Nonlinear Vlasov-Fokker-Planck Equation Robert L. Warnock)

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