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BiBTeX citation export for WEPP22: Submicropulse Energy-Time Correlations of 40-Mev Electron Beams at Fast

@InProceedings{thurman-keup:ibic2020-wepp22,
  author       = {R.M. Thurman-Keup and A.H. Lumpkin},
  title        = {{Submicropulse Energy-Time Correlations of 40-Mev Electron Beams at Fast}},
  booktitle    = {Proc. IBIC'20},
  pages        = {150--153},
  paper        = {WEPP22},
  language     = {english},
  keywords     = {electron, laser, alignment, optics, instrumentation},
  venue        = {Santos, Brazil},
  series       = {International Beam Instrumentation Conference},
  number       = {9},
  publisher    = {JACoW Publishing, Geneva, Switzerland},
  month        = {10},
  year         = {2020},
  issn         = {2673-5350},
  isbn         = {978-3-95450-222-6},
  doi          = {10.18429/JACoW-IBIC2020-WEPP22},
  url          = {https://www.jacow.org/ibic2020/papers/wepp22.pdf},
  note         = {https://doi.org/10.18429/JACoW-IBIC2020-WEPP22},
  abstract     = {We have recently extended our ability to explore submicropulse effects in relativistic electron beams to energy-time (E-t) correlations. The Fermilab Accelerator Science and Technology (FAST) facility consists of a photoinjector, two superconducting TESLA-type capture cavities, one superconducting ILC-style cryomodule, and a small ring for studying non-linear, integrable beam optics called IOTA. The linac contains, as part of its instrumentation, an optical transport system that directs optical transition radiation (OTR) from an Al-coated Si surface to an externally located streak camera for bunch length measurements. For the first time, an OTR screen after the spectrometer magnet was used for measurements of submicropulse E-t correlations. The projected, micropulse time profile was fit to a single Gaussian peak with σ = 11.5 ± 0.5 ps for 500 pC/micropulse and with a 200-micropulse synchronous sum, in agreement with the upstream bunch-length measurement at a non-energy-dispersive location. The submicropulse E-t images were explored for four rf phases of CC1, and the E vs. t effects will be presented.},
}