% IMPORTANT: The following is UTF-8 encoded.  This means that in the presence
% of non-ASCII characters, it will not work with BibTeX 0.99 or older.
% Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or
% “biber”.

@INPROCEEDINGS{Hansli:191795,
      author       = {Hansli, Matthias and Angelovski, Aleksandar and Jakoby,
                      Rolf and Penirschke, Andreas and Flöttmann, Klaus and
                      Lipka, Dirk and Schlarb, Holger and Vilcins-Czvitkovits,
                      Silke and Grüner, Florian and Zeitler, Benno},
      title        = {{A} {B}eam {A}rrival {T}ime {C}avity for {REGAE} at {DESY}},
      address      = {Geneva},
      publisher    = {JACoW, Geneva, Switzerland},
      reportid     = {PUBDB-2014-03984},
      isbn         = {978-3-95450-132-8},
      series       = {JACoW conferences},
      pages        = {1820-1822},
      year         = {2014},
      comment      = {Proceedings of the 5th Int. Particle Accelerator Conf.,
                      IPAC2014, Dresden, Germany},
      booktitle     = {Proceedings of the 5th Int. Particle
                       Accelerator Conf., IPAC2014, Dresden,
                       Germany},
      abstract     = {REGAE (Relativistic Electron Gun for Atomic Exploration) at
                      DESY in Hamburg is a linear accelerator for electron
                      diffraction experiments. It is upgraded to allow for laser
                      driven wake field accelerator experiments. The bunch length
                      is around 10 fs and the wakefield structure is about 100 fs
                      and the synchronization of the laser and the electron bunch
                      needs to be in order of the bunch length. To achieve this, a
                      RFbased scheme will be used, comparing the phase of a beam
                      induced signal with the reference clock. To improve the
                      performance for the operation with charges well below 1 pC a
                      beam arrival time cavity (BAC) at 3.025 GHz is foreseen as a
                      highly sensitive pickup. To provide the maximum energy to
                      the measurement electronics, the cavity needs a high
                      R=Qvalue and an optimized coupling. An over-coupled setting
                      might be beneficial as it provides a higher signal-to-noise
                      ratio for the first samples. In this paper the concept of
                      the beam arrival time cavity, the influence of the dark
                      current on the measurement and parameter studies and
                      optimization of the cavity itself are presented.},
      month         = {Jun},
      date          = {2014-06-15},
      organization  = {5th International Particle Accelerator
                       Conference, Dresden (Germany), 15 Jun
                       2014 - 20 Jun 2014},
      keywords     = {Accelerator Physics (Other) / 06 Instrumentation, Controls,
                      Feedback $\&$ Operational Aspects (Other) / T24 Timing and
                      Synchronization (Other)},
      cin          = {MDI / MPY / MSK},
      cid          = {I:(DE-H253)MDI-20120806 / I:(DE-H253)MPY-20120731 /
                      I:(DE-H253)MSK-20120731},
      pnm          = {REGAE - Relativistic Electron Gun for Atomic Exploration
                      (POF2-515)},
      pid          = {G:(DE-H253)POF2-REGAE-20130405},
      experiment   = {EXP:(DE-H253)REGAE-20150101},
      typ          = {PUB:(DE-HGF)8 / PUB:(DE-HGF)7},
      doi          = {10.18429/JACoW-IPAC2014-TUPRI104},
      url          = {https://bib-pubdb1.desy.de/record/191795},
}