Ge 140 kV) Flange-to-flange length 500 cm Flange-to-flange length 500 cm Electron beam energy
Ge 140 kV) Flange-to-flange length 500 cm Flange-to-flange length 500 cm Electron beam energy 7 MeV Electron beam energy 7 MeV Bunch repetitionrate rate 43.four MHz Bunch repetition 43.four MHz Bunch rms transverse size Bunch rms transverse size = 1 mm = 1 mm Deflecting pulse width 92 ns flat-top required to deflect 4 out of 31 bunches in train Deflecting pulse width 92 ns flat-top needed to (715 ns pulsingof 31 bunches in train deflect four out period) Kicker operation per rate 1.four MHz KickerRise and fallper rate operation time 1.four MHz (715 ns pulsing period) 20 ns (ten ns desired) Aperture time 14 mm Rise and fall(gap) 20 ns (10 ns desired) 27.six kW peak energy per channel (55.two kW total) Aperture (gap) 14 mm Essential pulsed energy three.8 kW typical power per channel (7.six kW total) 27.6 kW peak energy per channel (55.two kW total) Expected pulsed energy 3.eight kW average power per channel (7.six kW total) two. Electromagnetic DesignFigure 2 demonstrates two. Electromagnetic Design and style the electromagnetic model of the kicker, utilized for the simulations in CST Microwave Studio. The kicker is formed with two Streptonigrin MedChemExpress parallel electrodes inside a Figure two demonstrates the electromagnetic model of your kicker, utilised for the simulavacuum chamber (7.5 mm pipe matching current JLAB beamline) and four 50 coaxial tions in CST Microwave Studio. The kicker is formed with two parallel electrodes inside a ports, two of which serve as energy inputs and two are terminated with matching 50 vacuum chamber (7.five mm pipe matching existing JLAB beamline) and 4 50 cowater-cooled loads. The style approach was carried out centrally focused around two most important axial ports, two of which serve as energy inputs and two are terminated with matching 50 elements: RF behavior and beam dynamics.Photonics 2021, 8, x FOR PEER Review Photonics 2021, 8, x FOR PEER REVIEW3 of 11 three ofPhotonics 2021, 8,of 11 water-cooled loads. The style procedure was carried out centrally focused around3two water-cooled behavior and beam dynamics. carried out centrally focused about two loads. The design and style course of action was principal aspects: RF major elements: RF behavior and beam dynamics.Figure two. Conceptual design on the stripline traveling wave kicker as a beamline Tasisulam custom synthesis insertion device. Figure two. Conceptual design on the stripline traveling wave kicker as a beamline insertion device. Figure two. Conceptual style of your stripline traveling wave kicker as a beamline insertion device.As a four-port RF device, the kicker must be able to provide matching across a As a four-port RF device, the kicker must be capable to supply matching across a As a four-port RF device, to make sure has to be capable the kind of the 10 ns across bandwidth of at least 000 MHz the kickerno distortion in to provide matching rise anda bandwidth of at least 000 MHz to ensure no distortion inside the type of the 10 ns rise and bandwidth 92 no less than 000 MHz to ensure no distortion within the kind of the 10 ns followfall times of of ns-long rectangular pulses. This requirement transforms in to the rise and fall instances of 92 ns-long rectangular pulses. This requirement transforms into the following fall instances with the stripline, consisting of two parallel electrodes inside a into should reping situation:92 ns-long rectangular pulses. This requirement transformspipe, the followcondition: the stripline, consisting of two parallel electrodes inside a pipe, have to represent ing condition: the stripline, consisting of two parallel electrodes inside a pipe, ought to represent a transmission line with 100 charac.
