PPT-Power Buildup Cavity at 355 nm for

MegaWatt pulse powers PI Mark Notcutt Boulder Precision ElectroOptics 5733 Central Ave Boulder CO Buildup of circulation Power in a cavity Spacing between both laser and cavity modes Equals the repetition rate of the laser 4025 MHz. Binping Xiao. Aug 20 2015. Cavity overview. No coupling slots between cells.. Beam pipe aperture: cell . to . cell & end cell 1.875”. Dimensions (cavity radius, FPC slot height, nose cones . etc. Andy Butterworth, Erk Jensen. Thanks to E. Ciapala, R. Calaga, E. Montesinos, O. Brunner, P. Baudrenghien, S. Claudet, D. Nisbet. 4. th. . TLEP3 Workshop . 05.04.2013. Overview. RF requirements. total accelerating voltage. Preparation of. . crab cavities for KEKB. RF aging of input couplers.. 17. th. September 2009 , LHC-CC09 at CERN. K.Nakanishi. Fabrication Procedure of Crab Cavity. Nb Sheet. Half Cell Hydro-forming. Andy Butterworth (CERN BE/RF). Thanks to . E. . Ciapala, R. Calaga, E. Montesinos, O. Brunner, P. Baudrenghien, S. Claudet. Overview. Introduction and general considerations. A bit of history: the LEP2 RF system. Thanks to E. Ciapala, R. Calaga, E. Montesinos, O. Brunner, P. Baudrenghien, S. Claudet, D. Nisbet. 4. th. . TLEP3 Workshop . 05.04.2013. Overview. RF requirements. total accelerating voltage. beam power. Han Li. On behalf of. FREIA . team. FREIA . Laboratory. , Uppsala . University. May. . . 2017. 1. FREIA . I. nfrastructure. 2. LHe. . cryo. -plant. The bunker. 704 MHz klystron . PPT modulator. RF switchboard, transfer lines, circulators, loads, etc. . Derun Li. Lawrence Berkeley National Laboratory. MICE RF Workshop. Fermilab, June 2, 2014. MICE. MICE RF Workshop, June 2, 2014 (Fermilab), Derun Li, LBNL. Our responsibilities . in . MICE cooling channel:. A. . Guzilov (VDBT), . I. Syratchev (CERN). Recent developments and perspectives. Bunching-Alignment-Collecting (BAC) technology. BAC is technical extension of COM, where the impedances of the cavities triplet allows to reduces dramatically the spatial wavelength of the core oscillations, thus . Dr G Burt. (most slides borrowed from Ben Woolley and . Shok. Karimian). XbFEL. meeting 28. th. July . 2015. Deflecting . Cavities. . Beam. Magnetic field. . horizontal. Electric Field. Deflecting . Rapid . RF Characterization of Superconducting Materials. Paul B. . Welander. , Matt Franzi, Sami Tantawi. SLAC National Accelerator Laboratory, Menlo Park, CA 94025. 28 July 2016. Superconducting RF Materials. Topics for Today. Why Elliptical Shape?. Multi-cells. Couplers. Input power. Higher Order . Mode. Tuners. 3. H. Padamsee. Multipacting. in Nearly Pill-Box Shaped . Cavities. The Folly of Youth!. Early SRF cavity geometries frequently limited by . ee. A. Butterworth, CERN. Thanks to: O. . Brunner, R. . Calaga. , E. Jensen, E. Montesinos, F. Zimmermann (CERN), U. . Wienands. (SLAC). Outline. FCC and the . e. +. e. -. option. FCC-. ee. requirements for operation at different beam energies. Feb. 17, 2014. Modeling Efforts. Design/optimization/evaluation of two designs toward engineering realization: . RF Dipole (RFD) cavity. Double Quarter Wave (DQW) cavity. RFD cavity. HOM coupler design improvement. RFTech. 4. th. Workshop . Status of the RF SYSTEMS . of the Spiral2 accelerator . . Marco Di Giacomo. Linac. RF System coordinator. On behalf of the Accelerator Team. Contents. Quick overview of the .