PPT-1D-FEL Without Approximations

m otivation capabilities 1D theory 1Dsolver for waves i mplementation without and with Lorentz transformation e xcitation of waves single particle w ithout self effects one and few particles with self effects. Pawlak’s. Rough Sets. Section 2.4. Properties of Approximations. Proposition 2.2. Proof (1). Proof (2). Proof (3). Proof (4). Proof (5). Proof (6). Proof (7). Proof (8). Proof (9). Proof (10). Proof (11). Local algebraic approximations. Variants on Taylor series. Local-Global approximations. Variants on “fudge factor”. Local algebraic approximations. Linear Taylor series. Intervening variables. Transformed approximation. Sean . Kalsi. on behalf of SLAC MCC operations group, WAO August 8, 2012 . 2. Outline. LCLS FEL WOA 2012. Free Electron Lasers. LCLS Overview. Deliverable X-Ray Parameters. Setting Up the Machine.  . in Various Civilizations. Rachel Barnett.  . BC. Babylon. ∏. = . 3 ⅛ = 3.125. A. B. C. D. E. Egypt. ∏ . = 4(8/9)² = 3.16049…. Problem number 50 . Rhind Papyrus. Insu. Yu. 27 May 2010. ACM Transactions on Applied Perception . (Presented at APGV 2009). Introduction. Can you see difference ? . Traditionally GI (Path tracing, photon mapping, ray-tracing) uses . James . B. Murphy, Director. BES Scientific User Facilities . Division. Status of International Light Sources:. Today and in the Near Future. presented . to the. BESAC . Meeting. 25 July 2013. Light Sources: ERL, . EuPRAXIA. Technical Options. Maria Weikum. 10. th. Steering Committee Meeting 11.06.2018. 2. M. Weikum – 10. th. Steering Committee Meeting 11.06.2018. 1. General Process. Steering Committee discusses and decides on criteria and criteria weighting to assess technical options. Beam. -Laser . M. . Artioli. , G. . Dattoli. , F. . Nguyen. and S. Pagnutti. We. are . trying. to go. Towards. «Bonsai» FEL. Whatever. . we. . do…. oscillators. , SASE…. Get. a fast and . photon-photon collisions. Total cross section . . unp. . of photon-photon scattering in the center-of-mass frame, where photons of equal energy collide, for . unpolarized. photons as a function of . J. Wu. FEL Physics Group. Beam Physics Department. Oct. 26, 2010. Accelerator Research Division Status Meeting. October 26, 2010. ARD Status meeting. jhwu@slac.stanford.edu. J. Wu, FEL Physics Group. Louise Cowie . on behalf of the XARA team at Daresbury. CLARA . S-band linear acceleration up to 250 MeV. Bunch charge 20-250 . pC. High repetition rate up to 400 Hz. Electron bunch lengths 250-850 fs. dzpj(1)dpj dz(A(z;z1)exp(ij)+c:c:)(2)@ @z@ @z1A(z;z1)=(z1)b(z;z1)(3)wherej=(kku)z!tjisthephaseofthejthelec-tronwithrespecttotheparticularponderomotivepotentialwellinwhichitevolvesandpj B.W.J. McNeil. University of Strathclyde. Outline. Unaveraged. simulation codes. Spontaneous Noise & QFEL . Amplifiers. Oscillators. Plasma Accelerator Driven FELs. ?. Not really FELs, but….. Much of the material was supplied by colleagues worldwide . cryomodule. integration. LCWS, Strasbourg, the 26. th. October 2017. ALSYOM a subsidiary of ALCEN Group. X-FEL . cryomodule. integration. X-FEL accelerator. Cryomodule. description. ALSYOM Industrial mission.