SIMULATION FOR TW LCLS-II Tor’s question on the undulator length in the TW FEL senario SASE FEL undulator length 9, 10, and 11: 9 – m, 10 – m, 11 – m FEL energy 8, 13, and 18 keV LCLS-II Undulator: period 3.2 cm, each undulator magnetic section is 3.4 m, and break length is 1 m Electron bunch 4 kA peak current, 0.3 mm-mrad emittance, and 1.3 MeV slice energy spread 13 & 18 keV FEL: electron bunch temporal profile: ideal flattop 8 keV FEL: electron bunch temporal profile: start-to-end FEL and Beam Phys. Dept. (ARD/SLAC), J. Wu,
SIMULATION FOR TW LCLS-II 8 keV FEL through a single crystal 0.1 mm thick C(400) with 1.2E-05 (FWHM) bandwidth The FEL Å FEL and Beam Phys. Dept. (ARD/SLAC), J. Wu, SASESASE S-2-E beam, horns lase strongly
SIMULATION FOR TW LCLS-II 8 keV FEL through a single crystal 0.1 mm thick C(400): 1.2E-05 (FWHM) bandwidth with Bragg angle 57 o The FEL Å FEL and Beam Phys. Dept. (ARD/SLAC), J. Wu, SeedSeed
SIMULATION FOR TW LCLS-II 8 keV FEL through an 1.2E-05 (FWHM) bandwidth The FEL Å FEL and Beam Phys. Dept. (ARD/SLAC), J. Wu, Seeded TW: Taper profile for 5 MW seed
SIMULATION FOR TW LCLS-II SASE FEL in the seed bandwidth: Gamma-distribution FEL and Beam Phys. Dept. (ARD/SLAC), J. Wu, Seeded TW
SIMULATION FOR TW LCLS-II 13 keV FEL through a single crystal 0.1 mm thick C(400) with 1.2E-05 (FWHM) bandwidth The FEL Å FEL and Beam Phys. Dept. (ARD/SLAC), J. Wu, SASESASE
SIMULATION FOR TW LCLS-II 13 keV FEL through a single crystal 0.1 mm thick C(400): 1.2E-05 (FWHM) bandwidth with Bragg angle 32 o The FEL Å FEL and Beam Phys. Dept. (ARD/SLAC), J. Wu, SeedSeed
SIMULATION FOR TW LCLS-II 13 keV FEL through a 1.2E-05 (FWHM) bandwidth The FEL Å FEL and Beam Phys. Dept. (ARD/SLAC), J. Wu, Seeded TW: Taper profile for 1 MW seed
SIMULATION FOR TW LCLS-II SASE FEL in the seed bandwidth: Gamma-distribution FEL and Beam Phys. Dept. (ARD/SLAC), J. Wu, Seeded TW Seeded TW: Taper profile for 1 MW seed
SIMULATION FOR TW LCLS-II 18 keV FEL through a single crystal 0.1 mm thick C(400) with 2.5E-05 (FWHM) bandwidth The FEL Å FEL and Beam Phys. Dept. (ARD/SLAC), J. Wu, SASESASE
SIMULATION FOR TW LCLS-II 18 keV FEL through a single crystal 0.1 mm thick C(400): 2.5E-05 (FWHM) bandwidth with Bragg angle 23 o The FEL Å FEL and Beam Phys. Dept. (ARD/SLAC), J. Wu, SeedSeed Need be improved, but electron beam will determine
Seeded TW: Taper profile for 1 MW seed SIMULATION FOR TW LCLS-II 18 keV FEL through a 2.5E-05 (FWHM) bandwidth The FEL Å FEL and Beam Phys. Dept. (ARD/SLAC), J. Wu,
SIMULATION FOR TW LCLS-II SASE FEL in the seed bandwidth: Gamma-distribution FEL and Beam Phys. Dept. (ARD/SLAC), J. Wu, Seeded TW: Taper profile for 1 MW seed
SIMULATION FOR TW LCLS-II Fundamental 6 keV 3 rd 18 keV (in progress), but let us look at 8 keV case FEL and Beam Phys. Dept. (ARD/SLAC), J. Wu, 8 keV: blue ideal (blue) red ideal 3 rd harmonic (x 30) (red) green start-to-end (green) 8 keV: blue ideal (blue) red ideal 3 rd harmonic (x 30) (red) green start-to-end (green)
SIMULATION FOR TW LCLS-II 8 vs 13, ideal vs s-2-e 8 keV: blue ideal (blue) green start-to-end (green) 13 keV: red ideal (red) 8 keV: blue ideal (blue) green start-to-end (green) 13 keV: red ideal (red) FEL and Beam Phys. Dept. (ARD/SLAC), J. Wu,
SIMULATION FOR TW LCLS-II Summary The next episode: Optimize for 150 m long TW undulator Any optimization on the break length between the undulator sections FEL and Beam Phys. Dept. (ARD/SLAC), J. Wu, FEL power (keV) SASE Undulator Length (m) TW Undulator Length (m) Seed power (MW) 100 m ± rms (TW) 150 m ± rms (TW) 200 m ± rms (TW) ± ± ± ± ± ± ± ± ± 0.022