hard x-ray s-2-e fel simulation for lcls-ii cdr
DESCRIPTION
Hard X-ray S-2-E FEL simulation for LCLS-II CDR. J. Wu In discussion with Y. Ding, P. Emma, Z. H uang, H.-D. Nuhn 02/01/2011. LCLS-II: Ranges for Individual Bunch Operation. Simulation example. (From H-D Nuhn, 10/13/2010). Setup. FEL at 13.5 keV , - PowerPoint PPT PresentationTRANSCRIPT
Hard X-ray S-2-E FEL simulation for LCLS-II CDR
J. WuIn discussion with Y. Ding, P. Emma, Z. Huang,
H.-D. Nuhn 02/01/2011
LCLS-II: Ranges for Individual Bunch Operation
(From H-D Nuhn, 10/13/2010)
Simulation example
Setup
• FEL at 13.5 keV,• Electron Centroid Energy 13.5 GeV; peak
current 3 kA– S2E file down to undulator entrance taken from P.
Emma
• Undulator lw = 3.2 cm; each section is about 4.4 m long with 3.4 m magnetic length; beta-function ~ 20 m
Electron bunch @ undulator entrance
• Current profile (head at right)
Without wakefield
• The S2E input electron distribution function is injected into an ideal undulator without any wakefield effect
FEL power
• Along the undulator: Saturation around 60 m
FEL profile and spectrum
• Along the undulator at 100 m
Energy loss• Along the undulator: entrance (black), 60 m
(red), 120 m (blue), and 150 m (green) – electron bunch head at right
Energy spread• Along the undulator: entrance (black), 60 m
(red), 120 m (blue), and 150 m (green) – electron bunch head at right
Setup
• FEL at 13.5 keV,• Electron Centroid Energy 13.5 GeV; peak
current 3 kA– S2E file down to undulator entrance taken from P.
Emma (No LSC included)
• Undulator lw = 3.2 cm; each section is about 4.4 m long with 3.4 m magnetic length; beta-function ~ 35 m
Electron bunch @ undulator entrance
With resistive-wall wakefield• We assume 5 mm diameter round aluminum
pipe; no surface roughness wake, no geometric wake; head at left
FEL power• Along the undulator: Saturation around 80 m;
with wakefield compensation of 150 keV/m which in reality is a tapering in the undulator
FEL power• Along the undulator: 80 m – electron bunch
head at left
FEL power• Along the undulator: 100 m – electron bunch
head at left
FEL power• Along the undulator: 120 m – electron bunch
head at left
FEL power• Along the undulator: 140 m – electron bunch
head at left
FEL spectrum• At the undulator end: 140 m– electron bunch
head at left
FEL spectrum• The wide spectrum is partially due to the
wakefield induced energy chirp along the electron bunch, head at left