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CSR Benchmark Test-Case Results

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Presentation on theme: "CSR Benchmark Test-Case Results"— Presentation transcript:

1 CSR Benchmark Test-Case Results
Paul Emma SLAC January 14, 2001 BERLIN CSR Workshop

2 Chicane CSR Test-Case Use line-charge CSR    transient model described in LCLS-TN-01-12… (Stupakov/Emma, Dec. 2001) [same now used in Elegant] …based on TESLA-FEL-96-14 (Saldin et al., Nov. 1996) (T566 included, no ISR* added) * incoherent synchrotron radiation

3 Initial Gaussian Distribution Prior to Chicane
perfectly linear correlation sE/E0 = 0.72 %  bunch head ss = 200 mm E0 = 5 GeV

4 Second Order Compression Included: T566
/mm T566  -3R56/2 leads to slight bunch shape distortion after drift-3 before drift-3

5 Beta and Dispersion Functions
‘CSR-altered’ bx ‘linear’ bx hx-max  267 mm ‘linear’ hx

6 Bunch Length and R56 ss0 = 200 mm ss = 20 mm R56 = -25 mm B1 B2 B3 B4

7 Final s-d phase space (gaussian input)
sE/E0 = %  bunch head ss = 20.3 mm

8 Energy Spread and Emittance (gaussian)
B1 B2 B3 B4 E /E0  % sd  0.021% B1 B2 B3 B4 gex  1.52 mm

9 Total RMS Relative Energy Spread (including ‘chirp’)
B1 B2 B3 B4

10 Chicane CSR-wake Movie (gaussian)

11 Chicane CSR-integrated-wake (gaussian)

12 Final x-x Phase Space (gaussian input)
ge  1.52 mm geCSR  mm ge0 = 1.00 mm bopt  1.37 m aopt  -1.10

13 Final x-x Phase Space (gaussian & optimal b0, a0)
emittance growth can be reduced by choosing optimal b-functions ge  1.15 mm geCSR  mm b  bopt a  aopt ge0 = 1.00 mm

14 Beta and emittance (gaussian & optimal b0, a0)
too big? bmin  0.6 m b  bopt a  aopt gex  1.15 mm

15 CSR wakefields (gaussian  bend-1 to drift-2)
L = 0.4 m drift-1 (20) L = 5 m Nbin = 600, smoothed over 4 bend-2 (10) L = 0.4 m drift-2 (10) L = 1 m

16 CSR wakefields (gaussian  bend-3 to drift-4)
L = 0.4 m drift-3 (40) L = 5 m bend-4 (20) L = 0.4 m drift-4 (20) L = 2 m

17 Compressing Uniform Distribution

18 Final s-d phase space – Uniform input dist.
sE/E0 = % ss = 20.2 mm

19 Energy Spread and Emittance (uniform)
E /E0  % sd  0.007% emittance growth reduced compared to gaussian gex  1.12 mm

20 Chicane CSR-wake Movie – Uniform Dist.

21 Chicane CSR-integrated-wake – Uniform Dist.

22 Final x-x Phase Space (uniform input)
ge  1.12 mm geCSR  0.07 mm ge0 = 1.00 mm bopt  3.9 m aopt  -0.51

23 CSR wakefields (uniform  bend-1 to drift-2)
L = 0.4 m drift-1 (20) L = 5 m Nbin = 600, smoothed over 4 bend-2 (10) L = 0.4 m drift-2 (10) L = 1 m

24 CSR wakefields (uniform  bend-3 to drift-4)
L = 0.4 m drift-3 (40) L = 5 m bend-4 (20) L = 0.4 m drift-4 (20) L = 2 m

25 Betatron Amplitude per Bunch Slice
gaussian l(s) uniform l(s)

26 Final s-d phase space - Single-Bend
sE/E0 = % ss = 20.1 mm

27 Energy Spread and Emittance – Single Bend
steady-state bend magnet sd = 0.011% (24ssR2)1/3

28 CSR-Wake Movie - Single-Bend

29 LCLS BC2 CSR-integrated-wake (tracked dist.)


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