eexs for bunch compression

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EEXs for Bunch Compression A. Meseck

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EEXs for Bunch Compression. A. Meseck. Motivation: avoid correlated energy deviation Idea:. Electron. beam. metamorphose. EEX1 Exchange Z↔X. EEX2 Exchange X↔Z. Quad focuses X Before EEX2. A. Meseck. Horizontal phase space. Beam energy= 7.5 GeV Horzontal : Norm.emitt =0.3mm mrad - PowerPoint PPT Presentation

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Page 1: EEXs for Bunch Compression

EEXs for Bunch Compression

A. Meseck

Page 2: EEXs for Bunch Compression

Motivation: avoid correlated energy deviation

Idea:

EEX1Exchange Z↔X

EEX2Exchange X↔ZQuad

focuses XBefore EEX2

A. Meseck

Page 3: EEXs for Bunch Compression

Horizontal phase space

Longitudinal phase space

Exch

ange

d

Exch

ange

d

Dipole=>Ldipol=15m, r=90m

L

L L L

L L

L

L

L1 L1

L=20mL1=10m

Quad=>Lquad=0.5mG=2-3T/mLarge Aperture ~ 10cm

Beam energy= 7.5 GeVHorzontal:Norm.emitt=0.3mm mradBetax=30mAlphax=0

Longitudinal:2ps rms pulse duration 2e-4 rms relative energy spread100 pC

~ 280m

Horzontal:Norm.emitt=1.7mm mradBetax=86m+ ISR BUT NO CSRLongitudinal:0.25ps rms pulse duration 1.63e-3 rms relative energy spread100 pC

beam.in

Page 4: EEXs for Bunch Compression

Horizontal phase space

Horzontal:Norm.emitt=0.3mm mradBetax=30mAlphax=0

Horzontal:Norm.emitt=1.7 mm mradDue to ISR! Can not be reduced as there are larger beta-amplitudes involved in the exchange process

Betax=86m (at the end)

X’ [rad]

X [m]

X’ [rad]

X [m]

X’ [rad]

X [m]

BMAD-STANDARD

Page 5: EEXs for Bunch Compression

Longitudinal phase space

Longitudinal:2ps rms pulse duration 2e-4 rms relative energy spread100 pC

Longitudinal:0.25ps rms pulse duration 1.63e-3 rms relative energy spread No way to avoid this!100 pC

σγ/γ

σz [m]

σγ/γ

σz [m]

σγ/γ

σz [m]

BMAD-STANDARD

Page 6: EEXs for Bunch Compression

More realistic phase space distribution+ NO ISRNO CSR

Horzontal:Norm.emitt=0.3mm mradBetax=30mAlphax=0

Longitudinal:2ps rms pulse duration 2e-4 rms relative energy spread100 pC

Horzontal:Norm.emitt=0.3mm mradBetax=24m

+ NO ISR, NO CSRLongitudinal:0.23ps rms pulse duration 1.63e-3 rms relative energy spread100 pC

X’ [rad]

X [m]

X’ [rad]

X [m]

σγ/γ

σz [m]

σγ/γ

σz [m]

Taylor map 1 order

Page 7: EEXs for Bunch Compression

More realistic phase space distribution+ NO ISRNO CSR

Horzontal:Norm.emitt=0.3mm mradBetax=30mAlphax=0

Longitudinal:2ps rms pulse duration 2e-4 rms relative energy spread100 pC

Horzontal:Norm.emitt=0.315mm mradBetax=23m

+ NO ISR + NO CSRLongitudinal:0.25ps rms pulse duration 1.63e-3 rms relative energy spread100 pC

X’ [rad]

X [m]

X’ [rad]

X [m]

σγ/γ

σz [m]

σγ/γ

σz [m]

Taylor map 3 order

Page 8: EEXs for Bunch Compression

More realistic phase space distribution+ ISRNO CSR

Horzontal:Norm.emitt=0.3mm mradBetax=30mAlphax=0

Longitudinal:2ps rms pulse duration 2e-4 rms relative energy spread100 pC

Horzontal:Norm.emitt=1.47mm mradBetax=90m

+ ISR BUT NO CSRLongitudinal:0.25ps rms pulse duration 1.63e-3 rms relative energy spread100 pC

X’ [rad]

X [m]

X’ [rad]

X [m]

σγ/γ

σz [m]

σγ/γ

σz [m]

Taylor map 3 order

Page 9: EEXs for Bunch Compression

More realistic phase space distribution+ NO ISR+CSR

Horzontal:Norm.emitt=0.3mm mradBetax=30mAlphax=0

Longitudinal:2ps rms pulse duration 2e-4 relative energy spread100 pC

Horzontal:Norm.emitt=3.18 mm mradBetax=68m

CSR but no ISRLongitudinal:0.247ps rms pulse duration 1.63e-3 rms relative energy spread100 pC

X’ [rad]

X [m]

X’ [rad]

X [m]

σγ/γ

σz [m]

σγ/γ

σz [m]

Taylor map 3 order

Page 10: EEXs for Bunch Compression

More realistic phase space distributionComparison ISR with CSR

Horzontal:Norm.emitt=0.3mm mradBetax=30mAlphax=0

Longitudinal:2ps rms pulse duration 2e-4 relative energy spread100 pC

σγ/γ

σz [m]

σγ/γ

σz [m]

X’ [rad]

X [m]

X’ [rad]

X [m]

Taylor map 3 order

Page 11: EEXs for Bunch Compression

More realistic phase space distributionISR + CSR

Horzontal:Norm.emitt=0.3mm mradBetax=30mAlphax=0

Longitudinal:2ps rms pulse duration 2e-4 relative energy spread100 pC

Horzontal:Norm.emitt=3.66 mm mradBetax=65m

CSR and ISRLongitudinal:0.247ps rms pulse duration 1.63e-3 relative energy spread100 pC

X’ [rad]

X [m]

X’ [rad]

X [m]

σγ/γ

σz [m]

σγ/γ

σz [m]

Taylor map 3 order

Page 12: EEXs for Bunch Compression

7.5 GeV beam (rf curvature included): norm_emitt _x beta_x rms pulse length rms energy spread

Initial 3.00000000E-07 3.00000000E+01 5.99585000E-04 2.00000000E-04Final-thridorder 3.14928525E-07 2.30628088E+02 7.46578955E-05 1.63872330E-03Final-ISR-noCSR 1.46982166E-06 9.00624160E+01 7.48045872E-05 1.63882406E-03Final-ISR-CSR 3.66210475E-06 6.53924997E+01 7.41145508E-05 1.63599854E-03

1GeV beam (rescaled EEX Compressor ; rf curvature not included, BMAD-STANDARD): norm_emitt _x beta_x rms pulse length rms energy spread

Initial 3.00000000E-07 3.00000000E+01 5.99585000E-04 5.00000000E-05Final-ISR-noCSR 3.07024662E-07 1.42481898E+02 2.93357319E-05 1.03152631E-03Final-ISR-CSR 4.49764204E-06 2.69827366E+01 3.24663673E-05 1.00185760E-03

According to Zholents (PAC2011), there is a chance that an increase in initial betafuction reduces the 2D CSR.