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1 Bunch compressors ILC Accelerator School May 20 2006 Eun-San Kim Kyungpook National University Korea.

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Presentation on theme: "1 Bunch compressors ILC Accelerator School May 20 2006 Eun-San Kim Kyungpook National University Korea."— Presentation transcript:

1 1 Bunch compressors ILC Accelerator School May Eun-San Kim Kyungpook National University Korea

2 2 Locations of bunch compressors in ILC 2 nd stage ILC : 1 TeV - extension of main linac - moving of SR and BC 1st stage ILC : 500 GeV BCs locates between e - (e + ) damping rings and main linacs, and make bunch length reduce from 6 mm rms to 0.15 mm rms.

3 3 Why we need bunch compressors  Beams in damping rings has bunch length of 6 mm rms. - Such beams with long bunch length tend to reduce effects of beam instabilities in damping rings. - Thus, beams are compressed after the damping rings.  Main linac and IP in ILC require very short beams: - to prevent large energy spread in the linac due to the curvature of the rf. - to reduce the disruption parameter ( ~  z ) : (ratio of bunch length to strength of mutual focusing between colliding beams)  Thus, bunches between DRs and main linacs are shortened. - Required bunch length in ILC is 0.15 mm rms.

4 4 Main issues in bunch compressors  How can we produce such a beam with short bunch length?  How can we keep low emittance (  x /  y = 8  m / 20nm) and high charge (~3.2 nC) of the e - and e + beams in bunch compression?  How large is the effects of incoherent and coherent synchrotron radiation in bunch compression?

5 5 How to do bunch compression  Beam compression can be achieved : (1) by introducing an energy-position correlation along the bunch with an RF section at zero-crossing of voltage (2) and passing beam through a region where path length is energy dependent : this is generated by bending magnets to create dispersive regions. -z  E/E lower energy trajectory higher energy trajectory center energy trajectory  To compress a bunch longitudinally, trajectory in dispersive region must be shorter for tail of the bunch than it is for the head. Tail (advance) Head (delay)

6 6 Consideration factors in bunch compressor design  The compressor must reduce bunch from damping ring to appropriate size with acceptable emittance growth.  The system may perform a 90 degree longitudinal phase space rotation so that damping ring extracted phase errors do not translate into linac phase errors which can produce large final beam energy deviations.  The system should include tuning elements for corrections.  The compressor should be as short and error tolerant as possible.

7 7 Beam parameters in bunch compressors for ILC  beam energy : 5 GeV  rms initial horizontal emittance : 8  m  rms initial vertical emittance : 20 nm  rms initial bunch length : 6 mm  rms final bunch length : 0.15 mm  compression ratio : 40  rms initial energy spread : 0.15 %  charge / bunch : 3.2 nC (N=2x10 10 )

8 8 Different types of bunch compressor Chicane Double chicane Chicanes as a Wiggler Arc as a FODO-compressor

9 9 Different types of bunch compressor  Chicane : Simplest type with a 4-bending magnets for bunch compression.  Double chicane : Second chicane is weaker to compress higher charge density in order to minimize emittance growth due to synchrotron radiation.  Wiggler type : This type can be used when a large R 56 is required, as in linear collider. It is also possible to locate quadrupole magnets between dipoles where dispersion passes through zero, allowing continuous focusing across the long systems.  Arc type : R 56 can be adjusted by varying betatron phase advance per cell. The systems introduce large beamline geometry and need many well aligned components.

10 10 Path length in chicane  A path length difference for particles with a relative energy deviation  is given by   z  R 56  566  2  U 5666  3 ……  : longitudinal dispersion  : relative energy deviation (=  E/E)  R 56 : linear longitudinal dispersion  (leading term for bunch compression)  T 566 : second - order longitudinal dispersion  U 5666 : third - order longitudinal dispersion

11 11 Longitudinal particle motion in bunch compressor k rf = 2  f rf /c  Longitudinal coordinates z : longitudinal position of a particle with respect to bunch center Positive z means that particle is ahead of reference particle (z=0).  relative energy deviation When a beam passes through a RF cavity on the zero crossing of the voltage (i.e. without acceleration,  rf =   /2 )

12 12 Then,  When reference particle crosses at some  rf, reference energy of the beam is changed from E o to E 1. Initial (E i ) and final (E f ) energies of a given particle are Longitudinal particle motion in bunch compressor

13 13 Longitudinal particle motion in bunch compressor To first order in eV rf /E o << 1, In a linear approximation for RF,

14 14 Longitudinal particle motion in bunch compressor In a wiggler (or chicane), In a linear approximation R 56 >> T 566  , Total transformation For  rf  =  /2, R 66 =1, the transformation matrix is sympletic, which means that longitudinal emittance is a conserved quantitiy.

15 15  Zeuthen Chicane : a benchmark layout used for CSR calculation comparisons at 2002 ICFA beam dynamics workshop A simple case of 4-bending magnet chicane B3B2 B4 B1 LBLB LBLB LcLc  L LL   Bend magnet length : L B = 0.5m Drift length B1-B2 and B3-B4(projected) :  L = 5 m Drift length B2-B3 :  L c = 1 m Bend radius :  = 10.3 m Effective total chicane length : (L T -  L c ) = 12 m Bending angle :  o = 2.77 deg Bunch charge : q = 1nC Momentum compaction : R 56 = -25 mm Electron energy : E = 5 GeV 2 nd order momentum compaction : T 566 = 38 mm Initial bunch length : 0.2 mm Total projected length of chicane : L T = 13 m Final bunch length : 0.02 mm

16 16 If a particle at reference energy is bent by  o, a particle with relative energy error  is bent by  o   Path length from first to final bending magnets is  Relations among R 56, T 566 and U 5666 in Chicane a ab

17 17 By performing a Taylor expansion about  = 0 Difference in path length due to relative energy error is Relations among R 56, T 566 and U 5666 in Chicane For large ,   and   terms may cause non-linear deformations of the phase space during compression.

18 18 Momentum compaction  The momentum compaction R 56 of a chicane made up of rectangular bend magnets is negative (for bunch head at z<0).  The required R 56 is determined from the desired compression, energy spread and rf phase. First-order path length dependence is  From the conservation of longitudinal emittance, final bunch length is

19 19 RF phase angle  Energy-position correlation from an rf section is  In general case that beam passes through RF away zero- crossing of voltage, that is R 66 = 1, there is some damping (or antidamping) of the longitudinal phase space, associated with acceleration (or deceleration).

20 20 Synchrotron Radiation  Incoherent synchrotron radiation (ISR) is the result of individual electrons that randomly emit photons. Radiation power P ~ N (N : number of electrons in a bunch)  Coherent synchrotron radiation (CSR) is produced when a group of electrons collectively emit photons in phase. This can occur when bunch length is shorter than radiation wavelength. Radiation power P ~ N 2  ISR and CSR may increase beam emittance in bunch compressors with shorter bunch length than the damping rings.

21 21 Coherent synchrotron radiation  Opposite to the well known collective effects where the wake-fields produced by head particles act on the particles behind, radiation fields generated at tail overtake the head of the bunch when bunch moves along a curved trajectory.  CSR longitudinal wake function is r R R=L o /  zz Coherent radiation for r >  z Overtaking length : L o  (24  z R 2 ) 1/3 LoLo

22 22 Coherent synchrotron radiation  CSR-induced relative energy spread per dipole for a Gaussian bunch is  This is valid for a dipole magnet where radiation shielding of a conducting vacuum chamber is not significant, that is, for a full vacuum chamber height h which satisfies h  (  z √R) 2/3  h c.  Typically the value of h required to shield CSR effects (to cutoff low frequency components of the radiated field) is too small to allow an adequate beam aperture (for R  2.5 m, h « 10 mm will shield a 190  m bunch.)  With very small apertures, resistive wakefields can also generate emittance dilution.

23 23 Incoherent Synchrotron Radiation The increase in energy spread is given by:  Transverse emittance growth is  Beam energy loss is  Increase of energy spread is C q =3.84x m H  x  '   x  '  x   When an electron emits a photon of energy u, the change in the betatron action is given by

24 24 Bunch compressors for ILC  Two-stages of bunch compression were adopted to achieve σ z = 0.15 mm.  Compared to single-stage BC, two-stage system provides reduced emittance growth.  The two-stage BC is used : (1) to limit the maximum energy spread in the beam (2) to get large transverse tolerances (3) to reduce coherent synchrotron radiation that is produced

25 25 Designed types of bunch compressors for ILC  A wiggler type that has a wiggler section made up of 12 periods each with 8 bending magnets and 2 quadrupoles at each zero crossing of the dispersion function : baseline design (SLAC)  A chicane type that produces necessary momentum compaction with a chicane made of 4 bending magnets : alternative design (E.-S. Kim)

26 26 Baseline design for ILC BC A wiggler based on a chicane between each pair of quadrupoles Each chicane contains 8 bend magnets (12 chicanes total).

27 27 Baseline design for ILC BC BC1 RF BC1 Wiggler BC2 RF BC1 Wiggler

28 28  First stage BC - contains 24 9-cell RF cavities arranged in 3 cryomodules. - Because the bunch is long, relatively strong focusing is used to limit emittance growth from transverse wakefields.  Second stage BC - contains cell RF cavities arranged in 57 cryomodules. - A wiggler has optics identical to the wiggler in the first BC, but with weaker wiggler. Baseline design for ILC BC

29 29 Parameters of baseline design Initial Energy Spread [%]0.15 Initial Bunch Length [mm] Initial Emittance [  m] / 0.02 BC1 Voltage [MV]253 BC1 Phase [°]-100 BC1 R 56 [mm]-750 End BC1 Bunch Length [mm]1.14 End BC1 Energy [GeV]4.96 End BC1 Energy Spread [%]0.82 BC2 Voltage [MV]12,750 BC2 Phase [°]-58 BC2 R 56 [mm]-41 End BC2 Bunch Length [mm] End BC2 Emittance [  m] / 0.02 End BC2 Energy [GeV]11.7 End BC2 Energy Spread [%]2.73

30 30 Chicane 1Chicane 2 RF section MatchingQuadrupoles  Main linac Alternative design for ILC BC

31 31 Initial Energy Spread [%]0.15 Initial Bunch Length [mm] Initial Emittance [  m] / 0.02 BC1 Voltage [MV]348 BC1 Phase [°]-114 BC1 R 56 [mm] End BC1 Bunch Length [mm]1.1 End BC1 Energy [GeV]4.86 End BC1 Energy Spread [%]1.1 BC2 Voltage [MV]11,800 BC2 Phase [°]-45 BC2 R 56 [mm]-50.8 End BC2 Bunch Length [mm] End BC2 Emittance [  m] / 0.02 End BC2 Energy [GeV]13.26 End BC2 Energy Spread [%]2.2 Parameters of alternative design

32 32 Alternative Baseline Required bunch length achieved System length shorter longer Tolerence of emittance acceptable comparable acceptable comparable GDE Requirement correction of vertical dispersion shorten system length Alternative Baseline Chicane length 68.4 m 480 m Matching 4 m 310 m Number of RF cavity Total length 680 m 1400 m Bunch compressors for ILC

33 33 Summary  Compared to single-stage BC, two-stage BC system provides reduced emittance growth at σ z = 0.15 mm.  Two stage system can be tuned to ease transverse tolerances.  Two stage system is longer than one-stage system. –A shorter 2-stage may be also possible.

34 34 Problems  Show that emittance growth and increase of energy spread due to incoherent synchrotron radiation are given by 1) 2)


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