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Electron-cloud instability in the CLIC damping ring for positrons H. Bartosik, G. Iadarola, Y. Papaphilippou, G. Rumolo TWIICE workshop, 16.01.2014 TWIICE workshop, H. Bartosik 16.01.2014

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Introduction o Electron cloud can lead to coherent beam instability (see talk of G. Rumolo) Coupled bunch instability feedback Single bunch instability emittance growth faster than radiation damping, feedback difficult due to bandwidth (see talk of K. Li) o Single bunch electron cloud instability depends on electron density optics (beta functions) synchrotron tune chromaticity transverse emittance bunch length o Here: study of single bunch instability for superconducting wigglers 1TWIICE workshop, H. Bartosik 16.01.2014 … needs to be studied in detail

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CLIC damping rings DescriptionSymbolValue Beam energyE 0 [GeV]2.86 Normalized transverse equilibrium emittancesε n,x,y [nm]500, 5 Average beta and dispersion functions (Wigglers)b x,y, D x [m]4.2, 9.8, 2.6 x 10 -5 Bunch length (rms)σ z [mm]1.6 Synchrotron tuneQsQs 6.5 x 10 -3 2TWIICE workshop, H. Bartosik 16.01.2014 Wigglers occupy ~ ¼ of the total ring… C = 427.5 m, L wigglers = 104 m See talk of F. Antoniou 2 options: 0.5 ns or 1 ns bunch spacing Q x =48.38 Q y =10.39

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Electron cloud simulations 3TWIICE workshop, H. Bartosik 16.01.2014 Multi-bunch beam s Primary and secondary electron production, chamber properties E-cloud build up x y Equations of motion of the beam particles Noise

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Electron cloud simulations: splitting the problem 4TWIICE workshop, H. Bartosik 16.01.2014 Multi-bunch beam One turn s Primary and secondary electron production, chamber properties E-cloud build up x y The build up problem Equations of motion of the beam particles Noise The instability problem Single bunch Several turns e.g. with PyECLOUD see talk of G. Iadarola used here: HEADTAIL code

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The HEADTAIL code: simulation principle 5TWIICE workshop, H. Bartosik 16.01.2014

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The HEADTAIL code: simulation principle 6TWIICE workshop, H. Bartosik 16.01.2014

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The HEADTAIL code: simulation principle 7TWIICE workshop, H. Bartosik 16.01.2014 →The effect of the electron cloud on the beam becomes visible only after many turns →The electron cloud is refreshed at every interaction point →Slicing is renewed at every turn

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Instability threshold for e-cloud in wigglers o Simulations with uniform electron density o Electrons in magnetic dipole field ( no horizontal motion in HEADTAIL) No (single bunch) instability in horizontal plane 8TWIICE workshop, H. Bartosik 16.01.2014 Horizontal centroid motionVertical centroid motion

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Instability threshold for e-cloud in wigglers o Simulations with uniform electron density o Electrons in magnetic dipole field ( no horizontal motion in HEADTAIL) No (single bunch) instability in horizontal plane Strong growth of vertical emittance (ε n,y ) above threshold 9TWIICE workshop, H. Bartosik 16.01.2014 rise time τ ≈ 0.7 ms τ ≈ 0.5 ms τ ≈ 0.4 ms ⇒ fast growth compared to vertical damping time (2 ms) ⇒ local electron densities of 1.2 x 10 13 m -3 in wigglers (25% of circumference) drive beam unstable Vertical emittance

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Dependence on bunch intensity o Simulations with uniform electron distributions o Weak dependence of instability threshold on bunch intensity Studied in view of future optimization of CLIC parameters 10TWIICE workshop, H. Bartosik 16.01.2014 ⇒ Similar threshold electron density for the studied range of positron bunch intensities … nominal CLIC intensity Threshold electron density in wigglers

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Using electron distributions from PyECLOUD o PyECLOUD simulation for generation of macroparticle distribution 1 ns bunch spacing 11TWIICE workshop, H. Bartosik 16.01.2014 ⇒ Using distribution (just before bunch passage) with maximum central density = most critical for instability max. central density See talk of G. Iadarola SEY = 1.5

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Using electron distributions from PyECLOUD o PyECLOUD simulation for generation of macroparticle distribution 1 ns bunch spacing Generation of uniform spatial distribution with variable charges/weights 12TWIICE workshop, H. Bartosik 16.01.2014 Histogram Electron distribution beam (±3σ) SEY = 1.5 (bunch 350)

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Using electron distributions from PyECLOUD o PyECLOUD simulation for generation of macroparticle distribution 1 ns bunch spacing Generation of uniform spatial distribution with variable charges/weights o HEADTAIL simulations with distributions from PyECLOUD Bunch passages with maximum central density along the train 13TWIICE workshop, H. Bartosik 16.01.2014 Vertical emittanceMaximum central density along train ⇒ Beam unstable as soon as electron build-up saturated

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Mitigation with chromaticity? o Increasing vertical chromaticity is one of the measures against e-cloud instability o Simulation for uniform e-cloud distribution ρ e = 4 x 10 13 / m 3 (equivalent to ρ e = 1.6 x 10 14 / m 3 in the wigglers) 14TWIICE workshop, H. Bartosik 16.01.2014 ⇒ Even very high chromaticity not sufficient for beam stability (+ incoherent effects) Vertical emittance

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Summary and conclusions o Electron cloud instability simulations with HEADTAIL Decoupled from build-up simulations (computing power) Semi-self consistent by using electron distribution from build-up code Only single bunch instability o Simulations for wigglers with uniform e - distribution Threshold density in wigglers ≈ 1.2 x 10 13 / m 3 Emittance growth rate fast compared to damping times Little dependence on bunch intensity Mitigation by chromaticity not sufficient o Simulations for wigglers using distribution from PyECLOUD Beam is unstable for all SEY values above build-up threshold (i.e. SEY>1.4) Need to suppress e-cloud build-up! 15TWIICE workshop, H. Bartosik 16.01.2014

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G. Rumolo, G. Iadarola, H. Bartosik, G. Arduini for CMAC#6, 16 August 2012 Many thanks to: V. Baglin, G. Bregliozzi, S. Claudet, O. Dominguez, J. Esteban-

G. Rumolo, G. Iadarola, H. Bartosik, G. Arduini for CMAC#6, 16 August 2012 Many thanks to: V. Baglin, G. Bregliozzi, S. Claudet, O. Dominguez, J. Esteban-

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