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45 th ICFA Beam Dynamic Workshop June 8–12, 2009, Cornell University, Ithaca New York Preliminary Results on the Introduction of the Rediffused SEY Component in ECLOUD Jim Crittenden Cornell Laboratory for Accelerator-Based Sciences and Education Electron Cloud Simulations Meeting 2 September 2009

Preliminary Results on the Introduction of the Rediffused SEY Component in ECLOUD

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Jim Crittenden Cornell Laboratory for Accelerator-Based Sciences and Education Electron Cloud Simulations Meeting 2 September 2009. Preliminary Results on the Introduction of the Rediffused SEY Component in ECLOUD. Problems with ECLOUD tune shift calculation for long bunch trains. - PowerPoint PPT Presentation

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Page 1: Preliminary Results on the Introduction of  the Rediffused SEY Component in ECLOUD

45th ICFA Beam Dynamic WorkshopJune 8–12, 2009, Cornell University, Ithaca New York

Preliminary Results on the Introduction of

the Rediffused SEY Component in ECLOUD

Jim Crittenden

Cornell Laboratory for Accelerator-Based Sciences and EducationElectron Cloud Simulations Meeting

2 September 2009

Page 2: Preliminary Results on the Introduction of  the Rediffused SEY Component in ECLOUD

23 September 2009 Preliminary Results from the Introduction of the Rediffused SEY Component in ECLOUD / J.A.Crittenden 2/6

See also slides presented on 22 April 2009

in preparation for PAC 2009and the followup on

20 May 2009

Figure 3 of Studies of the Effects of Electron Cloud Formation at CESRTAPAC 2009

J.A.Crittenden, J.Calvey, G.Dugan, D. L.Kreinick, J. A.Livezey, M.A.Palmer, D.L.Rubin (Cornell), K.C.Harkay (ANL), R.L.Holtzapple (CalPoly), K.Ohmi (KEK),

M.Furman, G.Penn, M.Venturini (LBNL), M.T.F. Pivi, L.Wang (SLAC)

Problems with ECLOUD tune shift calculation

for long bunch trains

Page 3: Preliminary Results on the Introduction of  the Rediffused SEY Component in ECLOUD

23 September 2009 Preliminary Results from the Introduction of the Rediffused SEY Component in ECLOUD / J.A.Crittenden 3/6

Relative Drift and Dipole Contributions

Fluctuations set in for late bunches in long trains in dipole regions.Frank suggested testing numerical approximations.

Time step size, field calculation frequency – no help (see 20 May).Problem resolved by increasing number and reducing charge of macroparticles (see 2 Sep).

Page 4: Preliminary Results on the Introduction of  the Rediffused SEY Component in ECLOUD

23 September 2009 Preliminary Results from the Introduction of the Rediffused SEY Component in ECLOUD / J.A.Crittenden 4/6

Replacement for figure 3following resolution of the fluctuation problem

Next step: Does POSINST exhibit a similar problem if the rediffused component is removed?

Page 5: Preliminary Results on the Introduction of  the Rediffused SEY Component in ECLOUD

23 September 2009 Preliminary Results from the Introduction of the Rediffused SEY Component in ECLOUD / J.A.Crittenden 5/6

Compare ECLOUD Result to POSINST with Rediffused SEY Component Removed

YES ! And very precisely. (See D.L.Kreinick talk of 9 Sep)Physics lesson:

Long bunch trains (>20) are sensitive to cloud energy spectrum/SEY curve near E

peak/multipacting

ECLOUD POSINST without rediffused SEY component

Page 6: Preliminary Results on the Introduction of  the Rediffused SEY Component in ECLOUD

23 September 2009 Preliminary Results from the Introduction of the Rediffused SEY Component in ECLOUD / J.A.Crittenden 6/6

Substantial modification of ECLOUD SEY routines finished yesterday. Removed redundant code, etc.

YES ! And very precisely. (See D.L.Kreinick talk of 9 Sep)Physics lesson:

Long bunch trains (>20) are sensitive to cloud energy spectrum/SEY curve near E

peak/multipacting

ECLOUD

Furman & Pivi LBNL-49771

rediffused

= Pred

* (1d0-dexp(-exparg)) * (1.d0+0.26d0*(1-costheta**2))