Title: Status of Headon BeamBeam Compensation
1Status of Head-on Beam-Beam Compensation
US LHC Accelerator Research Program
BNL - FNAL- LBNL - SLAC
A. Valishev, FNAL 09 April 2009 LARP CM12
2E-Lens in FY09 LARP Beam-Beam Task
The Goal Evaluate the possible benefit to LHC
(RHIC) luminosity from HO beam-beam compensation.
- Experimental studies at the Tevatron
- Installation of the Gaussian profile gun is
planned - Will allow to experiment with beam to beam
alignment tolerances - Possibly attempt tune footprint suppression
- Identify operational problems
- Provide data for comparison with simulations
- Theoretical analysis
- Effect of dispersion and chromaticity on RDTs,
finite e-beam rigidity - Numerical simulations
- Develop and validate codes/machine models using
existing experimental data - Provide predictions for RHIC and LHC to support
E-Lens installation
3Beam-Beam Simulation Mini WorkshopBNL 12/3/2008
- 11 participants, 13 presentations
- Workshop Goals
- Identify beam-beam related issues in LHC and RHIC
that could be mitigated using e-lenses. - Assess the group capabilities and establish means
of collaboration. - Establish near and long term simulation program,
set priorities and schedule. - We addressed a list of about ten questions. Full
report is available at - http//larpdocs.fnal.gov/LARP-public/DocDB/ShowDoc
ument?docid907 - Near term plan code benchmarking on a number of
excercises for RHIC and LHC - Long term plan study robustness of beam-beam
compensation schemes
4Beam-Beam Simulation Mini WorkshopE-Lens Physics
Questions
- Beam-Beam effects in Tevatron and RHIC
- Combination of HO and LR is important (TEV)
- Separation above 6s must be maintained (TEV)
- Chromatic effects are very important (TEV, RHIC)
- Nonlinearities of final focus triplets
significantly influence dynamics (RHIC) - Working point near 3Qx requires resonance
suppression (RHIC) - Head-on compensation in RHIC
- Strength of beam-beam effects depends on choice
of parameters - Benefits of E-Lens have to be evaluated
- Expectation for Beam-Beam effects in LHC
- LPA upgrade scenario Np 5x1011, hence HO
beam-beam effect - LR collisions will make situation worse
- E-Lens may be used to mitigate HO effect
5Available Computing Tools
- Short-term simulations
- BBSIM (T. Sen, H.-J. Kim, FNAL)
- SixTrack (N. Abreu, Y. Luo, BNL)
- Long-term (weak-strong macro particle simulation
codes) - BBSIM (T. Sen, H.-J. Kim, FNAL)
- LIFETRAC (A. Valishev, FNAL)
- PlibB (A. Kabel, SLAC)
- SixTrack (Y. Luo, G. Robert-Demolaize, BNL)
Heimdall cluster 16x4 cpu
NERSC (?)
BOINC -gt BlueGene, NERSC
6Beam-beam compensation parameter scan
Y. Luo, BNLSixTrack
7Head-on Beam-Beam Compensation in RHICBBSIM
Results (H.-J. Kim, FNAL)
- SEFT Electron Lens
- Flat top edge is 4sigma
- Small Ne reduces beam loss much
- Gaussian Electron Lens
- Same beam size as IP10's
- Small Ne reduces beam loss
- Ne lt 0.5 Nip Np
Is this a tune effect?
NO BBC
- 1x bbc beam-beam compensation with Ne Nip
Np 22E11
8Head-on Beam-Beam Compensation in RHICLifetrac
Results (A. Valishev, FNAL)
9Head-on Beam-Beam Compensation in RHICBBSIM vs.
Lifetrac (H.-J. Kim, A. Valishev, FNAL)
- Model differences
- Initial distribution
- BBSIM hollow Gaussian
- Lifetrac weighted Gaussian
- Aperture
- Lattice chromaticity (sextupoles)
- Model similarities
- Machine optics
- Includes multipoles
- Beam parameters
- 3D beam-beam
NO BBC
1/2 BBC
10Head-on Beam-Beam Compensation in LHCPlibB vs.
Lifetrac (A. Kabel/SLAC, A. Valishev/FNAL)
Lifetrac
PlibB
11Recent TEL-2 ExperienceV. Kamerdzhiev, A.
Valishev (FNAL)
5155, Dec 2006, 2.5E32
- TEL-2 was installed in 2006
- By then, adverse beam-beam effects shifted to
protons! - Specifically, bunch 12 in the train had
considerably higher losses due to lower vertical
tune - In 2008 after improvements in the machine optics
bunch 12 is no longer different at luminosities
up to 3.3E32 - Requested several high initial luminosity stores
- Started preparations to test Gaussian gun
6598, Nov 2008, 3.3E32
12Recent TEL-2 Experience V. Kamerdzhiev, A.
Valishev (FNAL)
Nov 22 2008, 3.3E32 With intentional tune changes
Dec 6, 2008, 3.5E32 No intentional tune changes
Valuable experience gained with e- and p beam
alignment, timing, operation at high luminosity
with SEFT gun.
13Experiment with Gaussian Gun at Tevatron(A.
Valishev, A. Romanov, FNAL)
The new gun was trained and emission
characteristic was measured together with the
beam profile. Still awaiting an opportunity to
install into TEL-2, at least 12 hour tunnel
access is required
14TEL-2 Solenoid Field Profile
15Gaussian TEL-2 Head-on Tune Spread (A. Valishev,
A. Romanov, FNAL)
Changes in beam shape (right) and tune spectra
(left) due to imperfection of guiding solenoidal
field.
16Possibility of Head-on Compensation with SEFT(A.
Valishev, A. Romanov, Fermilab)
Changes in beam shape (right) and tune spectra
(left) due to imperfection of guiding solenoidal
field. It is feasible to generate noticeable tune
spread with the existing gun. Experiment is in
progress.
17Summary
- Reasonable agreement have been achieved between 3
simulation groups for RHIC beam-beam
compensation. A more rigorous comparison is in
progress - Adverse beam-beam effects are observed for RHIC
upgrade parameters - Extent of EL beam-beam compensation is sensitive
to the choice of e- and p beam parameters - Two codes have been configured to run the same
LHC case - Beam-beam induced losses are more pronounced than
in the RHIC case better opportunities for
compensation - Gaussian gun could not be installed in TEL-2
(restricted access time) - Calculations show that SEFT gun can generate
sizeable tune spread attempt to demonstrate
this will be made during remaining Tevatron run
in FY09