Multi-Objective Optimization with possible application in SuperKEKB(in progress) Y. Zhang, D. Zhou 16-03-25.

Slides:



Advertisements
Similar presentations
Beam-Beam Optimization for Fcc-ee at High Energies (120, 175 GeV) at High Energies (120, 175 GeV) Dmitry Shatilov BINP, Novosibirsk 11 December 2014, CERN.
Advertisements

Working Group 3 Summary M. Sullivan / Y. Funakoshi.
Topic Three: Perturbations & Nonlinear Dynamics UW Spring 2008 Accelerator Physics J. J. Bisognano 1 Accelerator Physics Topic III Perturbations and Nonlinear.
Yichao Jing 11/11/2010. Outline Introduction Linear lattice design and basic parameters Combined function magnets study and feasibility Nonlinear dynamics.
6. betatron coupling sources: skew quadrupoles, solenoid fields concerns: reduction in dynamic (& effective physical) aperture; increase of intrinsic &
Dynamic Aperture Study for the Ion Ring Lattice Options Min-Huey Wang, Yuri Nosochkov MEIC Collaboration Meeting Fall 2015 Jefferson Lab, Newport News,
1 Dynamic aperture of non-scaling FFAG with sextupole Shinji Machida CCLRC/RAL/ASTeC 21 July, ffag/machida_ ppt.
A U.S. Department of Energy Office of Science Laboratory Operated by The University of Chicago Office of Science U.S. Department of Energy Containing a.
Study and Optimization of Dynamic Aperture for the SuperKEKB LER E.Levichev and P.Piminov, BINP SB RAS, Novosibirsk, Russia.
Nonlinear Dynamic Study of FCC-ee Pavel Piminov, Budker Institute of Nuclear Physics, Novosibirsk, Russia.
1 NICA Collider: status and further steps O.S. Kozlov LHEP, JINR, Dubna for the NICA team Machine Advisory Committee, JINR, Dubna, October 19-20, 2015.
E Levichev -- Dynamic Aperture of the SRFF Storage Ring Frontiers of Short Bunches in Storage Rings INFN-LNF, Frascati, 7-8 Nov 2005 DYNAMIC APERTURE OF.
1 Dynamic aperture studies in e+e- factories with crab waist IR’07, November 9, 2007 E.Levichev Budker Institute of Nuclear Physics, Novosibirsk.
Orbits, Optics and Beam Dynamics in PEP-II Yunhai Cai Beam Physics Department SLAC March 6, 2007 ILC damping ring meeting at Frascati, Italy.
Six-dimensional weak-strong simulations of head-on compensation in RHIC Y. Luo, W. Fischer Brookhaven National Laboratory, USA ICFA Mini-workshop on Beam-Beam.
Lattice design for FCC-ee Bastian Haerer (CERN BE-ABP-LAT, Karlsruhe Institute of Technology (KIT)) 1 8 th Gentner Day, 28 October 2015.
Preliminary Result on L*=1.5m CEPC Interaction Region Yiwei Wang, Dou Wang, Sha Bai Yingshun Zhu, Teng Yue CEPC acc. meeting, 5 September 2014.
CEPC Interaction Region design and Dynamic Aperture Optimization Yiwei Wang, Yuan Zhang, Dou Wang, Huiping Geng, Xiaohao Cui, Sha Bai, Tianjian Bian, Feng.
Application of Differential Evolution Algorithm in Future Circular Colliders Yuan IHEP, Beijing Demin Zhou, KEK, Ibaraki, Japan.
Choice of L* for FCCee: IR optics and DA A.Bogomyagkov, E.Levichev, P.Piminov Budker Institute of Nuclear Physics Novosibirsk HF2014, IHEP Beijing, 9-12.
Dynamic Aperture Studies with Acceleraticum
The Studies of Dynamic Aperture on CEPC
Multi-Turn Extraction studies and PTC
Cui Xiaohao, Zhang Chuang,Bian Tianjian January 12,2016
Summary of CEPC pretzel scheme design
Non-linear Beam Dynamics Studies for JLEIC Electron Collider Ring
CEPC pretzel scheme study
First Look at Nonlinear Dynamics in the Electron Collider Ring
Optics Development for HE-LHC
Optimization of CEPC Dynamic Aperture
Electron collider ring Chromaticity Compensation and dynamic aperture
CEPC Partial Double Ring Lattice Design and DA Study
Updates on IR and FF for super-B factory
SC Overview 2013 White & Rouge The Codes in Comparison The Noise Issue
Dynamic Aperture Optimization in CEPC
The new 7BA design of BAPS
DA study for CEPC Main Ring
DA Study for the CEPC Partial Double Ring Scheme
Progress of SPPC lattice design
Interaction region design for the partial double ring scheme
Comparison of the final focus design
ZHANG, Yuan WANG, Yiwei WANG, Dou GENG, Huiping
CEPC主环lattice及动力学孔径研究
Lattice design for the CEPC collider ring
DA Optimization/ Beam-Beam Tail Wyw170816/0823-bx0.36
SuperB CDR Machine P. Raimondi for the SuperB Team Paris, May 9, 2007.
CEPC 动力学孔径优化 in progress
Design study of CEPC Alternating Magnetic Field Booster
Optimization of partial double ring optics
PEPX-type BAPS Lattice Design and Beam Dynamics Optimization
V12 work needed (some in progress):
M. E. Biagini, LNF-INFN SuperB IRC Meeting Frascati, Nov , 2007
Update on CEPC pretzel scheme design
Lattice design and dynamic aperture optimization for CEPC main ring
Triplet corrector layout and strength specifications
Some Issues on Beam-Beam Interaction & DA at CEPC
Lattice Design of the Collider Ring toward TDR
Progress on DA Optimization with MODE
Yuri Nosochkov Yunhai Cai, Fanglei Lin, Vasiliy Morozov
Progress on Non-linear Beam Dynamic Study
Update on MEIC Nonlinear Dynamics Work
Update on study of chromaticity correction schemes for ion ring
Ion ring lattice with -I sextupole pairs for ir chromaticity correction Y. Nosochkov, M-H. Wang
Update on MEIC Nonlinear Dynamics Work
Chromaticity correction in e-ring with TME cells and –I sextupole pairs in arcs Y. Nosochkov 28 February 2017.
Update on MEIC Nonlinear Dynamics Work
DYNAMIC APERTURE OF JLEIC ELECTRON COLLIDER
100th FCC-ee Optics Design Meeting
Update for ion ring lattice chromaticity correction
CEPC主环lattice及动力学孔径研究
Presentation transcript:

Multi-Objective Optimization with possible application in SuperKEKB(in progress) Y. Zhang, D. Zhou 16-03-25

Introduction This work was firstly excited by Oide’s talk. K. Oide, “A design of beam optics for FCC-ee”, 2015-09 “255 sextupole pairs per half ring” Downhill Simplex is a local optimization algorithm We use a global optimization algorithm: Diffential Evolution (Suggested by Ji Qiang@LBNL) Other popular algorithm: Genetic Algorithm, Particle Swarm

Differential Evolution The “DE community” has been growing since the early DE years of 1994 – 1996 (new) DE is a very simple population based, stochastic function minimizer which is very powerful at the same time. There are a few strategies, we choose ‘rand-to-best’. Attempts a balance between robustness and fast convergence. v i,j = 𝑥 𝑖,𝑗 +𝐹× 𝑥 𝑏,𝑗 −𝑥(𝑖,𝑗) +𝐹× 𝑥 𝑟1,𝑗 −𝑥(𝑟2,𝑗) , 𝐼𝑓 𝑟𝑎𝑛𝑑 𝑗 <𝐶𝑅 𝑥 𝑖,𝑗 , 𝑂𝑡ℎ𝑒𝑟𝑤𝑖𝑠𝑒 Different problems often require different settings for NP, F and CR F is usually (0.5,1) but according to our experience, maybe (0.1~0.5) better

Optimization with Algorithm - Objective function 𝑥 2 20 2 + 𝑧 2 16 2 =1 𝑧 for energy deviation in unit of 𝜎 𝑝 𝑥 for transverse amplitude in unit of 𝜎 For z =Range[-15,15,3], objective function = 0, if aperture boundary is outside the ellipse distance between the boundary and the ellipse, otherwise

The first test, with 240 sextupoles, 100turns V1, 100 turns

CEPC: Dynamic Aperture Optimization with 240 sextupoles in ARC (v1-IR) SF SD

Tune

The multiple objective algorithm based on differential evolution is implemented referencing J. Qiang, IPAC’13. Yongjun Li, IAS Program on HEP Conference, 2016

More Objective in CEPC test DA with PhaseX->0,PhaseY->0 DA with PhaseY->Pi/2, PhaseY->Pi/2 Qx in [0, 0.5] Qy in [0, 0.5] ChromaticityX in [0, 5] ChromaticityY in [0, 5] DA: 𝑥 2 20 2 + 𝑦 2 50 2 + 𝑧 2 16 2 =1, 𝑓𝑜𝑟 𝑧=0 DA: 𝑥 2 20 2 + 𝑦 2 50 2 + 𝑧 2 16 2 =1, 𝑓𝑜𝑟 𝑧=−5 DA: 𝑥 2 20 2 + 𝑦 2 50 2 + 𝑧 2 16 2 =1, 𝑓𝑜𝑟 𝑧=+5

A solution (not good enough, just a test)

We have to suppress the skew sextupole resonance, and enlarge the DA in the mean time This is a multiple objective task.

Objective DA: 𝑥 2 50 2 + 𝑧 2 26 2 =1 with PhaseX->0,PhaseY->0, for z=-26:2:26 DA: 𝑥 2 50 2 + 𝑧 2 26 2 =1 with PhaseX->pi/2,PhaseY->pi/2, for z=-26:2:26 𝑦 𝜎 𝑦 for a particle with initial coordinate (5 𝜎 𝑥 ,0,0,0,0,0) 𝑦− 𝑦 𝜎 𝑦 for a particle with initial coordinate (5 𝜎 𝑥 ,0,0,0,0,0) Coupling Chromaticity: 𝑅 1 𝑅 4 − 𝑅 2 𝑅 3 , for 𝛿=(−0.018,+0.018) To correct the skew sextupole nonlinear terms, the skew sextupole strength symmetry in one pair is broken. Totally we use 24 skew sextupole.

Status of Optimization

It’s evolving, but too slow

How to do next Is it possible to use all sext/oct to enlarge DA Is it possible to use all sext/oct/skew-sext to suppress the resonance driving term, and keep the DA unchanged (or even larger) Is it possible to speed up the optimization We could only track 100 turns to determine DA as in Phase I. 200 turns in Phase II 400 turns in Phase III 1000 turns

DA with Sext DA: 𝑥 2 50 2 + 𝑧 2 26 2 =1 with PhaseX->0,PhaseY->0, for z=-26:2:26 DA: 𝑥 2 50 2 + 𝑧 2 26 2 =1 with PhaseX->pi/2,PhaseY->pi/2, for z=-26:2:26

DA with Sext (100turns)

DA with Sext (200turns)

DA with Sext (400turns & 1000turns)

Try to use all sext/skewsext to enlarge DA and suppress skewsext resonance driving term

Other way to be tried Insert a skew sextupole pair before/after IP, the pair could cancel each other and help compensate the nonlinear resonance at IP. It is like the crab-waist scheme. This may need to change the linear optics. If the DA with suppressed skew sextupole resonance is not good enough, we may need to optimize the sextupole strength further.

Summary DA optimization is a complicated problem DA is not the only objective. Chromaticity, coupling and even nonlinearity should also be well controlled. We have a multiple objective task. The multi-objective optimization has been used in light source machine (not only storage ring based) for a few years SuperKEKB team has developed powerful optimization tool. We wish the Multi-Objective-Differential-Evolution could also help the optimization of SuperKEKB The MODE is just a tool, no physics. Physics exist in the definition of objective function. The tool could only help us find the ‘ceiling’ of a design. But the ‘ceiling’ is determined by the design itself.