Design study of CEPC Alternating Magnetic Field Booster

Design study of CEPC Alternating Magnetic Field Booster Tianjian Bian Jie Gao Michael Koratzinos (CERN) Chuang Zhang Xiaohao Cui Sha bai Dou Wang Yiwei Wang Feng Su

Wiggling Bend Scheme n Introduction of Wiggling Bend Scheme Ø The inject energy is 6 Ge. V. Ø If all the dipoles have the same sign, 33 Gs@6 Ge. V may cause problem. Ø In wiggling bend scheme, adjoining dipoles have different sign to avoid the low field problem. Ø Shorten the Damping times greatly. Ø The picture below shows the FODO structure.

Linear Optics

Linac Parameters n Linac parameters Ø From : Li Xiaoping, Pei Guoxi, etc, "Conceptual Design of CEPC Linac and Source". Parameter Symbol Unit Value E- beam energy Ee- Ge. V 6 E+ beam energy Ee+ Ge. V 6 Repetition rate frep Hz 50 E- bunch population Ne- 2× 1010 E+ bunch population Ne+ 2× 1010 Energy spread (E+/E-) σE <1× 10 -3 Emitance (E-) 0. 3 mm mrad Emitance (E+) 0. 3 mm mrad

Booster Parameters n Contrast With the Alternating Magnetic Field Scheme. Ø Main difference in parameters caused by wiggling bend scheme. Old@6 Ge. V New@6 Ge. V U 0 [Me. V/turn] 0. 019 0. 70 Damping times(x/y) [s] 115. 61 3. 12 Emittances(x) [pi nm] 0. 015 0. 11 Strength of dipole [Gs] 33 -164. 3/+229. 9 Beam offset in dipole[cm] 0 2. 3 Length of dipole [m] 19. 6*1 4. 9*4 Length of FODO [m] 47. 2 Parameter

Booster Parameters n Parameter List for Alternating Magnetic Field Scheme. Parameter Unit Value Beam energy [E] Ge. V 6 Circumference [C] km Revolutionfrequency[f 0] Unit Value RF voltage [Vrf] GV 0. 213867 54. 3744 RF frequency [frf] GHz 1. 3 k. Hz 5. 5135 Harmonic number [h] SR power / beam [P] MW 6. 41 E-04 Synchrotronoscillationtune[ns] Beam off-set in bend cm 2. 30 E+00 Energy acceptance RF [h] 2. 70 E-05 SR loss / turn [U 0] Momentum compaction factor[α] Bending radius [r] m n. B/beam 50 Lorentz factor [g] 11742. 9 Magnetic rigidity [Br] T·m 20. 01 Beam current / beam [I] m. A 0. 9197 Bunchpopulation[Ne] Bunch charge [Qb] emittance-horizontal[ex] inequilibrium 2. 08 E+10 n. C 3. 34 m·rad 1. 11 E-10 injected from linac m·rad 3. 00 E-07 emittance-vertical[ey] inequilibrium m·rad 1. 11 E-12 injected from linac m·rad 3. 00 E-07 Parameter 235800 0. 190183 % 5. 95053 Ge. V 6. 97 E-04 Energyspread[sd] inequilibrium % 0. 01610 injected from linac % 0. 1 Bunch length[sd] inequilibrium mm 0. 05 injected from linac mm ~1. 5 Transversedampingtime[tx] ms 3124. 6 turns 17228 ms 1. 6 turns 9 Longitudinaldampingtime[te]

Booster Parameters n Parameter List for Alternating Magnetic Field Scheme. Angle of dipole v. s. time Field of dipole v. s. time

Booster Parameters n Parameter List for Alternating Magnetic Field Scheme. U 0 v. s. time η v. s. time

Booster Parameters n Parameter List for Alternating Magnetic Field Scheme. Vrf v. s. time Phase v. s. time

Nonlinear Optimization and Sextupole Scheme n Challenges we face Ø It is a big ring. Nonlinear optimization for big ring is much harder than small ring. Ø SSRF booster(only 180 meters) is also made up with FODO structure. SSRF booster's dynamic apture@injection is 11 sigma in horizontal and 42 sigma in vertical without any sextupole optimization[]. Ø Without sextupole optimization, What we have is: 3. 6 sigma in horizontal and 1. 7 sigma in vertical. Ø We have long straight section that we can correct the chromaticity locally. Ø In FODO structure, we can not place harmonic sextupoles easily as DBA structure do. Ø No released code for the sextupole optimization.

Nonlinear Optimization and Sextupole Scheme n Optimization algorithm Ø There are so many sextupoles in the booster. So, the tune shift effect is serious, Ø In the paper[], tune shift with amplitude is derived. We can see that it is related to the sextupole strength, beta function, working point, etc. Ø We choose three value as our goal function, and genetic algorithm is used in the optimization process.

Nonlinear Optimization and Sextupole Scheme n Step 1: Divide sextupoles into diferent families. Ø See three FODOs as a cell, and there are six sextupoles in a cell as the picture below. Ø We have 320 cells in the whole ring. Every cell use the same sextupoles. So there are six sextupole famliies in total. Ø The most important task for sextupole is to correct the linear chromaticity and this is the constraint condition. Ø In this step, minimize the goal function is not important, the most important task is choosing the direction of tune shift.

Nonlinear Optimization and Sextupole Scheme n Step 2: Fake harmonic sextupole Ø It is difficult to add harmonic sextupole in a cell, because there is no zero dispersion point. Ø We arrange SH 1, SH 2, SH 3, SH 4, SH 5, SH 6 as fake harmonic sextupole, use zero chromaticity contribution as their constraint condition. And this is why we call them fake harmonic sextupoles. Ø Smaller goal function values do not means bigger DA, plot DA in the process of optimization and choose the best result.

Nonlinear Optimization and Sextupole Scheme n Tune shift optimization results Ø The working opint is not good. Ø Direction of tune shift

Nonlinear Optimization and Sextupole Scheme n Change working point Ø Working point effects the DA greatly.

Nonlinear Optimization and Sextupole Scheme n First order tune shift optimization is suitable for CEPC? Ø Plot tune shift as a function of Jx. CEPC FODO HEPS DBA

Nonlinear Optimization and Sextupole Scheme n My understanding Ø Why second order tune shift play an important role? Ø First order tune shift in CEPC: Ø Second order tune shift in HEPS:

Conclusion n The low field problem is solved by the wiggling bend scheme. Strength of dipole increase from 33 Gs to -164. 3/+229. 9 Gs. n A ramping method of is alternating magnetic field booster proposed. n Shorter damping times are obtained, which is 3. 12 seconds. n DA is still a problem. The "second order tune shift" idea is proposed and waiting to try and carefully thought.

Thanks for your attention!