Design of a symmetry in-flight separator optics for medium heavy-ion beams Hwang Ji-Gwang, Noh Seon-Yeong, Kim Eun-San Accelerator Physics Laboratory, Kyungpook National University Hatanaka Kichiji Research Center for Nuclear Physics, Osaka University 1
13
Embed
Design of a symmetry in-flight separator optics for medium ...webbuild.knu.ac.kr/~accelerator/ppt/2010_kps_heavy.pdf · 경북대가속기물리연구실 (~15 명: 대학원생, 박사연구원,
This document is posted to help you gain knowledge. Please leave a comment to let me know what you think about it! Share it to your friends and learn new things together.
Transcript
Design of a symmetry in-flight separator optics for medium
heavy-ion beamsHwang Ji-Gwang, Noh Seon-Yeong, Kim Eun-San
Accelerator Physics Laboratory, Kyungpook National University
Hatanaka Kichiji
Research Center for Nuclear Physics, Osaka University
Past-R&D (국내 가속기)- 10 GeV FEL 설계 참여 (포항가속기)- 3 GeV 저장링 설계 참여(포항가속기)- 등등
Layout & feature of in-flight separator
Maximum rigidity: 9 Tm
Energy acceptance: ±4%
Angular acceptance : θ= ± 20 mrad
Φ= ± 35 mrad
Energy degrader : Uniform thickness
Energy dispersion: 1.5448 m
Mass dispersion: -0.90818 m
E/ΔE (x0=2.36 mm): 180
(d/R=0.5; without energy straggling)
A/ΔA (x0=2.36 mm): 128
(d/R=0.5; without energy straggling)
Path length : 24.183m
Beryllium Target
TripletAluminum Degrader
Focal point-1
Sector
Primary beam( 12C6+, 430MeV)
9Li3+
200MeV/u
Degrader optimization in LISE++
5
IPPIr WIPWPWICombined PIIP )(10log10
Slit
Slit
Beam separation using by LISE++
6
Beam separation at the F1
Beam separation at the F2
Yield of the 9Li at the F2 has 400 times larger than yield of 8Li.
Yield of 9Li: 4.58 X 106 pps (=0.732 ppA)(when the primary beam 12C has 50 pnA)
Transmission rate : 7.32%
Beam profile at the exit of separator
7
9Li 8Li8He
The high order effect by magnets
• The transfer matrix of degrader, bending magnet and quadrupole has higher order terms.
where Rij,Tijk , Uijkl is the first, second, third order transfer matrix of each element, respectively.
• The 2nd and 3rd order effect could be corrected by sextupole and octupole, respectively.
j jk jkl
lkjijklkjijkjiji XXXUXXTXRX 0000001
Up to 2nd order effect in beam separator
9
The effect of the 2nd order aberration could be compensate by slit at the F1.
The 2nd order effect of magnets and degrader cause the beam size growth at the F2.
Sllit
Up to 3rd order effect in beam separator
10
Focusing problem(→Large beam size)
Sllit
s [mm]
Correction of the high order effect
11
Beryllium Target
Triplet
Aluminum DegraderFocal point-1
Sector
Primary beam( 12C6+, 430MeV)
Focusing was improved
Feature of designed beam line
Beryllium Target (9.9cm)
12C6+ (430MeV/u)
9Li3+, 200MeV/u
Primary beam: 12C6+ (430MeV/u)Secondary beam: 9Li3+ (200MeV/u)Energy acceptance: ±4%Angular acceptance : ± 20 mrad, ± 35 mradEnergy degrader : Uniform thickness (d/R=0.53)Energy dispersion: 1.5448 m Mass dispersion: -0.90818 mE/ΔE (x0=2.36mm): 180(d/R=0.5; without energy straggling)A/ΔA (x0=2.36mm): 128(d/R=0.5; without energy straggling)Path length : 24.183m
Summary
• We perform the beam separation simulation on the in-flight separator for Gi-Jang Heavy-ion accelerator.
• The optimum wedge thickness was selected.
• In-flight separator has 40mrad of horizontal angular acceptance, 70mrad of vertical angular acceptance, 8% of energy acceptance with d/R=0.53 aluminum homogeneous degrader.
• The high order effect in the in-flight separator was investigated and corrected by three sextupole.(The focusing at the F2 was improved)