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OBSERVATION OF COLLECTIVE RESONANCE STOPBANDS IN SIMULATOR FOR PARTICLE ORBIT DYNAMICS S. Ohtsubo, M. Fujioka, H. Higaki, K. Ito, K. Izawa, M. Kuriki, H. Okamoto, K. Tanaka Graduate School of Advanced Sciences of Matter, Hiroshima University 1-3-1 Kagamiyama, Higashi-Hiroshima, 739-8530 Abstract We have designed and constructed a compact non-neutral plasma trap system to study various collective effects in space-charged-dominated particle beams. The tabletop apparatus is called “S-POD (Simulator for Particle Orbit Dynamics)” that consists mainly of a radio-frequency quadrupole trap, several diagnostic systems, a vacuum system, a data-taking computer, and a number of AC and DC power supplies for control of the plasma confinement potential. In the present experimental study, S-POD is employed to demonstrate the existence of linear and nonlinear collective resonance stopbands that depend on various machine parameters. To simulate lattice-dependent effects on the stopbands, we apply periodic perturbations to ion plasmas and confirm the excitation of additional resonances. We also observe the shifts of stopbands caused by the collective space-charge force. ງᏕ◂✪⏕ භ㫾Ꮽᏽᛮ ᐁ㥺Ⓩ◂✪ 㸦㸣ࡋࡢᗀᓞኬᏕ∸⌦◂✪ᐄ1998ࢡࡡ㊂௧ᮮ㸡࡞ࢪࢠᇱ♇◂ ✪ᐁ㥺Ⓩ⌦ㄵⓏᒈ㛜࡞ࡂ㎾ᖳ∸⌦ᏕᡥἪᚺ⏕ࡒࡊ≺⮤ງᏕ ࡞✪◂ງථ㔔ᚨ⣌㎦菜財s饋さ攷事質璽昨⊘y溷寉搾疽 堠搾擦桟a綽載三榆晒⊘曉淊曄㋯崎ヂ耆斎傘財裕滝 ⅲs饋さ攷採皿耆三倁単磔字汐旨治埼HPɔ作2灯 崎催三 [1,2] 腰菜財栽堺咲⊘本」吮単搾事質璽栽1載耜 三ⅲ搾逵嗷Iぅ昨⊘棊壺崎倁澳作晄灯鷺字汐旨治視 汐紙字◦1桟砥堺咲㋯2ɔ作ŠW崎歳三梁勝磔栽催 三腰砦搾o籠作嫗肴歳⊘耄惚昨事質璽堀斟ŠWブ伺 四叱視汐紙字孜施脂璽“S-POD (Simulator for Particle Orbit Dynamics)”スゝ疾└3菜財 [3] S-POD搾嫗鑢 └耆㊌昨⊘玫弄尨嗅臍黻伺四叱視汐紙字∑♂7⊘ f疊滋質式視汐紙字∭⊘豁搾字汐旨治㎦孜施脂 璽⊘Z薛蔗㋯⊘至質獅兵Pブ志叱似耳質獅⊘字汐 旨治磨裁殺寉搾呆癪ブ緑ⅲ饋鷺碕崎催三腰 痛琢崎寃連載三曉淊作砥ブ菜財滋質式視汐紙字鑢 鉄埼字汐旨治㎦吮搾彖撮採鷺噴1嘸桟嘸θ作1載腰 視汐紙字搾亡昨20cm8熾崎⊘侍残汐至質士紙字皐 治伺子鴫私示諮式字識質視(MCP)薩礼殺⊘406 mmZ朿吮作離撮堺咲最三腰本」吮皐事質璽ó4㋯ 埼屛匙三埼⊘が貼ビ昨靖作2菜最搾崎⊘曉淊ɔ作 倫惨剤咲れ鷺三疊o搾視汐紙字桟砥ブ菜咲最三腰諜 嗜搾曉淊崎昨⊘嘸搾伺四叱娌娉崎字汐旨治搾ヂ耆 埼葢Ú桟〒最⊘曉淊娌娉昨仲曉濯砥ブ菜咲最鷺最腰 藐ブ菜財伺四叱ⅲ昨 40 Ar + 崎⊘単磔搾仕式思叱始施桟 饋攷强作鮫晒伺四叱杢菜咲ヂ耆載三腰赭鱗搾伺四 叱磨裁殺昨単徃作U搾Z最財隘饋黻皐師質視嗅 臍黻饋黻作㌹饋嗇桟容本載三砦埼作鮫晒祉耆菜⊘ 砦傘皿搾㌹饋嗇桟肬暘搾獅伺爾叱屍崎四叱四侍菜 咲字汐旨治桟㎦吮搾赭鱗笹昨歳瞥載腰葢Ú伺四叱 豁搾㎦暘鷺皿策作字汐旨治搾贇倧疊o皐赭鱗㎟熾 搾㎦暘鷺碕栽梁勝崎催三腰S-POD 朿載三曉淊 脂質治昨豁惚催三栽⊘痛琢崎昨鎬ǐ曉赳菜財逵嗷錨 螵事質璽鐸晄暘磔搾㎦0霄作榊最咲寃連載三腰 嘸θǖ伺四叱視汐紙字搾齔む嘸 Proceedings of Particle Accelerator Society Meeting 2009, JAEA, Tokai, Naka-gun, Ibaraki, Japan 121

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Page 1: OBSERVATION OF COLLECTIVE RESONANCE STOPBANDS IN … · OBSERVATION OF COLLECTIVE RESONANCE STOPBANDS IN SIMULATOR FOR PARTICLE ORBIT DYNAMICS S. Ohtsubo, M. Fujioka, H. Higaki, K

OBSERVATION OF COLLECTIVE RESONANCE STOPBANDS IN SIMULATOR FOR PARTICLE ORBIT DYNAMICS

S. Ohtsubo, M. Fujioka, H. Higaki, K. Ito, K. Izawa, M. Kuriki, H. Okamoto, K. Tanaka

Graduate School of Advanced Sciences of Matter, Hiroshima University 1-3-1 Kagamiyama, Higashi-Hiroshima, 739-8530

Abstract

We have designed and constructed a compact non-neutral plasma trap system to study various collective effects in space-charged-dominated particle beams. The tabletop apparatus is called “S-POD (Simulator for Particle Orbit Dynamics)” that consists mainly of a radio-frequency quadrupole trap, several diagnostic systems, a vacuum system, a data-taking computer, and a number of AC and DC power supplies for control of the plasma confinement potential. In the present experimental study, S-POD is employed to demonstrate the existence of linear and nonlinear collective resonance stopbands that depend on various machine parameters. To simulate lattice-dependent effects on the stopbands, we apply periodic perturbations to ion plasmas and confirm the excitation of additional resonances. We also observe the shifts of stopbands caused by the collective space-charge force.

1998

[1,2]

“S-POD (Simulator for Particle Orbit Dynamics)” スゝ [3] S-POD

さ々 ゝ

┷㎲ ″

ゝ㍂ 20cm

(MCP) 406 mm┷

40Ar+

㍂㎲ ❻

├├

ゝ㍂

S-POD セ

Proceedings of Particle Accelerator Society Meeting 2009, JAEA, Tokai, Naka-gun, Ibaraki, Japan

121

Page 2: OBSERVATION OF COLLECTIVE RESONANCE STOPBANDS IN … · OBSERVATION OF COLLECTIVE RESONANCE STOPBANDS IN SIMULATOR FOR PARTICLE ORBIT DYNAMICS S. Ohtsubo, M. Fujioka, H. Higaki, K

よSacherer[4] Gluckstern[5]

smooth approximation1 [6]

!

"m

= n / 2 (1)

!

"m

mn

!

"m

[7]

!

"m# m($0 %C

m&$). (2)

!

"0

スゝ

!

"#

!

Cm

1

!

N sp

!

"0#Cm$" % N sp &

n

2m (3)

┘ ㎰ 2Ⅴ

!

m = 2

!

1/ 4

S-POD

[2,3] LabVIEW

12 FODO

3

!

N sp = 3

996 kHz

FODO93 V 0.5

↓3

4 1 249 kHz

1 msec

12FODO 83 kHz83 ┞

3.1

12

!

N sp = 12

!

"0

2.2 3.1 ㎰

ぜ (3)

!

"0#C

m$" % 6n / m

!

"0

3

!

m = 2

!

"0

2

!

m = 3

Proceedings of Particle Accelerator Society Meeting 2009, JAEA, Tokai, Naka-gun, Ibaraki, Japan

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Page 3: OBSERVATION OF COLLECTIVE RESONANCE STOPBANDS IN … · OBSERVATION OF COLLECTIVE RESONANCE STOPBANDS IN SIMULATOR FOR PARTICLE ORBIT DYNAMICS S. Ohtsubo, M. Fujioka, H. Higaki, K

!

N sp = 3

0.5% 1.0% ス

!

N sp = 12 ふ

!

"0

0.8 1.6

!

"0#C

m$" % 3n / 2m

!

m = 2

4

!

m = 4

3.2

!

N sp " (n / 2m)

1 msec ゝ

(3) ↓

3Ⅴ

(3)

!

Cm

!

Cm

m[4,6]

!

C2

0.75

!

Cm

m1 ふ

S-POD々

m

!

N sp / m

!

N sp / 2m

S-POD

1000

CPUさS-POD さ 2 3

S-POD

[1] H. Okamoto and H. Tanaka, Nucl. Instrum. Meth. A 437

(1999) 178. [2] H. Okamoto, Y. Wada, and R. Takai: Nucl. Instrum. Meth.

A 485 (2002) 244. [3] R. Takai, H. Enokizono, K. Ito, Y. Mizuno, K. Okabe, and H.

Okamoto: Jpn. J. Appl. Phys. 45 (2006) 5332. [4] F.J. Sacherer: Ph.D. Thesis, UCRL 18454 (1968). [5] R.L. Gluckstern: Proc. Linac Conf. (Fermilab, Batavia, IL,

1970) p.811. [6] H. Okamoto and K. Yokoya: Nucl. Instrum. Meth. A 482

(2002) 51. [7] R. Baartman: AIP Conf. Proc. No. 448 (AIP, New

York, 1998) p.56.

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