ares cavity system for superkekb - pasj · from 1998 through 2010, ares cavities had been...

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ARES CAVITY SYSTEM FOR SuperKEKB Tatsuya Kageyama # , Tetsuo Abe, Hiroshi Sakai, Yasunao Takeuchi, Kazuo Yoshino High Energy Accelerator Research Organization (KEK) 1-1 Oho, Tsukuba-shi Ibaraki-ken, 305-0801 Abstract The ARES cavity is a normal-conducting, three-cavity system developed for KEKB. The acronym “ARES” stands for Accelerator Resonantly coupled with Energy Storage, just representing its RF configuration based on the π/2-mode operation, where an accelerating cavity is resonantly coupled with an energy storage cavity via a coupling cavity between. The energy storage cavity functions as “an electromagnetic flywheel” to stabilize the accelerating mode against the reaction from a high current beam. From 1998 through 2010, ARES cavities had been successfully operated in KEKB (from 2005 through 2010, 32 ARES cavities in total, 20 ARESs at the 3.5-GeV positron ring LER, and 12 ARESs at the 8-GeV electron ring HER). To push the luminosity frontier, the SuperKEKB project has been launched. Its innovative machine design employing the “nanobeam” scheme has led us to the conclusion that the current ARES cavity system can be reused neither upgrading the cavity structure itself nor even its HOM loads. Only the input coupler needs to be upgraded since the beam power per cavity will increase from 200 kW to 600 kW. First, we report key issues on the operation of ARES cavities in SuperKEKB: the coupled-bunch instabilities due to the accelerating (π/2) and parasitic (0 and π) modes. Next, we cover the experimental results for the power handling capabilities of two different types of HOM loads used for the current ARES cavity. Finally, we describe a prototype input coupler and its performance demonstrated through the actual operation with a high-current beam in KEKB. -K4エ・キ KEKB ' SuperKEKB t 1. äiáâ]+)メヒ,mソ U KEKB )d$JD= 39.NBLM9.-,l(%;=@OE ヌヤルkdーィf* S)TIM2!ラリ~IM2[ 0D85M4pセオァqキノ[CO5pt @OEeキ,}マSn@OEリヲ a|%ワv、nホ349E|@OE 7/M>OWニ^。ムスS) Pfw![0D85M4リ~モユ ュラリ~6MAM2IM2トVム& '*)gツャヘ(メ%"クã SuperKEKB j#ハレy,ッ ウ!TIM2Zワv、nホエ・キ| R テNナロコ,W 'zu) 2. -K4エ・キ!nホエ・リア{0<J1Oネ シエ・コsエ・,Xhンョコs*Qエ ・キ) xá-K4エ・キフタx,イ ゥチPoカ`Qミ~キG:J,xâ イ-K4エ・! KEKB }リヲ@OE ,nホ)&ユュ* ケョ! KEKB 3.5-GeV ラリ~IM2(LER)âàr8-GeV リ~IM2(HER) áârツãâr_ォ* KEKB ワv、nホキg\「゙ 2005 Y ヨ゚メヒ?HFO5゙サb゚,イ ____________________________________________ # [email protected] xáå-K4エ・ギã」cフタx゚ xâåカ`Qミ~G:J Proceedings of the 8th Annual Meeting of Particle Accelerator Society of Japan (August 1-3, 2011, Tsukuba, Japan) - 1245 -

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ARES CAVITY SYSTEM FOR SuperKEKB

Tatsuya Kageyama #, Tetsuo Abe, Hiroshi Sakai, Yasunao Takeuchi, Kazuo Yoshino

High Energy Accelerator Research Organization (KEK)

1-1 Oho, Tsukuba-shi Ibaraki-ken, 305-0801

Abstract The ARES cavity is a normal-conducting, three-cavity system developed for KEKB. The acronym “ARES” stands for Accelerator Resonantly coupled with Energy Storage, just representing its RF configuration based on the π/2-mode operation, where an accelerating cavity is resonantly coupled with an energy storage cavity via a coupling cavity between. The energy storage cavity functions as “an electromagnetic flywheel” to stabilize the accelerating mode against the reaction from a high current beam. From 1998 through 2010, ARES cavities had been successfully operated in KEKB (from 2005 through 2010, 32 ARES cavities in total, 20 ARESs at the 3.5-GeV positron ring LER, and 12 ARESs at the 8-GeV electron ring HER). To push the luminosity frontier, the SuperKEKB project has been launched. Its innovative machine design employing the “nanobeam” scheme has led us to the conclusion that the current ARES cavity system can be reused neither upgrading the cavity structure itself nor even its HOM loads. Only the input coupler needs to be upgraded since the beam power per cavity will increase from 200 kW to 600 kW. First, we report key issues on the operation of ARES cavities in SuperKEKB: the coupled-bunch instabilities due to the accelerating (π/2) and parasitic (0 and π) modes. Next, we cover the experimental results for the power handling capabilities of two different types of HOM loads used for the current ARES cavity. Finally, we describe a prototype input coupler and its performance demonstrated through the actual operation with a high-current beam in KEKB.

KEKB SuperKEKB

1.

KEKB

SuperKEKB

2.

KEKB

KEKB 3.5-GeV (LER) 8-GeV(HER)

KEKB 2005

____________________________________________ # [email protected]

Proceedings of the 8th Annual Meeting of Particle Accelerator Society of Japan (August 1-3, 2011, Tsukuba, Japan)

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1.1m 1.2m

US / UA

TE013

/

UA/(UA+US) = 1/10

fRF 508.887 MHz

US / UA 9

R / Q 15

Q0 1.1 105

Vc 0.5 MV

Pc 150 kW ( 60kW 90kW)

/

0

/

0

0

0

3. SuperKEKB SuperKEKB

2010 11

SuperKEKBHER 8 GeV 7 GeV LER 3.5 GeV

4 GeVSuperKEKB

KEKB

KEKB HER 1.6

HER

LER 2.7

KEKB1 MW

SuperKEKB

SuperKEKB LER HER

D4D5 D7 D8

D7 D8D5 HER

LER D4

Proceedings of the 8th Annual Meeting of Particle Accelerator Society of Japan (August 1-3, 2011, Tsukuba, Japan)

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. SuperKEKB SuperKEKB

KEKB

SuperKEKB

KEKB

4.1

RFdetuning

frev

-1 mode

/2

frev = 99.4 kHz

KEKB LER 1.8 A20 1 0.4

MV 3SuperKEKB LER 3.6 A

22 1 0.48 MV5

fA170 kHz 280 kHz

US/UA = 9 / f /2

SuperKEKB LER

22 ms -1

mode 3.6 A4 ms

RF

4. 2 0

/20

100

0

Proceedings of the 8th Annual Meeting of Particle Accelerator Society of Japan (August 1-3, 2011, Tsukuba, Japan)

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0 0

KEKB LER (1.8 A)70 ms

21 ms KEKB 0

SuperKEKB LER (3.6 A) 21 ms 22 ms

RFby

4. 3

ARES(HOM) ARES

HOM

HOM

HOM

† calorimetric measurement

(KEKB) (SuperKEKB)1.25 GHz

HOM SuperKEKB KEKB

5.0 kW 3.3 kW

2008

WR650

1.2 kW2008

RF

KEKB

SuperKEKB

Ibeam (LER) 1.6 A 3.6 A -

Nbunch 1293 2503 -

σz 7 mm 6 mm -

k / ARES 0.40 (0.39 †) V/pC 0.44 V/pC -

PHOM / ARES 5.4 kW † 17 kW -

PHOM / 1.05 kW † 3.3 kW 5.0 kW

PHOM / 0.3 kW † 0.93 kW 1.2 kW

1.25 GHz

VSWR

Proceedings of the 8th Annual Meeting of Particle Accelerator Society of Japan (August 1-3, 2011, Tsukuba, Japan)

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1.5 kW

2010

1.2 kWSuperKEKB LER (3.6 A) 0.93 kW

30%

4. 4

SuperKEKB

SuperKEKB 750 kW150 kW 550~600 kW

KEKB 160~250 kW

3 6

KEKB32 2

43 mm 8

Q TE013

Q

800 kW600 kW

KEKB D5

D5-CHER 6.4

BELLE

KEKB0.47 MV 133 kW

1250 mA610 kW

5.

[1] Y. Yamazaki and T. Kageyama, Particle Accelerators 44

(1994), p. 107. [2] T. Kageyama et al., Proc. of the Particle Accelerator

Conference, Vancouver, Canada, 1997, p. 2902. [3] K. Akai et al., PASJ8-MOPL02, 2011. [4] T. Kageyama, “Grooved beam pipe for damping dipole

modes in RF cavities,” KEK-PREPRINT-91-133, 1991. [5] Y. Takeuchi et al., Proc. of the Particle Accelerator

Conference, Vancouver, Canada, 1997, p.2986. [6] F. Naito et al., Proc. of the Asian Particle Accelerator

Conference, Tsukuba, Japan, 1998, p. 776. [7] T. Abe et al., EPAC-2006-TUPCH127. [8] K. Yoshino et al., PASJ7-THPS036, 2010. [9] H. Sakai et al., PAC-2005-TPPT012. [10] T. Abe et al., PASJ8-TUPS131, 2011.

770 kW

Proceedings of the 8th Annual Meeting of Particle Accelerator Society of Japan (August 1-3, 2011, Tsukuba, Japan)

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