rf kicker for head-on-collision

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AccLabBmSc i ICR KyotoUn ivers ity RF Kicker for Head-on-Collision Y. Iwashita Accelerator Laboratory, Advanced Research Center of Beam Science, Institute for Chemical Research, Kyoto University, Gokanosho, Uji, Kyoto 611-0011, JAPAN [email protected] http://wwwal.kuicr.kyoto-u.ac.jp

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RF Kicker for Head-on-Collision. Y. Iwashita Accelerator Laboratory, Advanced Research Center of Beam Science, Institute for Chemical Research, Kyoto University, Gokanosho, Uji, Kyoto 611-0011, JAPAN [email protected] http://wwwal.kuicr.kyoto-u.ac.jp. - PowerPoint PPT Presentation

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AccLab BmSci ICRKyotoUniversity

RF Kicker for Head-on-Collision

Y. IwashitaAccelerator Laboratory,

Advanced Research Center of Beam Science, Institute for Chemical Research, Kyoto University,

Gokanosho, Uji, Kyoto 611-0011, [email protected]

http://wwwal.kuicr.kyoto-u.ac.jp

AccLab BmSci ICRKyotoUniversity

Time Structure of Beam

e+

e–t=0

IP300ns ~ 100m

LRF = 25m

t=τ0/4

- -Out bunch at the Center of In bunch

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ǙDZÇÃÉsÉNÉ`ÉÉÇ å©ÇÈÇΩÇflÇ…ÇÕïKóvÇ≈Ç∑ÅB

AccLab BmSci ICRKyotoUniversity

Magnetic Field Strength

B = ~1 T.km @ 250GeV =L(4m)/(1mrad)=4kmB=0.25T

θ~1m rad

ρL=4m

AccLab BmSci ICRKyotoUniversity

Sketch of a Kicker

L=4m

Double C-typeBetter shieldingStep at center?

Variant

Stored Energy W ~ 125[J] @0.25T3cm x133 units

DC+3MHz (+9MHz)

AccLab BmSci ICRKyotoUniversity

Magnetic Alloy (Finemet)

Q <1 for non-cut coreQ~10 for cut core @a few mm gap

Large Test Core for JPARC

AccLab BmSci ICRKyotoUniversity

High B, low core loss

AccLab BmSci ICRKyotoUniversity

FT-3L

High B, low core loss, high Tc

AccLab BmSci ICRKyotoUniversity

Core Loss

FT-3L is the best option here.

AccLab BmSci ICRKyotoUniversity

Waveforms-1

1 2 3 4

-1

-0.5

0.5

1DC + 3MHz

25m

1 2 3 4

-1

-0.5

0.5

1 DC+3MHz+H1ê4L6MHz25m

1 2 3 4

-1

-0.5

0.5

13MHz + 6MHz

25m

Single RF needs DC

Wide Baseneeds DC

Two RF in One

No DCNarrow Base

Two RF in One

Two RF in One: Two cosine components superposition

AccLab BmSci ICRKyotoUniversity

Waveforms-2

1 2 3 4

-1

-0.5

0.5

13MHz+H1ê2L6MHz

25ê3m

1 2 3 4

-1

-0.5

0.5

13MHz+H1ê3L9MHz

12.5 m

No DCSeparate RF

Short LRF

Two RF

No DCSeparate RF

6MHz too(if 2 sides OK)

Short LRF

Two RF

Separate RF: Each component for each separate kicker

AccLab BmSci ICRKyotoUniversity

Combination

3MHz

9MHz

3MHz

•Separate two RF system for the latter two options.

•Phase slip for in-bunch can be compensated by phasing. ––> less perturbation

AccLab BmSci ICRKyotoUniversity

Comments•MA has been used for RF accelerating cavity to generate high voltage(V==BS). –> Not for generation of B. ( R&D! )•The number units 133 reduces a serious hazard. (133 cores, 133 Amp’s)

•Upgradable to 1TeV(6MHz) –– Two sets?

•Easier than Crab-cavity