EMMA MA RF System
- C. Ohmori and J. S. Berg
EMMA MA RF System C. Ohmori and J. S. Berg EMMA MA System * Many - - PowerPoint PPT Presentation
EMMA MA RF System C. Ohmori and J. S. Berg EMMA MA System * Many FFAG applications require slow acceleration * Linear non-scaling FFAGs cross many resonances - Nonlinear resonances - Imperfection resonances * Resonances damage beam
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* Many FFAG applications require slow acceleration
* Linear non-scaling FFAGs cross many resonances
* Resonances damage beam more when you cross them slowly
* There is thus a minimum rate at which you can cross resonances
* Low-frequency RF to allow slow acceleration
* Accelerate rapidly then reduce rate
10-5
2 4 6
10-4
2 4 6
10-3
2 4 6
10-2
normalized DA [ m rad]
100 80 60 40 20
1 of alignment error [m]
100 Turns 1,000 Turns
(Machida)
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Frequency 18 MHz comments Frequency sweep 3 % Possible up to ~8% Total voltage 100 kV 100 turns / cycle Number of cavities 3 Voltage 33.3 kV / cavity 50 kV to run further off-crest Length of cavity 10 cm Number of cores 2 / cavity Size of core 27 O.D, 10 cm ID, 2.5 cm thickness Cut/un-cut core Cut core Q-value About 11 Cavity impedance 1000 Ω FT3L will be used. Core material FT3M
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High impedance MA cores
Cut core cavity
Space around beam pipe to avoid discharge
Ceramic gap to stand high voltage of > 1.6 kV/mm
Compact AMP and PS for low duty
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Assuming ordinary MA material is used
The cavity will have about 600 Ω at 18 MHz Large O.D/I.D ratio is necessary. If I.D. is 10 cm, O.D. will be about 30 cm. Assuming to use PRISM amplifier to drive
− Rf current of 60 A is available.
About 30 kVp per cavity might be achievable ?
If cavity impedance is high, higher voltage can
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impedance core for J-PARC beam-power upgrade.
thickness) has two times higher impedance than
(FT3M, 18 µm) .
core becomes available.
uQf (磁性体コアの特性) 2 4 6 8 10 12 14 1 2 3 4 5 6 frequency (MHz) uQf (GHz) uQf(FT3L,13um) uQf(FT3L,18um) uQf(FT3M,18um)
∝shunt impedance
More than two times higher impedance is expected at higher
power.
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4 MA cores using a new material is produced (27 cm O.D) for J-PARC R&D.
Impedance measurement, next
as we planned : 500 Ω/core.
Test of immersion and cut core are next step for J-PARC and EMMA.
These cores will be references (or used) for EMMA MA system
system design will be easy.
FT3L core with 27 cm O.D.
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Un-cut core has a larger inductance and the resonant frequency will be low because of floating capacitance in cavity and amplifier.
Cut core configuration is a possible way to reduce the inductance.
High impedance will increase Q-value and it is preferable as it can avoid waveform distortion.
Obtained bandwidth is wide much enough to sweep frequency by 3%.
Floating capacitance About 100 pF Core inductance 0.8 µH Shunt impedance 1000 Ω Q-value About 11 Bandwidth 1.5 MHz
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Length of ceramic gap will be about 2 cm
30 (-60) kV will applied on it. Ordinary ceramic pipe can not stand for 1
Need to stand at 1.5 (-3) time higher
A new ceramic made by Kyocera can stand
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Peak RF power is 400 kW
33.3 kV X 24 A
To save the system cost,pulse operation of small
PRISM amplifier and anode power supply can be used.
50 kW tetrodes, 4CW50,000, can be used. (150 kW tubes,
Specification of APS is much smaller than PRISM.
PRISM amplifier still sufficient for 50 kV
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RF system using MA cavity is designed. Using a new MA material, FT3L, the system will
If you need 2 times faster acceleration, PRISM amplifier
R&D on FT3L and new ceramic are carried on