EMMA MA RF System C. Ohmori and J. S. Berg EMMA MA System * Many - - PowerPoint PPT Presentation

emma ma rf system
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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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SLIDE 1

EMMA MA RF System

  • C. Ohmori and J. S. Berg
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SLIDE 2

FFAG09

EMMA MA System

* Many FFAG applications require slow acceleration

* Linear non-scaling FFAGs cross many resonances

  • Nonlinear resonances
  • Imperfection resonances

* Resonances damage beam more when you cross them slowly

* There is thus a minimum rate at which you can cross resonances

  • May depend on magnitude of errors

* Low-frequency RF to allow slow acceleration

  • EMMA as-is only allows very rapid acceleration
  • Primarily due to high-frequency RF system

* Accelerate rapidly then reduce rate

  • Start with 100 turns to insure success
  • Reduce acceleration rate and study effects

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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SLIDE 3

FFAG09

Parameters of MA system

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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SLIDE 4

FFAG09

EMMA MA CAVITY

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SLIDE 5

FFAG09

Technical Issues to solve

  • Need high impedance to get > 33 kV/cavity

High impedance MA cores

  • Resonant frequency at 18 MHz

Cut core cavity

  • High voltage in a small space

Space around beam pipe to avoid discharge

Ceramic gap to stand high voltage of > 1.6 kV/mm

  • High power amplifier and power supply

Compact AMP and PS for low duty

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SLIDE 6

FFAG09

Cavity Impedance

 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

be obtained and/or system will be compact.

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SLIDE 7

FFAG09

Improvements of cavity impedance

  • We are interested in higher

impedance core for J-PARC beam-power upgrade.

  • A new material (FT3L, 13µm

thickness) has two times higher impedance than

  • rdinary Magnetic Alloy

(FT3M, 18 µm) .

  • So far, up to 10 cm core was
  • available. Now, up to 27 cm

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

  • frequency. Gap voltage will be twice higher if amplifier has enough

power.

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SLIDE 8

FFAG09

Improvement of cavity impedance

4 MA cores using a new material is produced (27 cm O.D) for J-PARC R&D.

Impedance measurement, next

  • week. Preliminary results are good

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

  • design. Using high impedance core,

system design will be easy.

FT3L core with 27 cm O.D.

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SLIDE 9

FFAG09

Cut core configuration

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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SLIDE 10

FFAG09

Ceramic Gap

 Length of ceramic gap will be about 2 cm

because cavity length is 10 cm.

 30 (-60) kV will applied on it.  Ordinary ceramic pipe can not stand for 1

kV/mm on surface.

 Need to stand at 1.5 (-3) time higher

voltage.

 A new ceramic made by Kyocera can stand

4 times higher field (4kV/mm). A beam pipe for J-PARC RCS cavity #12 will use it.

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SLIDE 11

FFAG09

Compact amplifier and anode power supply

 Peak RF power is 400 kW

 33.3 kV X 24 A

 To save the system cost,pulse operation of small

vacuum tubes is preferable. Duration is 5.6 µs (100 turns/18 MHz) and repetition rate is small (~1 Hz).

 PRISM amplifier and anode power supply can be used.

 50 kW tetrodes, 4CW50,000, can be used. (150 kW tubes,

4CW150,000, are used for PRISM)

 Specification of APS is much smaller than PRISM.

  • Combination of small DC PS and capacitor bank will reduce cost.

 PRISM amplifier still sufficient for 50 kV

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SLIDE 12

FFAG09

summary

 RF system using MA cavity is designed.  Using a new MA material, FT3L, the system will

be compact and fit all requirements.

 If you need 2 times faster acceleration, PRISM amplifier

and APS will be a suitable system to drive.

 R&D on FT3L and new ceramic are carried on

at J-PARC for upgrade.