Muon acceleration - amplitude effects in non-scaling FFAG - - PowerPoint PPT Presentation

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Muon acceleration - amplitude effects in non-scaling FFAG -

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Possible cures (higher harmonics) Second harmonics makes dp/p around 1% up to 50 pi mm. ... Possible cures (summary) ... 2 or more cures (partially done). etc. ... – PowerPoint PPT presentation

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Title: Muon acceleration - amplitude effects in non-scaling FFAG -


1
Muon acceleration- amplitude effects in
non-scaling FFAG -
  • Shinji Machida
  • CCLRC/RAL/ASTeC
  • 26 April, 2006
  • http//hadron.kek.jp/machida/doc/nufact/
  • ffag/machida_20060426.ppt pdf

2
Contents
  • Code benchmarking
  • Possible cures of amplitude problem
  • Matching between two FFAG rings
  • Next steps

3
Code benchmark (1)
  • Zgoubi and S(hinjis)-code had discrepancy (?)
  • Initial distributions were different.
  • Zgoubi assumed 6-D ellipsoid. S-code assumed 2-D
    ellipse independently in horizontal, vertical,
    and longitudinal space.

Zgoubi
S-code
(5 to 10 GeV 30 p mm in transverse, 0.05 eVs in
longitudinal.)
4
Code benchmark (2)
  • With the same initial condition independent in
    each plane.
  • Large amplitude particles make a problem also on
    Zgoubi.
  • Another confirmation of the problem by Keil with
    MAD.

Zgoubi
S-code
(10 to 20 GeV 30 p mm in transverse, 0.05 eVs in
longitudinal.)
5
Code benchmark (3)
Some particles are not accelerated.
No correlation Jllta, Jhlta, and Jvlta
Correlation in T only Jllta and JhJvlta
Correlation in L and T JlJhJvlta
Correlation between transverse and longitudinal
space eliminates large amplitude particles in
both planes.
(10 to 20 GeV 30 p mm in transverse, 0.05 eVs in
longitudinal.)
a is amplitude in normalized phase space.
6
Code benchmark (4)
  • In real life, there will be some correlation
    between horizontal and vertical, but probably
    independent of longitudinal.
  • The best way is to take particle distribution at
    the end of linac or RLA. Use it as an initial
    distribution to FFAG.

7
Possible cures (1)
  • Longitudinal dynamics is parameterized by

Relative energy gain per phase slip.
RF frequency relative to revolution freq.
Amplitude effects
0
25
36 p mm
dp/p (normalized)
Left figure is slightly different for finite
amplitude particle.
Phase (1/2 pi)
8
Possible cures (2)
  • Cure 1
  • Increase V to increase a.
  • Cure 2
  • Decrease w to increase a.
  • Cure 3
  • Flatten crest by introduction of higher harmonics.

9
Possible cures (RF voltage)
e0 pi, V1 dp/p0.36
e30 pi, V1 dp/p2.8
5
e30 pi
Dp/p_rms
e30 pi, V1.4 dp/p0.88
0
1
2
V/V_nominal
10
Possible cures (RF voltage)
  • 50 increase of RF voltage makes dp/p around 1
    up to 50 pi mm.

11
Possible cures (higher harmonics)
e0 pi, h1 dp/p0.36
e0 pi, h12 dp/p0.42
e30 pi, h12 dp/p0.58
e30 pi, h13 dp/p0.77
12
Possible cures (higher harmonics)
  • Second harmonics makes dp/p around 1 up to 50 pi
    mm.
  • It requires more RF power because second
    harmonics reduce peak voltage 25.

13
Possible cures (lower frequency)
274 MHz e30 pi, V1 dp/p2.8
88 MHz e30 pi, V2x88/200 dp/p1.2
44 MHz e30 pi, V2x44/200 dp/p1.4
2 MHz e30 pi, V4x2/200 dp/p3.7
14
Possible cures (lower frequency)
  • Lower frequency helps.
  • However, it requires relatively higher voltage
    and time to complete acceleration.

15
Possible cures (summary)
  • Increase of a few 10 of RF voltage or second
    harmonics makes dp/p around 1 up to 50 pi mm
    beam.
  • That requires additional RF power.
  • Amplitude effects can be cured when there is only
    one FFAG.

16
Matching between two FFAG rings (1)
  • Zero transverse emittance beam has no problem of
    longitudinal matching.

dp/p_rms
longitudinal phase space
3
20GeV
2
1
10GeV
0
5GeV
  • 10 20
  • GeV

17
Matching between two FFAG rings (2)
e30 pi, h1, V1
e30 pi, h12, V1.1
  • Second harmonics and 10 increase of RF voltage
    partially cure the problem.
  • It depends decay ring acceptance if it is allowed.

18
Matching between two FFAG rings (3)
  • Still many parameters we can play with.
  • Injection phase of the second ring (partially
    done).
  • Optical parameters of the first ring at injection
    (partially done).
  • Combination of 2 or more cures (partially done).
  • etc.
  • Need criterion how much dp/p is tolerable.

19
Next steps
  • Scaling FFAG with higher RF frequency
  • Does 44 MHz, 88 MHz makes a reasonable bucket in
    scaling FFAG ?
  • How high is the k-value supposed to be if the
    frequency is fixed at 200 MHz ? (Berg)
  • k1800 (my number), 1100 (mori) vs. 800 (present
    lattice)
  • How much dp/p can be allowed in the decay ring?
  • Need a target value for optimization.
  • RLA may have as much dp/p as FFAG with amplitude
    effects a few percent ?
  • dp/p of scaling FFAG with either low and high
    frequency is unknown.
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