Top-up injection into the SLS using a sextupole...
Transcript of Top-up injection into the SLS using a sextupole...
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Top-up injection into the SLSusing a sextupole kicker
Group members:Linda Stoel, Salim Ogur, Samira Kasaei, Nikolaos Charitonidis, Claudio
Digiulio, Daniel Barna
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Strategy
● Too many parameters to optimize● Not a single figure-of-merit ● Lack of time and expertise● By coding the formulae and optimizing by computer
we might loose the insight...
1) Find guiding principles...
2) ...to fix as many parameters as possible
3) Leave max. 2 free parameters, create catchy figures
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Best (x,x')This schematics suggests parallel injection.
Might be misleading...
s=0 sk
ss
β
x
x'
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Best (x,x')This schematics suggests parallel injection.
Might be misleading...
s=0 sk
ss
β
x
x'
Goal: minimize the Courant-Snyder invariant (ε) of the motion of the injected beam's center
x ' k=−αk /βk⋅xk
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Best (x,x')This schematics suggests parallel injection.
Might be misleading...
s=0 sk
ss
β
Same ε by smaller xk and x'
k=0 is “more
expensive” in terms of kicker strength
x ' k=−αk /βk⋅xkx
x'
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Use this:
Best (x,x')This schematics suggests parallel injection.
Might be misleading...
s=0 sk
ss
β
Same ε by smaller xk and x'
k=0 is “more
expensive” in terms of kicker strength
x ' k=−αk /βk⋅xkx
x'
![Page 7: Top-up injection into the SLS using a sextupole kickercas.web.cern.ch/sites/cas.web.cern.ch/files/case... · Top-up injection into the SLS using a sextupole kicker Group members:](https://reader034.fdocuments.us/reader034/viewer/2022050113/5f4a5fec06987f57ea3e8ba3/html5/thumbnails/7.jpg)
Where to put the septum and kicker?
s=0 sk
ss
β
xs=θk √βk βs sin(μ)● “Put where β
k and β
s is large to have large separation at septum with small kick by
kicker”... i.e. at the extremes of the the straight section.● But wait! there is μ as well....
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Where to put the septum and kicker?
s=0 sk
ss
β
dxs=θk √βk βs sin(μ)=d=sk−ss
● “Put where βk and β
s is large to have large separation at septum with small kick by
kicker”... i.e. at the extremes of the the straight section.● But wait! there is μ as well.... ● Do not mistify! For a drift, this is just the distance between the two points!
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Where to put the septum and kicker?
xs=θk √βk βs sin(μ)=d=sk−ss
● “Put where βk and β
s is large to have large separation at septum with small kick by
kicker”... i.e. at the extremes of the the straight section.● But wait! there is μ as well.... ● Do not mistify! For a drift, this is just the distance between the two points!
kicker
septum
d
So put them as far apart as needed to reduce kicker strength
s=0 sk
ss
β
d
xs=d⋅θk
Grandma's wisdom:
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Where to put the septum and kicker?
s=0 sk
ss
β
Biggest distance if symmetrically at the extremes... but...
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Where to put the septum and kicker?
s=0 sk
ss
β
x
x'
Biggest distance if symmetrically at the extremes... but...
● Ellipse is vertically flipped there...● Oscillation amplitude at septum is the same as the injection position
at kicker
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Where to put the septum and kicker?
s=0 sk
ss
β
Biggest distance if symmetrically at the extremes... but...
● Ellipse is vertically flipped there...● Oscillation amplitude at septum is the same as the injection position
at kicker● Best x
max,s/x
k if septum at crest (s=0)
x
x'
xmax , s
xk
=√βs/βk
xmax,s
xk
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Where to put the septum and kicker?
s=0 sk
ss
β
Biggest distance if symmetrically at the extremes... but...
quad
● Septum too close to upstream quad● Must be strong to avoid the beam hitting the quad
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Where to put the septum and kicker?
s=0 sk
ss
β
d
1) Have enough distance (d) between them to release kicker strength requirements
2) Shift both downstream➢Septum close to s=0
➢Or as it fits conveniently
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Cross the beam axis?
septum
kicker
x ' k=−αk /βk⋅xk
Which one needs a weaker kicker?
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Chosen parameters
● Fixed parameters– ss = 0 – septum at center of straight, at crest
● It is currently there, no need to move● Have space to avoid hitting upstream quad● Minimize oscillation amplitude of injected beam here
– sk = 4 m – kicker position along beamline● Largest possible distance leaving some more room
– L = 1 m – kicker length● easy to remember and multiply by
– r0 = 15 mm – kicker aperture radius
● Free parameters– xs, xk
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Multipole kicker●
●
● From this express sextupole strength “S”
● Pole tip field:
● Excitation coil: single-turn (minimizeL for fast risetime)
● Required current:
By=S2
xk2
xk '=xs '+B(xk )L
Bρ=
xk−x s
sk−ss
+ LS2 Bρ
x k2=−αk /βk⋅xk
S2
r02
r0
Coil (I0)
∮Bdl=∫0
r 0
S2
r2 dr=S6
r03=μ0 I 0/2
I 0=S3
r 03
μ0
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Kicker strength vs. injection offset
Pole tip field strength
● xs=18 mm
● xk=8 mm
● Injected beam 0.5 m at upstream quad
● Injected beam oscillation at septum: 6 mm
Easier on the positive side
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The sextupole kicker defocuses..tune incoming beam
to give required ellipse after kicker
Required input – strongly focused (i.e. large beamsize upstream)
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Decay of kicker field over several turns ● Subsequent kicks bring
beam center to larger orbits
● Strong defocusing makes beam large
● Kicker needs to have larger aperture
Possible solutions:● Change machine tune
close to 0.25 or 0.75● Make kicker decay faster● Introduce a small 'flat'
into the B(x) profile
x
B
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Magnet design
1/12 of the 2D cross section modelled
“Magnetic insulation” B.C.
“Perfect magnetic conductor” B.C.
Yoke, 6 poles, usingLHC magnet's B(H) curve
Pole shape iscircular
Samplingline atr=8 mmfor field quality analysis
conductor
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Magnet design
conductor
12⋅12∬ B⃗⋅H⃗=
12
LI 2
L≃11μ H /mU=11 kV for I 0=1 kA ,δ t=1μ s
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Magnet design: pole shape
Fourier spectrum of Az at r=8 mm
6-pole
First allowed higher-ordercomponent: 18-pole (n=9)
Ideal Rpole
/Raperture
ratio: ~0.57
(Just for fun... it probably doesn't matter at all)