4. Space Charge Effects in RF Linear Accelerators
Transcript of 4. Space Charge Effects in RF Linear Accelerators
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4. Space Charge Effects in RF Linear Accelerators
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4.1. Principles of linear resonance acceleration
Layout of RF linear accelerator. (Courtesy of Sergey Kurennoy). 4. 2
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Layout of ion linear resonance accelerator.
Energy gain in RF linear accelerator. (Courtesy of Larry Rybarcyk.) 4. 3
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(Courtesy of Larry Rybarcyk)
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(Courtesy of Larry Rybarcyk) 4. 5
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4.2. Electromagnetic wave equations
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Cell of Drift Tube Accelerator (from M.Weiss, CERN 96-02, p.39)
Electric field lines between the ends drift tubes (from M.Konte, W.MacKay, 1991)
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Alvarez accelerating structure (from M.Weiss, CERN 96-02, p.39) 4. 9
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accelerating wave opposite wave
Z(z)T (t) = Eo cos(kzz)cos(ωt) =Eo
2[cos(ωt − kzz) + cos(ωt + kzz)]
kz =2πL
= 2πβλWave number
Cyclic frequency of RF field
Ez (z, r, t) = E cos(ωt − kzz)R(r)Equivalent traveling wave
Standing wave:
1r∂∂r(r ∂R
∂r)− R(kz
2 − ω 2
c2) = 0Substitution into wave equation gives for radial field component:
ω = 2πcλ
= 2π fRF
kz2 − ω 2
c2= kz
2 (1− ω 2
kz2c2) = kz
2 (1− β 2 ) = kz2
γ 2
R(r) = Io(kz rγ)Solution for radial field component:
where Io(x) is the modified Bessel function 4. 10
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4.3. Hamiltonian of particle motion in RF field
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H = (Px − qAx )2
2mγ+(Py − qAy )
2
2mγ+
pz2
2mγ 3 +qEkz[Io(
kzrγ)sin(ϕ s − kzζ )+ kzζ cosϕ s ]+ q
Ub
γ 2 (5.29)
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ω L =qB2mγ
H =P̂x2 + P̂y
2
2mγ+
pz2
2mγ 3 +qEkz[Io(
kzrγ)sin(ϕ s − kzζ )+ kzζ cosϕ s ]+mγω L
2 r2
2+ qUb
γ 2
Hamiltonian of particle motion in magnetic field :
where Larmor frequency
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Example of beam dynamics in accelerating structure. (Courtesy of Larry Rybarcyk.) 4. 19
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4.4. Longitudinal particle motion in RF field
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where is the phase deviation from synchronous particle (5.37) ψ ψ = kzζ
Relief of potential function and a family of phase trajectories (from Kapchinsky, 1985), . pψ =Ws −W
Separatrix of longitudinal phase space oscillations including acceleration.
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Longitudinal oscillations in RF field with = - 90o. (Courtesy of Larry Rybarcyk.) ϕs4. 26
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4.5. Transverse particle motion in RF field
Quadrupole beam focusing in RF linear accelerator. (Courtesy of Sergey Kurennoy). 4. 27
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H =px2 + py
2
2mγ+
pz2
2mγ 3 +qEkz[Io(
kzrγ)sin(ϕ s − kzζ )+ kzζ cosϕ s ]+mγ Ωr
2 r2
2+qUb
γ 2
Io(kzrγ) ≈1+ 1
4(kzrγ)2
sin(ϕ s − kzζ ) ≈ sinϕ s − kzζ cosϕ s = sinϕ s (1−ψ ctgϕ s )
ψ = kzζ
qE4kz
(kzrγ)2 = qEπ
2βγ 2λ
Ht =px2 + py
2
2mγ+ qE4kz
(kzrγ)2 sin(ϕ s − kzζ )+mγ Ωr
2 r2
2+ qUb
γ 2
Hamiltonian of particle motion in RF field:
Hamiltonian of transverse motion:
Near-axis approximation:
Expansion near synchronous particle:
Phase deviation from synchronous particle 4. 28
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Ht =px2 + py
2
2mγ+ qEπ2βγ 2λ
sinϕ s (1−ψ ctgϕ s )r2 +mγ Ωr
2 r2
2
Ω2 = 2πλqEmsinϕ s
βγ 3
Ht =px2 + py
2
2mγ− mγ4
Ω2 (1−ψ ctgϕ s )r2 +mγ Ωr
2 r2
2
Ht =px2 + py
2
2mγ+ mγ2r2[Ωr
2 − Ω2
2(1−ψ ctgϕ s )]
Ωrs2 =Ωr
2 − Ω2
2
Hamiltonian of near-axis, near synchronous particle motion, with Ub = 0:
Frequency of longitudinal oscillations:
Hamiltonian becomes:
Transverse oscillation frequency of synchronous particle in presence of RF field:
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Ωrs =n2Ω, n = 1, 2, 3 Parametric resonance occurs when
µs =ΩrsLβzc
γ s =14Ω2 ( L
βzc)2
Let us introduce phase advance for synchronous particle in RF field
and defocusing factor
Transversal equation of motion: d 2xdt 2
+ x[Ωrs2 − Ω2
2ctgϕ sΦsin(Ωt +ψ o )] = 0
4.6. Parametric resonance and beam emittance growth in RF field
Ht =px2 + py
2
2mγ+ mγ2r2 (Ωrs
2 + Ω2
2ψ ctgϕ s )
ψ = −Φsin(Ωt +ψ o )
Hamiltonian becomes:
Longitudinal particle oscillations with amplitude and frequency : Φ Ω
Finally, Hamiltonian is: Ht =px2 + py
2
2mγ+ mγ2r2[Ωrs
2 − Ω2
2ctgϕ sΦsin(Ωt +ψ o )]
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Parametric resonance regions (from Kapchinsky, 1985).
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Effective beam emittance growth outside of parametric resonance:
Phase space of transverse oscillations in presence of RF field (from Kapchinky, 1985).
εeffε
= 1+Φctgϕ sΩ2
4Ωrs2 −Ω2
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Required transverse focusing in presence of RF field
Ωr2 =ω L
2 − Ω2
2sinϕsinϕ s
H =P̂x2 + P̂y
2
2mγ+mγ r
2
2(ω L
2 − Ω2
2sinϕsinϕ s
)+ qUb
γ 2
d 2Rdz2
− ∍2
R3+ Ωr
2
(βc)2R − 2I
Ic (βγ )3R
= 0
d 2Redz2
= 0
Ωr2 = (βc
Re)2 ( ∍
2
Re2 +
2IIc (βγ )
3 )
B = 2mcβγqRe
( ∍Re)2 + 2I
Ic (βγ )3 +π (
qEλmc2
) sinϕ(βγ )3
(Reλ)2
Hamiltonian of particle motion in RF field with solenoid focusing Transverse oscillation frequency in presence of RF field
Envelope equation
Beam equilibrium condition Ωr2
(βc)2Re +
∍2
Re3 −
2IIc (βγ )
3Re= 0
Required magnetic field
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4.7. Beam bunching in RF field
Layout of klystron beam bunching scheme (from http://en.wikipedia.org/wiki/Klystron)
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RF beam bunching scheme: (left) initial beam modulation in longitudinal momentum, (right) final beam modulation in density. 4. 35
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dvdt
= qmU1
dsinωt
ϕ in +ϕout
2=ωt1
ϕout −ϕ in
2= θ12
vo =2qUo
m
v = vo +qmU1
ωd2sin(ϕ in +ϕout
2)sin(ϕout −ϕ in
2)
v = vo + v1 sinωt1
v = vo +qmU1
d tin
tout
∫ sinωt dt
v1 = voU1
2U0
M1
M1 =sinθ1
2θ12
θ1 =ωdvo
Equation of motion in RF gap of width d and applied voltage U1
Longitudinal particle velocity in RF gap
Longitudinal particle velocity after RF gap
Initial particle velocity after extraction voltage Uo
RF phase in the center of the gap
Transit time angle through the gap
Longitudinal particle velocity after RF gap
Amplitude of modulation of longitudinal velocity
Transit time factor of RF gap
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t2 = t1 +z
vo + v1 sinωt1≈ t1 +
zvo(1− v1
vosinωt1)
θ =ω zvo
Phase of arrival of particle into second gap as a function phase of the same particle in the first gap.
ωt2 −ωzvo
=ωt1 −ωzv1vo2 sinωt1
X =ω zv1vo2 = U1M1
2Uo
ωzvo
ωt2 −θ =ωt1 − X sinωt1
Time of arrival of particle to the second gap
Phase of arrival of particle into the second gap
Transit angle between gaps
Bunching parameter
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i2 =I
1− X cosωt1
Current in the second gap as a function of time.
X < 1
X = 1
X > 1
i1dt1 = i2dt2
i2 = i1dt1dt2
= Idt2dt1
Conservation of charge
Beam current in the second gap
Beam current in the second gap as a function of RF phase in the first gap and bunching parameter
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Phase of arrival of particle into second gap
i2 (x) = Ao + An cosnxn=1
∞
∑
Ao =1π
i2 (x)dxo
π
∫ An =2π
i2 (x)cosnxdxo
π
∫dx =ωdt2
Ao =1π
I dt1dt2
ω dt2o
π
∫ = I
Jn (z) =1π
cos(nϕ − zsinϕo
π
∫ )dϕ
An =2Iπ
cos(nωt1 − nX sinωt1o
π
∫ )dωt1 = 2IJn (nX)
x =ωt2 −θ =ωt1 − X sinωt1
i2 (x) = I + 2I Jn (nX)cosnxn=1
∞
∑
Expansion of the current in the second gap in Fourier series
Fourier coefficients
Differentiation of RF phase
Constant in Fourier series
Other coefficients in Fourier series
Bessel function (integral representation)
Beam current in the second gap
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Bessel functions determine amplitude of the fist, third and tenth harmonics of induced current in two-resonator buncher.
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The first harmonic of the induced beam current in the second gap as a function of z for different values of voltage at first gap.
The optimal value of bunching parameter is Xopt = 1.84.
I1I= 2J1(X)
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Beam bunching in presence of space charge forces*
2Ez =ρεo2zp
Ez =ρεozp
Gauss theorem
md 2zpdt 2
= q(Eext − Ez )
d 2zpdt 2
+ω p2zp =
qmEext
ω p =qρmεo
= 2cR
IIcβ
ρ = IπR2βc
* From Yu.A.Katsman, Microwave Devices, Moscow, 1973 (in Russian).
1D longitudinal space charge field
Space charge density of the beam
Substitution of space charge field gives:
Plasma frequency
Longitudinal oscillation in presence of space charge field, Ez, and external field Eext
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Reduction of beam plasma frequency in presence of conducting tube
ωq = Fpω p
d 2zpdt 2
+ωq2zp = 0
zp = Bo sinωq (t − t1)
dzpdt
= Boωq cosωq (t − t1)
dzpdt(t1) = Boωq = v1 sinωt1
Bo =v1ωq
sinωt1
Fp = 2.56J12 (2.4 R
a)
1+ 5.76
(ωavo)2
Reduced plasma frequency of the beam of radius R in the tube of radius a
Plasma frequency reduction factor
Longitudinal plasma oscillations in tube
Longitudinal particle oscillations under space charge forces
Longitudinal velocity of particle oscillations under space charge forces:
Constant Bo is defined from initial conditions for particle velocity after first RF gap:
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Effect of space charge repulsion on beam bunching. 4. 44
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zp =v1ωq
sinωq (t − t1)sinωt1
z = vo(t2 − t1)+ zp
z = vo(t2 − t1)+v1ωq
sinωq (t2 − t1)sinωt1
ωzvo
=ωt2 −ωt1 +ωv1ωqvo
sinωq (t2 − t1)sinωt1
ωt2 −θ =ωt1 − X sinωt1
X = ωv1ωqvo
sinωq (t2 − t1)
X = U1M1
2Uo
(ωzvo)sin(ωq
zvo)
ωqzvo
Finally, particle oscillations under space charge forces in the moving system
Particle drift
Multiply by
RF phase in the second gap
Modified bunching parameter in presence of space charge forces
sin(ωqzvo) = 1 ωq
zvo
= π2Condition for maximum bunching:
Xopt =U1M1
2Uo
( ωωq
) I1I= 2J1(Xopt )
ω
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(Left) initial and (right) final beam distribution in RF field. (Courtesy of Sergey Kurennoy.)
* From Y.B., NIM-A 483 (2002), 611-628.
4.8. Space charge dominated bunched beam in RF field*
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Sequence of bunches in RF field. 4. 47
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4.9. Beam equipartitioning in RF field
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The space charge density of the beam is obtained as an integral of the b eam distribution function over the particle momentum:
ρ (x,y,ζ) = q -∞
∞
-∞
∞
-∞
∞f dpx dpy dpz = ρoexp (- q Uext + Ubγ -2
Ho), (5.61)
where o is the space charge density in the center of the bunch. The value of o is unknown at this point due t o the unknown space charge potential of the bea m, Ub. For further analysis let us introduce an av erage value o f the spa ce charge density, ρ, which is equal to the density of an equivalent uniformly-charged cylindrical bunch with the same beam radius, R, and the same half-bunch length, l, as that of unknown stationary bunch. The space charge density of the cylindrical bunch, ρ = Q/V, is
ρ =Iλ
2πR2l c
(5.62)
where Q = I /c is the c harge of the bunch, V = πR22l is the volume o f the bunch and I is the beam current. Let us compare the value of ρ, Eq. (5.62), with that for another distributions. The space charge density of a uniformly populated spheroid with semi-axises R and l is
ρs = 3 I λ4π R2 l c
= 32
ρ. (5.63)
Space charge field of the bunch
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More precise analysis based on numerical solution of equation for beam potential indicates that synchronous phase is shifted in space charge dominated beam and phase width of the bunch also decreases but much slower than vertical size of the separatrix.
The separatrix shape for different values of space charge parameter (from Kapchinsky, 1985).
The potential function and separatrix of the beam with high space-charge density (from Kapchinsky, 1985).
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Stationary bunch profile
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Fig. 5.4. Comparison of potential functions of the bean and RF field: (dotted line) space charge potential of bunched beam distribution at the axis, s = -60o, C = 3.8; (solid line) inverse external potential at the axis, -Uext( ,0) .
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C =C (Gtb
Gzb )
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Fig. 5.5 Coefficient C in bunch shape for s = -30o as a function of ratio of transverse and longitudinal gradients of space c harge field of the beam: a) = 1, b) = 3, c) = 6.
Fig. 5.6 Coefficient C in bunch shape for s = -60o as a function of ratio of transverse and longitudinal gradients of space charge field of the beam: a) = 1, b) = 3, c) = 6.
a
a
b
bc
c
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4.10. Maximum beam current
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Fig. 5.7. Function f (ϕ s) = 3ϕs sinϕ s - 92
ϕs2 cosϕs + cosϕ s - cos2ϕ s in
maximum beam current, Eq. (5.118).
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Comparison with ellipsoidal model
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