unit 4 - lecture 9 - rf cavities - uspas - u.s. particle...
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![Page 1: Unit 4 - Lecture 9 - RF cavities - USPAS - U.S. Particle ...uspas.fnal.gov/materials/09UNM/Unit_4_Lecture_9_RF_Cavities.pdf · Unit 4 - Lecture 9 - RF cavities.ppt Author: William](https://reader031.vdocument.in/reader031/viewer/2022030403/5a794f8a7f8b9aee3b8cbae8/html5/thumbnails/1.jpg)
US Particle Accelerator School
Unit 4 - Lecture 9
RF-accelerators:
RF-cavities
William A. Barletta
Director, United States Particle Accelerator School
Dept. of Physics, MIT
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US Particle Accelerator School
RF-cativties for acceleration
Microtron Synchrotron
Linac
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US Particle Accelerator School
S-band (~3 GHz) RF linac
RF-input
RF-cavities
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RF cativties: Basic concepts
Fields and voltages are complex quantities.
For standing wave structures use phasor representation
For cavity driven externally, phase of the voltage is
= t +
For electrons v c; therefore z = zo+ct
˜ V = Vei t where V = ˜ V
Zo is the reference plane
At t = 0 particle receives maximum voltage gain
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Basic principles and concepts
Superposition
Energy conservation
Orthogonality (of cavity modes)
Causality
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Basic principles:Reciprocity & superposition
If you can kick the beam, the beam can kick you
==>
Total cavity voltage = Vgenerator+ Vbeam-induced
Fields in cavity = Egenerator+ Ebeam-induced
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Basic principles: Energy conservation
Total energy in the particles and the cavity is conserved
Beam loading
Ui Uf
Wc
Wc = Ui - Uf
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Basics: Orthogonality of normal modes
Each mode in the cavity can be treated independently in
computing fields induced by a charge crossing the cavity.
The total stored energy is equals the sum of the energies in
the separate modes.
The total field is the phasor sum of all the individual mode
fields at any instant.
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Basic principles: Causality
There can be no disturbance ahead of a charge moving at
the velocity of light.
In a mode analysis of the growth of the beam-induced
field, the field must vanish ahead of the moving charge for
each mode.
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Example: Differential superposition
A point charge q induces a voltage Vo passing through a cavity, what
voltage is induced by a Gaussian bunch of charge q?
A differential charge induces the differential voltage
Say dq passes z = 0 at to; at time t the induced voltage will be
The bunch has a Gaussian distribution in time
d ˜ V = ˜ V odq
q = Voe
j ot dq
q
d ˜ V = Vo
qe j o ( t to )dq(to)
dq(to) =q
2e
to2
2 2dto
Integrate
V =Voej ote
o2 2
2 dto
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Basic components of an RF cavity
Outer region: Large, single turn Inductor
Central region: Large plate Capacitor
Beam (Load) current
I
B
EDisplacement current
Wall current
a
RdPower feed from rf - generator
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Lumped circuit analogy of resonant cavity
V(t)
I(t)
C
L
R
Z( ) = j C + ( j L + R) 1[ ]1
The resonant frequency is o = 1LC
Z( ) =1
j C + ( j L + R) 1=
( j L + R)
( j L + R) j C +1=
( j L + R)
(1 2LC) + j RC
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Q of the lumped circuit analogy
The width is0
=R
L /.C
Z( ) ~ 12
o2
2
+ ( RC)2
1
Converting the denominator of Z to a real number we see that
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More basics from circuits - Q
Q = o o Energy stored
Time average power loss
= 2 o Energy stored
Energy per cycle
E =
1
2L IoIo
*and
P = i2(t) R = 1
2IoIo
*Rsurface
Q = L
CR
= o
1
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Translate circuit model to a cavity model:
Directly driven, re-entrant RF cavity
Outer region: Large, single turn Inductor
Central region: Large plate Capacitor
Beam (Load) current
I
B
EDisplacement current
Wall current
a
Rd
L =μo a
2
2 (R + a)
C = o
R2
d
o = 1LC
= c2((R + a)d
R2a2
12
Q – set by resistance in outer region
Q =LCR
Expanding outer region
raises Q
Narrowing gap
raises shunt impedance
Source: Humphries, Charged Particle
Accelerators
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Properties of the RF pillbox cavity
We want lowest mode: with only Ez & B
Maxwell’s equations are:
and
Take derivatives
==>
1
r rrB( ) =
1
c 2 tEz r
Ez =tB
t
1
r rrB( )
= t
B
r+B
r
=1
c 2
2Ezt 2
r
Ezr
=r
B
t
2Ezr 2
+1
r
Ezr
=1
c 2
2Ezt 2
d
Ez
b
B
walls =
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For a mode with frequency
Therefore,
(Bessel’s equation, 0 order)
Hence,
For conducting walls, Ez(R) = 0, therefore
Ez r, t( ) = Ez (r) ei t
E z + E z
r+
c
2
Ez = 0
Ez (r) = Eo Jo cr
2 f
cb = 2.405
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E-fields & equivalent circuit: Ton1o mode
Ez
B
Rela
tive inte
nsity
r/R
T010
CL
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E-fields & equivalent circuits
for To2o modes
T020
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E-fields & equivalent circuits
for Tono modes
T030
T0n0 has
n coupled, resonant
circuits; each L & C
reduced by 1/n
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Simple consequences of pillbox model
L
Ez
R
B
Increasing R lowers frequency
==> Stored Energy, E ~ -2
E ~ Ez2
Beam loading lowers Ez for the
next bunch
Lowering lowers the fractional
beam loading
Raising lowers Q ~ -1/2
If time between beam pulses,
Ts ~ Q/
almost all E is lost in the walls
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The beam tube makes the field modes(& cell design) more complicated
Ez
B
Peak E no longer on axis
Epk ~ 2 - 3 x Eacc
FOM = Epk/Eacc
o more sensitive to cavity
dimensions
Mechanical tuning & detuning
Beam tubes add length & ’s
w/o acceleration
Beam induced voltages ~ a-3
Instabilities
a
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Cavity figures of merit
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Make the linac with a
series of pillbox cavities
Power the cavities so that Ez(z,t) = Ez(z)ei t
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Figure of Merit: Accelerating voltage
The voltage varies during time that bunch takes to cross gap
reduction of the peak voltage by (transt time factor)
=sin 2( )
2 where = d
c
2
TrfFor maximum acceleration ==> = 2/
d
Vt
Epk
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Figure of merit from circuits - Q
E =μo2
Hv
2dv =
1
2L IoIo
*
P = Rsurf
2H
s
2ds =
1
2IoIo
*Rsurf
Q = LC
Rsurf
= o
1
Q = o o Energy stored
Time average power loss=
2 o Energy stored
Energy lost per cycle
Rsurf =1
Conductivity o Skin depth~ 1/ 2
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Measuring the energy stored in the cavity
allows us to measure
We have computed the field in the fundamental mode
To measure Q we excite the cavity and measure the E field
as a function of time
Energy lost per half cycle = U Q
Note: energy can be stored in the higher order modes that
deflect the beam
U = dz0
ddr2 r
0
b Eo2
2
J1
2(2.405r /b)
= b2d Eo2 /2( ) J1
2(2.405)
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Keeping energy out of higher order modes
d/b
b/c
0 1 2 3 4
TM020
TM010
TE011
TE111Source bandwidth
(green)
Dependence of mode frequency
on cavity geometry
Choose cavity dimensions to stay far from crossovers
10
5
1
TE111 mode
End view
Side view
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Figure of merit for accelerating cavity:power to produce the accelerating field
Resistive input (shunt) impedance at relates power dissipated in walls to
accelerating voltage
Linac literature commonly defines “shunt impedance” without the “2”
Typical values 25 - 50 M
Rin = V 2(t)
P =
Vo2
2P = Q L
C
Rin = Vo
2
P ~
1
Rsurf
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Computing shunt impedance
P = Rsurf
2H
s
2ds
Rin = Vo
2
P
Rsurf =μ
2 dc
= Zoskin
rf
where Zo =μo
o= 377
The on-axis field E and surface H are generally computed with a
computer code such as SUPERFISH for a complicated cavity shape
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Compute the voltage gain correctly
The voltage gain seen by the beam can computed in the co-moving frame,
or we can use the transit-time factor, & compute V at fixed time
Vo2
= E(z)dzz1
z2
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Exercise: Pillbox array
Derive the Q and Rsh for the pillbox cavity as a function of
the dimensions of the cavity and the frequency of the
fundamental mode
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Z( ) =1
j C + ( j L + R) 1=
( j L + R)( j L + R) j C +1
=( j L + R)
(1 2LC) + j RC
=( j L + R)
12
o2
2
+ j RC
=
( j L + R) 12
o2
j RC
12
o2
2
+ RC( )2
=
j L 12
o2
R2C
+ R 1
2
o2
+
2
o2 R
12
o2
2
+ RC( )2
j L 12
o2
R2C
+ R
12
o2
2
+ RC( )2
=1
12
o2
2
+ RC( )2
R + j L 12
o2
R2C
Z =1
12
o2
2
+ RC( )2
R2 + 2 L 12
o2
R2C
2
1/ 2
Note on previous slide