A Brief Introduction of Radio Frequency Cavity in Particle ... · In accelerator physics (and many...
Transcript of A Brief Introduction of Radio Frequency Cavity in Particle ... · In accelerator physics (and many...
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A Brief Introduction of Radio Frequency Cavity
in Particle Accelerator
Nawin JuntongAccelerator Physicist
July 30, 2014
ATD seminarSLRI, Nakhon Ratchasima, Thailand
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Contents outline
• A brief history of DC and RF acceleration
• Principle of RF cavity
• RF cavity classification
• RF cavity properties
• RF cavity design criterion
• Effects of RF cavity to particle beam and suppression method
• RF cavity fabrication
• 2nd RF cavity at SLRI
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Lorentz Force
• Force that keeps a charged particle circulate in a ring or travel along a line.
• In the presence of E-field, a charged particle will experience a force in direction of E-field.
• In the presence of B-field, a charged particle will experience a force in a perpendicular direction of B-field.
𝐹 = 𝑞𝐸 + 𝑞( 𝑣 × 𝐵)
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DC Acceleration
• Use high DC voltage to accelerate a charged particle.
• Limitations:– High energy = High voltage DC source
(1 MeV = 1 MV DC source)
– Impossible for circular machine
𝐸 ∙ 𝑑 𝑠 = 0
– Breakdown limit of material
Cockcroft-Walton’s electrostatic accelerator
(1932)
Protons were accelerated and hit the lithium target producing helium and energy
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DC Acceleration
• Energy calculation
N. Juntong ([email protected]) February 7, 2014
Siam Photon Laboratory
V = 100 kVUE = 100 keV, 1 eV = 1.602×10−19 JUE = 1.6 x 10-14 J
Special relativity theory
E = E0 + Ek = mc2 = (𝑝𝑐)2+𝐸02 = γ𝐸0
𝛾 =1
1 − 𝛽2, 𝛽 =
𝑣
𝑐
𝛽 = 1 −1
𝛾2
Electrostatic potential energy
𝑈𝐸 = − 𝑞𝐸 ∙ 𝑑 𝑠 = qV Kinetic energy UE = Ek = mν2/2 = 1.6 x 10-14 J
ν = 2𝑈𝐸/𝑚 , me= 9.1 x 10-31 kg
ν = 1.8 x 108 m/sν = 0.6 c , c = 2.998 x 108 m/s
γ = E0 + Ek /E0
β = 1 − (𝐸0 (𝐸0+𝐸𝑘))2
, E0= 0.511 MeV
β = 0.548
ν = 0.548 c
40 MeV -> v = 0.99992 c
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RF Acceleration (time-varying field)
• Rolf Wideroe applied a 25-kV, 1 MHz AC voltage to the drift tube between two grounded electrodes. The beam experienced an accelerating voltage in both gaps.
• He accelerated Na and K beams to 50 keV kinetic energy equal to twice the applied voltage.
• This is not possible using electrostatic voltages
1928 - World’s first RF accelerator
Drift tube linac (DTL)
For slow particles- Proton @ few MeV
Drift tube length vary according to the velocity of particle and the frequency of a source
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RF Acceleration (time-varying field)
Image courtesy of F. Gerigk Image courtesy of F. Gerigk
Wideroe linac (1928) Louis Alvarez linac (1946)Energy gain
∆𝐸 = 𝑞𝑁𝑔𝑎𝑝𝑉𝑅𝐹
𝑙𝑛 =𝑣
2𝑓
synchronism condition
- The length of the drift tubes become too long for higher velocities.
- The drift tube become antennas when operation at higher frequencies (> 10MHz) - very poor efficiency
- Put Wideroe linac in a conducting cylinder.
- Each gap has the same resonant frequency, which is now determined by the diameter of the cylinder, the distance between the drift tubes, and their diameter
- Frequency up to 200MHz
Π -mode 2Π -mode
This is not the RF cavity This is the RF cavity
Yes, we can accelerate without cavities, but reachinghigher energies becomes very inefficient
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Principle of RF cavity
Maxwell’s equations
𝛻 × 𝐻 = 𝐽 +𝜕𝐷
𝜕𝑡
𝛻 × 𝐸 = −𝜕𝐵
𝜕𝑡
𝛻 ∙ 𝐷 = 𝜌
𝛻 ∙ 𝐵 = 0
𝐷 = 𝜀𝐸, 𝐵 = 𝜇𝐻J- current density, ρ – charge density
The total flux entering a bounded region equals the total flux leaving the same region
The total flux of electric displacement crossing a closed surface equals the total electric charge enclosed by that surface
A time-dependent magnetic field generates an electric field
The magnetic field H integrated around a closed loop equals thetotal current passing through that loop
Maxwell’s equations are of fundamental importance in electromagnetism, because they tell us the fields that exist in the presence of various charges and materials.
In accelerator physics (and many other branches of appliedphysics), there are two basic problems:
• Find the electric and magnetic fields in a system of chargesand materials of specified size, shape and electromagneticcharacteristics.
• Find a system of charges and materials to generate electricand magnetic fields with specified properties.
- Andy WOLSKI
Maxwell’s equations are linear- This means that if two fields satisfy Maxwell’s equations, so
does their sum.- As a result, we can apply the principle of superposition to
construct complicated electric and magnetic fields just by adding together sets of simpler fields
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Principle of RF cavity
Pill-box cavitySolving in cylindrical coordinates (r,φ,z)
𝐸𝑟 = 𝑗𝑘𝑧𝑘𝑐𝐸0𝐽1(𝑘𝑐𝑟)𝑒
−𝑗𝑘𝑧𝑧𝑒𝑗𝜔𝑡
𝐸𝑧 = 𝐸0𝐽0(𝑘𝑐𝑟)𝑒−𝑗𝑘𝑧𝑧𝑒𝑗𝜔𝑡
𝐵𝜑 = 𝑗𝑘
𝑍0𝑘𝑐𝐸0𝐽1(𝑘𝑐𝑟)𝑒
−𝑗𝑘𝑧𝑧𝑒𝑗𝜔𝑡
J0 and J1 are Bessel functions of the first kind of zeroth and first order
ω = 2πf is the angular frequency
k is the wave number
kz is the wave propagation constant
Z0 is the wave-impedance in free space
E0 is the amplitude of the electric field
j indicates imaginary parts
r = a
Ez = 0 at r = a cut off wave length λc
𝑘 =2𝜋
𝜆=𝜔
𝑐𝑍0 =
𝜇0𝜀0
= 377 Ω
Only waves with shorter wavelength, or a frequency above the cut off frequency ωc can propagate in the cavity undamped 𝑘𝑧
2 = 𝑘2 − 𝑘𝑐2
𝑘𝑐 =2𝜋
𝜆𝑐=𝜔𝑐𝑐
𝜆𝑐 ≈ 2.61 𝑎
𝑣𝑝ℎ =𝜔
𝑘𝑧
Phase velocity of wave
𝑘𝑧2 =
𝜔2
𝑣𝑝ℎ2 =
𝜔
𝑐
2
−𝜔𝑐𝑐
2
Dispersion relation (Brioullin diagram)
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Principle of RF cavity
Image courtesy of F. Gerigk
Dispersion relation (Brioullin diagram) of a cylindrical pipe
- Each frequency corresponds to a certain phase velocity
- The phase velocity is always larger than the speed of light
- At ω = ωc the propagation constant kz goes to zero and the phase velocity becomes infinite
- It is impossible to accelerate particles in a circular waveguide because synchronism between the particles and the RF is impossible (particles would have to travel faster than light to be synchronous with the RF)
- Information and therefore energy travels at the speed of the group velocity vg = dω/dkz, and is always slower than the speed of light
𝑘𝑧2 =
𝜔2
𝑣𝑝ℎ2 =
𝜔
𝑐
2
−𝜔𝑐𝑐
2
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Principle of RF cavity (TW)Slowing down phase velocity, in order to accelerate particles
- Put obstacles into waveguide, i.e. discs.
𝜔 =2.405𝑐
𝑏1 + 𝜅(1 − cos(𝑘𝑧𝐿)𝑒
−𝛼ℎ)
𝜅 =4𝑎3
3𝜋𝐽12(2.405)𝑏2𝐿
≪ 1, α ≈2.405
𝑎
Image courtesy of F. Gerigk Thomas P. Wangler, RF Linear Accelerator
Dispersion curve of disc-loaded TW structure
𝑣𝑝ℎ ≤ 𝑐, 2𝜋 3 < 𝑘𝑧𝐿 < 𝜋When a structure operates in the 2π/3 mode it means that the RF phase shifts by 2π/3 per cell, or in other words one RF period stretches over three cells. The particles then move in synchronism with the RF phase from cell to cell.
Constant impedance each cell’s bore radii are kept constant, i.e. uniform structure. The electromagnetic wave becomes more and more damped along the structure.
Constant gradient bore radius are changing from cell to cell. The maximum possible accelerating gradient in each cell.
R. B. Neal, M Report No. 259 (1961), Hansen Laboratories of Physics, Stanford University
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Principle of RF cavity (SW)
http://www.boost.org/doc/libs/1_54_0_beta1/libs/math/doc/html/math_toolkit/bessel/bessel_root.html
beam
Closing both ends of a circular wave guide with electric walls. This will yield multiple reflections on the end walls until a standing wave pattern is established.
Only with discrete frequencies and discrete phase changes can exist in the cavity. If one feeds RF power at a different frequency, then the excited fields will be damped exponentially.
𝜔𝑛 =𝜔0
1 + 𝑘 cos( 𝑛𝜋 𝑁), 𝑛 = 0,1,… ,𝑁
Dispersion curve of half-cell terminated SW structure, magnetic coupling
𝑘 =𝜔𝜋 − 𝜔0
𝜔0
Thomas P. Wangler, RF Linear Accelerator
Image courtesy of F. Gerigk
The frequency bandwidth |ωπ-ω0| is independent of the number of cells, which means that we can determine the cell-to-cell coupling constant by measuring the complete structure
For electric coupling the 0-mode has the lowest frequency and the π-mode has the highest frequency. In case of magnetic coupling this behavior is reversed.
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RF cavity classification
N. Juntong ([email protected]) February 7, 2014
Siam Photon Laboratory
Constant velocity, constant RF frequency Changing velocity, constant RF frequency
Non-accelerating cavities Changing velocity, variable RF frequency
Application
EM wave EM mode
Material
Travelling wave (TW)- Constant impedance- Constant gradient
Standing wave (SW)
Normal conducting (NC)
Superconducting (SC)
TEM
TM TE
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RF cavity classification Application
Constant velocity, constant RF frequency- Relativistic particles (β = v/c > 0.99)- Synchrotron, no need to adapt RF frequency to the
revolution frequency of the particles- Linac, no need to change the distance between
accelerating gaps- Electron accelerators energy > 1 MeV- High energy proton accelerators (GeV)- Ion accelerators 10s-100s of GeV (depending on
ion species)
Changing velocity, constant RF frequency- The velocity of the particles is increased along the
acceleration cycle but where the RF frequency can be kept constant
- Cyclotrons, use single-cell cavities to avoid any problems with synchronicity between subsequent gaps of multi-cell structures
- Low-β ion and proton linacs, use multi-cell structures in order to keep the overall linac length compact, it is necessary to adapt the gap distance to the velocity of the particles
Non-accelerating cavities- Mainly used with relativistic particles- RF deflection
- Chopper cavities, Low energy beam chopping systems, JPARC- CRAB cavities, to maximize the collision rate of colliding particle
beams, which are brought to collision under a certain angle- Funneling cavities, combination of two beams arriving at a certain
angle into one common beam line, if interleaved one by one the bunch repetition frequency will doubles during this process
- RF bunching- Used to keep bunches longitudinally confined during beam
transport- Form bunches out of CW beams coming from a particle source
- Beam monitoring cavities
Changing velocity, variable RF frequency- These are the most demanding operating conditions
for RF cavities, in- Low-β (ion/proton) synchrotrons and FFAGs- A change in RF frequency can be achieved by putting
a material with an adjustable permeability (typically ferrites) into a cavity
- Small accelerating voltages (10s of keV) can be achieved in these cavities at rather poor efficiencies
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RF cavity examples
Constant velocity, constant RF frequency
Application
MAX-IV cavityhttp://www.lightsources.org/
http://www.esrf.eu/ ESRF cavity
ILC cavity
CEBAF cavityhttp://wwwold.jlab.org/
http://anim3d.web.cern.ch/
LHC cavityhttp://hep.phys.sfu.ca/
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RF cavity examples
Changing velocity, constant RF frequency
Application
CAS, RF for cyclotron (materials)Sytze Brandenburg (KVI), P. K. Sigg(PSI)
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RF cavity examples
Changing velocity, variable RF frequency
Application
ISIS ferrite loaded cavity
EMMA ns-FFAG cavity
Ian Gardner (ISIS, RAL)
http://www.hep.manchester.ac.uk/g/accelerators/conform/news/guide/
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RF cavity examplesNon-accelerating cavities
Application
http://pbpl.physics.ucla.edu/
Deflecting cavity
Hans-H. Braun / PSI
Graeme Burt ,Lancaster University/ CICarlo J. Bocchetta (ELETTRA (Trieste)
Harmonic cavity can be operated in ACTIVE mode (RF external power supply) or in PASSIVE mode (voltage induced by beam current). The choice of several Synchrotron Light Sources nowadays has been the Passive Mode
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RF cavity classification EM wave
Travelling wave (TW)- Cavities are filled in space (cell after
cell) – sub- µs
- Constant impedance- Each cell has the same shape (iris
radius)- Constant gradient
- Each cell has different iris radius
Standing wave (SW)- Cavities are filled in time (Slowly
build up SW pattern at desired amplitude) - 10s µs to ms
NLC cavity
MAX-IV cavityMAX-IV linac cavityLars Malmgren, ESLS RF 2012
F. Gerigk (CERN/BE/RF)
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RF cavity classification
N. Juntong ([email protected]) February 7, 2014
Siam Photon Laboratory
Material
Normal conducting (NC)- Need water cooling- Higher gradient < 150 MV/m
Superconducting (SC)- Need Cryogenic plant- Low gradient < 45 MV/m
ILC cavity
Hitachi
Toshiba
LHC cavityhttp://hep.phys.sfu.ca/
MAX-IV cavityhttp://www.lightsources.org/
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RF cavity classification
N. Juntong ([email protected]) February 7, 2014
Siam Photon Laboratory
EM Mode
TM- Transverse Magnetic field on beam
path- Mainly use for accelerating particle
TE- Transverse Electric field on beam
path- Low surface losses- Can be adapted by adding drift tube
to make axial E field on beam path for acceleration (H-mode cavity)
TEM- Low frequency < 100 MHz- Frequency determined by the length- QWR (Quarter wave resonator)- HWR (Half wave resonator)- Spoke cavity
Crossbar H-mode cavityTM-mode cavity (50.6 MHz)
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RF cavity classification EM Mode
F. Gerigk (CERN/BE/RF)
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RF cavity classification EM Mode
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RF cavity classification EM Mode
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RF cavity properties
• Accelerating voltage (Va)
– 𝑉𝑎 = 𝐸𝑧𝑒𝑖𝜔𝑧/𝑐𝑑𝑧
• Accelerating gradient (Ea)
– 𝐸𝑎 =𝑉𝑎
𝐿, L – effective length of cavity
• Store Energy (U)
– 𝑈 =1
2𝜇0 𝑉 𝐻
2𝑑𝑉 =
1
2𝜀0 𝑉 𝐸
2𝑑𝑉
• Power dissipate on cavity wall (Pc)
– 𝑃𝑐 =1
2𝑅𝑠 𝑆 𝐻
2𝑑𝑆 , Rs – Surface
resistance
• Unloaded Quality factor (Q0)
– 𝑄0 =𝜔𝑈
𝑃𝑐
• Shunt impedance (Ra)
– 𝑅𝑎 =𝑉𝑎2
𝑃𝑐
• R/Q
–𝑅
𝑄=
𝑉𝑎2
𝜔𝑈
• External Q (Qex), Loaded Q (QL)
– 𝑄𝑒𝑥 =𝜔𝑈
𝑃𝑒𝑥, 𝑄𝐿 =
𝜔𝑈
𝑃
–1
𝑄𝐿=
1
𝑄0+
1
𝑄𝑒𝑥
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RF cavity design criterion
• Efficiency of cavity
– 𝜂 = 𝑃𝑏𝑒𝑎𝑚𝑃𝑔𝑒𝑛
=𝑃𝑏𝑒𝑎𝑚
𝑃𝑏𝑒𝑎𝑚+𝑃𝑐
N. Juntong ([email protected]) February 7, 2014
Siam Photon Laboratory
NC SC
NC – increase peak fields in the area of nose to maximize shunt impedance, but it’s limit by Kilpatrick (maximum achievable field in vacuum as a function of frequency)
• Kilpatrick limit (1957)
– 𝑓 𝑀𝐻𝑧 = 1.64𝐸𝑘2𝑒
−8.5
𝐸𝑘 , Ek in MV/m
Modern cavities, Esurf = bEk, b is the bravery factor, 1<b<2.- Better vacuum and cleaner inner surfaces
SC – Pb >> Pc, no longer limit by losses- Optimize shape for a low ratios of Epeak,surf/Ea and Bpeak,surf/Ea , Ep/Ea ~ 2- Nose cone is not suitable, elliptical shape is basically used
F= 118 MHz, Ek =12 MV/m, Esm = 24 MV/mF= 500 MHz, Ek = 21 MV/m, Esm = 42 MV/m
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RF cavity design criterion
N. Juntong ([email protected]) February 7, 2014
Siam Photon Laboratory
Thomas P. Wangler, RF Linear Accelerator
Cost - Cost of building cavity, cost of RF station, cost of Cooling sytem, etc..
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RF cavity design criterion
Overall efficiency of project J.P.Delahaye, CLIC-ILC LET Beam Dynamics Workshop 23/06/09
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Effects to particle beam
Roger JONES (Manchester University), CAS 2010
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Effects to particle beam
Roger JONES (Manchester University), CAS 2010
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HOM suppression
Roger JONES (Manchester University), CAS 2010
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HOM suppression
Roger JONES (Manchester University), CAS 2010
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HOM suppression
Jörn Jacob, ESRF
V. Serrière, ESRF
Pascal SCHUMMER, SDMS
V. Serrière, ESRF, IPAC2011
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Cavity fabrication (ESRF cavity)
V. Serrière, ESRF
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Cavity fabrication (SCRF cavity)• From Sheets to Fields Hanspeter Vogel, RI
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SLRI 2nd RF Cavity
Source: Ake Andersson, MAX-LabSource: Soren Pape Moller, ASTRID2
Source: Ake Andersson, MAX-Lab
Source: Ake Andersson, MAX-Lab
Based on MAX-IV Cavity
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Proposed Cavity 3D shape
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Accelerating mode fields (118 MHz)
Electric field Magnetic field
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Higher Order Modes (HOM) in RF Cavity
Monopole Dipole Quadrupole
Sextupole Tenth-pole Twelfth-pole
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15/11/2012
Thank you
Synchrotron Light Research Institute
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