Lecture 4 wakefields
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Lecture 4 Wakefields. Dr G Burt Lancaster University Engineering. Beam-Wave Coupling. Wakefields occur where ever there is coupling between the beam and RF at any frequency or mode. Like acceleration, beam-wave coupling can only occur when the RF is resonant with the beam.

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Lecture 4 Wakefields

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Lecture 4 wakefields

Lecture 4 Wakefields

Dr G Burt

Lancaster University

Engineering


Beam wave coupling

Beam-Wave Coupling

  • Wakefields occur where ever there is coupling between the beam and RF at any frequency or mode.

  • Like acceleration, beam-wave coupling can only occur when the RF is resonant with the beam.

  • This means either the wave must have a phase velocity equal to the speed of the beam or the beam must only experience the RF a fraction of the time.

In multi-cell cavities or in waveguide a dispersion diagram can be used to find resonances.

Resonances occur where ever the light line (Phase Advance=kzL =wL/vbeam) crosses the modes dispersion line (ie phase velocity=beam velocity).


Generation of rf current

Generation of RF Current

The negative potential difference causes the electrons to slow down and the energy is absorbed into the cavity

C

A

The lower energy electrons then pass through the cavity and force the electrons within the metal to flow back to the opposite side

A bunch of electrons approaches a resonant cavity and forces the electrons to flow away from the bunch.

B


Pancake effect

Pancake effect

  • Due to lorentz contraction the electric fields of the bunch are almost entirely perpendicular to the bunch.

  • This means wakefields cannot affect charges in front of itself only behind.


Bunch spectrum

Bunch Spectrum

  • A charged bunch can induce wakefields over a wide spectrum given by, fmax=1/T. A Gaussian bunch length has a Gaussian spectrum.

  • On the short timescale (within the bunch) all the frequencies induced can act on following electrons within the bunch.

  • On a longer timescale (between bunches) the high frequencies decay and only trapped low frequency (high Q) modes participate in the interaction.


Coupling impedance

Coupling Impedance

Narrowband Impedance

Broadband Impedance

Cut-off

Impedance

frequency

The fourier transform of a wakefield is the coupling impedance. It has three regions (shown above).

The broadband impedance region doesn’t look like it has much of an effect but it covers a huge frequency spectrum so it’s integral can dwarf the narrowband region.


Fundamental theorem of beam loading

Fundamental Theorem of Beam Loading

  • A charge, q, traverses a cavity and induces a voltage, Vc, in a mode of the cavity.

  • What proportion of Vc is seen by the charge?

  • If the voltage in the mode was initially zero and has voltage Vq when the charge leaves the cavity, the average voltage is Vq/2. This is the voltage seen by the charge.

  • This is known as the fundamental theorem of beam loading.

  • If a cavity has an initial voltage, Vc, in a mode and a bunch passes and induced an additional voltage Vq, the bunch will loose energy


Mode excitation

Mode Excitation

If we have a mode in a cavity with initial voltage Vc and a bunch traverses the cavity inducing an additional, superimposed, voltage Vq, The modal energy is

And by conservation of energy

As Vq is proportional to q we can group the terms in powers of q and q2. The q2 term gives

As the power of q term must balance a must be 2p times an integer, hence


Short range wakes

Short range wakes

Short range wakes are the wakefields acting inside the bunch, where the charge in the head induce wakes that act on the tail of the bunch.

For short length bunches, this is dominated by the narrowband impedance.

The wake is not a step for a real bunch (shown above) as the charge density varies as a Gaussian.


Single bunch wake

Single Bunch Wake

A mode excited by a single bunch will decay exponentially with time due to ohmic heating and external coupling.

Wake (V)

The single bunch will excite several modes each with different beam coupling and damping rates.

Bunch Separation km


Mode indices

Mode Indices


Dipole modes

Dipole modes

Dipole mode have a transverse magnetic and/or transverse electric fields on axis. They have zero longitudinal field on axis. The longitudinal electric field increases approximately linearly with radius near the axis.

Electric Magnetic

Wakefields are only induced by the longitudinal electric field so dipole wakes are only induced by off-axis bunches.

Once induced the dipole wakes can apply a kick via the transverse fields so on-axis bunches can still experience the effect of the wakes from preceding bunches.


Panofsky wenzel theorem

Panofsky-Wenzel Theorem

If we rearrange Farday’s Law ()and integrating along z we can show

Inserting this into the Lorentz (transverse( force equation gives us

for a closed cavity where the 1st term on the RHS is zero at the limits of the integration due to the boundary conditions this can be shown to give

This means the transverse voltage is given by the rate of change of the longitudinal voltage


Multibunch wakefields

Multibunch Wakefields

  • For multibunch wakes, each bunch induces the same frequencies at different amplitudes and phases.

  • These interfere to increase or decrease the fields in the cavity.

  • As the fields are damped the wakes will tend to a steady state solution.


Long range wakefields

Long Range Wakefields

  • The long range wakes are found by summing over all modes and all bunches

  • This is known as the sum wake.

  • The kick from a dipole mode can then be found using the equation below


Long range transverse wakes

The time taken to converge to this value is dependant on the modal Q factors.

The long range wakefield is a sum of damped periodic oscillations and hence converges to a finite value.

Long Range Transverse Wakes

Horizontal kick for 4 offset.

Vertical kick for 4 offset.

9-cell

9-cell


Resonances

Resonances

  • As you are summing the contribution to the wake from all previous bunches, resonances can appear. For monopole modes we sum

  • Hence resonances appear when

  • It is more complex for dipole modes as the sum is

  • This leads to two resonances at +/-some Δfreq from the monopole resonant condition.


Effect of frequency errors

Effect of frequency errors

Cavity

Deflected beam

The effect of frequency errors can be estimated by introducing small variations in the bunch spacing.

X’

Undeflected beam

X’

Wakefield Kick

Tolerance

As can be seen if the beam hits a resonance with a HOM the wakefields increase significantly.

% variation in bunch separation


Damping

Damping

  • As the wakes from each bunch add together it is necessary to damp the wakes so that wakes from only a few bunches add together.

  • The smaller the bunch spacing the stronger the damping is required (NC linacs can require Q factors below 50).

  • This is normally achieved by adding external HOM couplers to the cavity.

  • These are normally quite complex as they must work over a wide frequency range while not coupling to the operating mode.

  • However the do not need to handle as much power as an input coupler.


Coaxial hom couplers

I

Cs

R

Coaxial HOM couplers

HOM couplers can be represented by equivalent circuits. If the coupler couples to the electric field the current source is the electric field (induced by the beam in the cavity) integrated across the inner conductor surface area.

If the coaxial coupler is bent at the tip to produce a loop it can coupler to the magnetic fields of the cavity. Here the voltage source is the induced emf from the time varying magnetic field and the inductor is the loops inductance.

L

V

R


Loop hom couplers

L

L

I

Cs

R

I

Cs

R

Cf

Loop HOM couplers

Inductive stubs to probe couplers can be added for impedance matching to the load at a single frequency or capacitive gaps can be added to loop couplers.

Also capacitive gaps can be added to the stub or loop inductance to make resonant filters.

The drawback of stubs and capacitive gaps is that you get increase fields in the coupler (hence field emission and heating) and the complex fields can give rise to an electron discharge know as multipactor (see lecture 6).

As a result these methods are not employed on high current machines.


F probe couplers

F-probe couplers

F-probe couplers are a type of co-axial coupler, commonly used to damp HOM’s in superconducting cavities.

Their complex shapes are designed to give the coupler additional capacitances and inductances.

These additional capacatances and inductances form resonances which can increase or decrease the coupling at specific frequencies.

Capacative gaps

Inductive stubs

Output antenna

Log[S21]

The LRC circuit can be used to reduce coupling to the operating mode (which we do not wish to damp) or to increase coupling at dangerous HOM’s.

frequency


Waveguide couplers

waveguide 2

waveguide 1

w2/2

w1/2

Waveguide Couplers

Waveguide HOM couplers allow higher power flow than co-axial couplers and tend to be used in high current systems. They also have a natural cut-off frequency.

They also tend to be larger than co-axial couplers so are not used for lower current systems.

To avoid taking the waveguides through the cryomodule, ferrite dampers are often placed in the waveguides to absorb all incident power.


Choke damping

load

choke

cavity

Choke Damping

For high gradient accelerators, choke mode damping has been proposed. This design uses a ferite damper inside the cavity which is shielded from the operating mode using a ‘choke’. A Choke is a type of resonant filter that excludes certain frequencies from passing.

The advantage of this is simpler (axially-symmetric) manufacturing


Beampipe hom dampers

Beampipe HOM Dampers

For really strong HOM damping we can place ferrite dampers directly in the beampipes. This needs a complicated engineering design to deal with the heating effects.


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