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Collective EffectsDr. K. Cornelis

CERN

Introduction

• COLLECTIVE EFFECTS are responsible for the final intensity limit in most accelerators.

• Why is that?• The beams in our accelerators are kept and controlled by electromagnetic

fields (Magnets, radio frequency,..).• Beams consist of charged particles (protons, electrons, ions..) which create

their proper electromagnetic fields.• Adding up a lot of particles in a bunch create intense e.m. fields which are

competing with the controlling fields. This result in naughty “collective” effects. (If they are too many, the particles will start to act ‘collectively’ to make life difficult)

Introduction

• This lecture is about the consequences of pushing too much particles in a bunch, such as:• Space charge effects

• Wakefields resulting in:Longitudinal coupled bunch and single bunch instabilities

Transverse coupled bunch instabilities

Head tail instability

• But first: reminder of basic particle motion in a bunch (a bee story)

Busy bees

A bunch is not a static thing; particles move around like bees in a swarm.

A stable envelope

Order in the chaos

Phase space

px

xLongitudinal position

x

The orderly motion of a single bee

Transverse oscillationshorizontal or vertical

Frequency : betatron tune, Qh, Qv

Longitudinal oscillations

Frequency : synchrotron tune, Qs.

Space charge (origin collective, result single bunch)

Protons in a bunch repel each other resulting in a de-focusing force.

This causes a betatron tune shift which is different for particles close to the center and particles at the outside of the bunch.

0 2 4 6 8 100

0.1

0.2

0.3

0.4

0.5

0.451

0.099

F ak

100.2 ak

0 2 4 6 8 100.5

0.4

0.3

0.2

0.10

0.498

Detu ak

100.2 ak

Force as function of amplitude Tune shift as function of amplitude

Space charge

dQ ~

• Tune spread makes it difficult to avoid resonances

• Depends strongly on energy: it is an important performance limiter for low energy accelerators

• Make bunches as long as possible

Wakefields: field induced by bunch in the vacuum chamber

Wakefields fi

eld

In cavity like structures standing waves are provoked leading to longer lasting wakefields.

More intensity, stronger fields

An important fact about Wake fields

Longer bunches induce weaker fields

Longitudinal coupled bunch modesfi

eld

Bunches can be (de)-accelerated by the wake field of preceding bunches.

Longitudinal coupled bunch instability in the PS.

Courtesy L. Ventura, H. Damerau

Longitudinal single bunch instability

Longitudinal single bunch instability

Envelope is changing in real space and phase space -> coherent motion

Transverse instabilities

pp

When the bunch is off center a net transverse wakefield is created

Transverse coupled bunch mode

72 bunches

Bunches will receive a transverse kick depending on the transverse position of the previous bunches.

One way coupling between oscillators

The tail sees a force depending on the position of the head

One way coupling from head to tail

0 5 104

1 105

1.5 105

2 105

10

5

0

5

10

10

10

xi

2 105

1 i

0 5 104

1 105

1.5 105

2 105

10

5

0

5

10

8.461

8.576

y i

2 105

1 i

A small oscillation form the head induces an increasing oscillation of the tail

HEAD TAIL

‘Beam break up’ or ‘Fast head Tail’

• Happens mainly in LINAC’s • Can happen also in large circular accelerators if strong

enough to develop in a few turns.

0 5 104

1 105

1.5 105

2 105

4

2

0

2

45

5

xi

2 105

1 i

0 5 104

1 105

1.5 105

2 105

0

0.5

1

1.5

1.5

0

ssi

2 105

1 i

0 5 104

1 105

1.5 105

2 105

4

2

0

2

4

4

4

y i

2 105

1 i

0 5 104

1 105

1.5 105

2 105

0

0.5

1

1.5

1.5

0

csi

2 105

1 i

HEAD

TAIL

Head and tail interchanging positionLow intensity

Head and tail interchanging position

0 5 104

1 105

1.5 105

2 105

4

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0

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45

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xi

2 105

1 i

0 5 104

1 105

1.5 105

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4

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y i

2 105

1 i

High intensity (strong coupling)

0 5 104

1 105

1.5 105

2 105

0

0.5

1

1.5

1.5

0

ssi

2 105

1 i

0 5 104

1 105

1.5 105

2 105

0

0.5

1

1.5

1.5

0

csi

2 105

1 i

HEAD

TAIL

A picture of what is happening

0 5 104

1 105

1.5 105

2 105

10

5

0

5

10

6.498

6.613

xi

y i

2 105

1 i

Tail

Head

Head becomes tail Head becomes tail

0 5 104

1 105

1.5 105

2 105

4

2

0

2

45

5

xi

2 105

1 i

0 5 104

1 105

1.5 105

2 105

4

2

0

2

45

5

xi

2 105

1 i

Head tail instability, how it looks like

How to fight these instabilities?

• Make a smooth vacuum pipe to avoid strong wakefields.

• Maximize bunch length to minimize the peak wake field.

• Create a frequency spread (make them walk out of step),using chromaticity or non linear magnets

• Active damping with a feedback. Measure position and kick to put bunch back in place.

• These measures have all their limitations: limited tune spread to avoid resonances, limited power and bandwith in feedbacks, …

Damping with frequency spread

Summary

• The fields created by high intensity bunches create undesirable effects which limit the performance.

• In low energy accelerators the defocusing force created by the charges, create a tune spread and put particles on resonances.

• Wakefields, induced by intense bunches, result in a coupling force between bunches resulting in instabilities (coupled bunch)

• Wakefield variations over the length of the bunch create longitudinal single bunch instabilities and transverse head tail instabilities.

• Remark: other mechanisms can create similar coupling forces such as e-cloud and beam-beam.

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