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Injector Options for CLIC Drive Beam Linac Avni Aksoy Ankara University.

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Motivation  Bunch compression To compress a bunch longitudinally, trajectory in dispersive region must be shorter for tail of the bunch than it is for the head. z  E/E lower energy trajectory higher energy trajectory center energy trajectory Tail Head A path length difference for particles with a relative energy deviation d is :  : relative energy deviation (=  E/E)  R 56 : linear longitudinal dispersion (leading term for bunch compression)  T 566 : second - order longitudinal dispersion A. Aksoy CLIC Workshop 2015
12
Injector Options for CLIC Drive Beam Linac Avni Aksoy Ankara University
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Page 1: Injector Options for CLIC Drive Beam Linac Avni Aksoy Ankara University.

Injector Options for CLIC Drive Beam Linac

Avni AksoyAnkara University

Page 2: Injector Options for CLIC Drive Beam Linac Avni Aksoy Ankara University.

A. Aksoy CLIC Workshop 20152 / 12

Introduction

The beam pulse with 140 µs pulse length and 4.2 A current which consists of 24 × 24 sub-trains of about 120 bunches each is accelerated up to 2.4 GeV in Drive Beam Linac (DBL).

After DBL, 24 sub-trains will be merged into a single sub-train using delay loop (DL), combiner ring one (CR1) and combiner ring two (CR2). (Each sub train will have 100 A pulse current and 240 ns pulse length)

In order to avoid effect of CSR the beam will be decompressed and compressed several times before and after dispersive sections.

Current stability 0.75 × 10 -3 Phase stability 2.5 º @ 12 GHz Bunch length stability 1%

Phase stability 2.5 º @ 12 GHz 0.2 º @ 1 GHzBunch length stability 1%

Full energy spread < 50 MeV

26.01.2014

Page 3: Injector Options for CLIC Drive Beam Linac Avni Aksoy Ankara University.

A. Aksoy CLIC Workshop 20153 / 12

Motivation Bunch compression

To compress a bunch longitudinally, trajectory in dispersive region must be shorter for tail of the bunch than it is for the head.

z

DE/E

lower energy trajectory

higher energy trajectorycenter energy trajectoryTail Head

A path length difference for particles with a relative energy deviation d is : d : relative energy deviation (= DE/E) R56 : linear longitudinal dispersion (leading term for bunch compression) T566 : second - order longitudinal dispersion 26.01.2014

Page 4: Injector Options for CLIC Drive Beam Linac Avni Aksoy Ankara University.

A. Aksoy CLIC Workshop 20154 / 12

Motivation Effect of charge distribution to wake potential,

therefore to relative energy spread..λ longitudinal charge distributionWz wake function of structure

Any tail or spike on charge distribution will introduce nonelinear chirp..

26.01.2014

Page 5: Injector Options for CLIC Drive Beam Linac Avni Aksoy Ankara University.

A. Aksoy CLIC Workshop 20155 / 12

Bunch coming from injector

Shahin Sanaye Hajari

Not only the satellites are problem

Bunch charge distribution will lead the wakefield effect

26.01.2014

Page 6: Injector Options for CLIC Drive Beam Linac Avni Aksoy Ankara University.

A. Aksoy CLIC Workshop 20156 / 12

Tracking the bunch through linac

The chirp is not suitable for compressing (decompressing) on further steps..

The energy spread is much more larger than accepted on DL

The tail will cause beam loss at high energies

26.01.2014

Page 7: Injector Options for CLIC Drive Beam Linac Avni Aksoy Ankara University.

A. Aksoy CLIC Workshop 20157 / 12

• We propose a chicane to improve the longitudinal charge distribution

• Use a scrapper as energy collimator on the middle of chicane

We propose energy collimator just after injector (a)

After we remove tails and try to optimize charge distribution the longitudinal phase space of bunch at the end of linac seems suitable for compression with small R56The spike can cause large CSR effect?

26.01.2014

Page 8: Injector Options for CLIC Drive Beam Linac Avni Aksoy Ankara University.

A. Aksoy CLIC Workshop 20158 / 12

We propose energy collimator just after injector (b)

Seems suitable for compression with small R56 but not perfect..The spike can cause large CSR effect?

In order to improve this situation we have to find better initial distribution 26.01.2014

Page 9: Injector Options for CLIC Drive Beam Linac Avni Aksoy Ankara University.

A. Aksoy CLIC Workshop 20159 / 12

Photocathode RF gun based injector

● Phin gun is scaled to 1 Ghz

Structures are identical to DBL structure

σz =25 psσx,y =2.5 mm

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Page 10: Injector Options for CLIC Drive Beam Linac Avni Aksoy Ankara University.

A. Aksoy CLIC Workshop 201510 / 12

Bunch after Photo injector

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Page 11: Injector Options for CLIC Drive Beam Linac Avni Aksoy Ankara University.

A. Aksoy CLIC Workshop 201511 / 12

DBL layout with photo injector

● Linerazer is chosen the 3 GHz structure being used at CTF3

The longitudinal distribtion much more better for decompression / compression on further sections of DBL

26.01.2014

Page 12: Injector Options for CLIC Drive Beam Linac Avni Aksoy Ankara University.

A. Aksoy CLIC Workshop 201512

We have preliminary compared thermionic gun based injector and photocathode gun based injector

The advantages of photocathode gun– Satellite problem can be

solved– Lower emittance– Better charge distribution

against the effect of wakefiled

The disadvantages of photocathode gun– Laser technology– Laser stabilization →

charge stabilization– Cathode lifetime

The advantages of thermionic gun– Demonstrated at CTF3 and

operation for long time– Easy to operate – Long cathode life time

The disadvantages of thermionic gun– Almost impossible to

remove satellites– Large emittance– Worse charge distribution

against the effect of wakefiled

Conclusion

● In terms of longitudinal tolerances the photocathode injector is more relax than thermionic case since we use single dispersive section.

● It is possible to reduce R56 on chicane also● One should also compare the efficiency of power generation using

the final distributions26.01.2014

Thank you !


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