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THE SMALL ISOCHRONOUS RING PROJECT AT MICHIGAN STATE UNIVERSITY J. Alberto Rodriguez

THE SMALL ISOCHRONOUS RING PROJECT AT MICHIGAN STATE UNIVERSITY J. Alberto Rodriguez

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Page 1: THE SMALL ISOCHRONOUS RING PROJECT AT MICHIGAN STATE UNIVERSITY J. Alberto Rodriguez

THE SMALL ISOCHRONOUS RING PROJECT AT MICHIGAN STATE UNIVERSITY

J. Alberto Rodriguez

Page 2: THE SMALL ISOCHRONOUS RING PROJECT AT MICHIGAN STATE UNIVERSITY J. Alberto Rodriguez

• Introduction

• Injection and Extraction Lines of SIR

• Simulations & Experimental Results

• Conclusions

OUTLINE:

Page 3: THE SMALL ISOCHRONOUS RING PROJECT AT MICHIGAN STATE UNIVERSITY J. Alberto Rodriguez

INTRODUCTION

• Several authors have proposed using high power cyclotrons for different applications.

• The space charge forces at these current levels (~ 10 mA) become very important and must be considered when such a machine is designed.

• Some understanding about space charge effects in the isochronous regime exists, although this knowledge is not yet complete.

Page 4: THE SMALL ISOCHRONOUS RING PROJECT AT MICHIGAN STATE UNIVERSITY J. Alberto Rodriguez

Turn separation

R

RINJ

REXT

ExtractionDeflector

Effects of the longitudinal space charge electric field:

• Energy spread within the bunch.

• Increase effective radial size.

• Destroys turn separation.

• Losses in extraction deflector.

v

Page 5: THE SMALL ISOCHRONOUS RING PROJECT AT MICHIGAN STATE UNIVERSITY J. Alberto Rodriguez

• Preliminary simulations showed a break up of the bunch.

y (cm)

x (c

m)

Page 6: THE SMALL ISOCHRONOUS RING PROJECT AT MICHIGAN STATE UNIVERSITY J. Alberto Rodriguez

Space charge forces scale with:

35

hm

Iqk AV

AV

BUNCHPEAKAV R

LhII

2

PSI Injector II (first turn)

SIR PSI Main Cyclotron

(first turn)

SIR

Ion H+ H2+ H+ H2

+

E 870 keV 20 keV 72 MeV 20 keV

IPEAK 34 mA 13 μA 290 mA 9 μA

Same k Same k

Page 7: THE SMALL ISOCHRONOUS RING PROJECT AT MICHIGAN STATE UNIVERSITY J. Alberto Rodriguez

Advantages of SIR:

• Time resolution of the diagnostics is much less demanding.

• Beam power is much lower.

• Availability is not an issue.

• Larger space charge forces than in PSI Injector II.

• Possibility of studying turn by turn evolution.

Page 8: THE SMALL ISOCHRONOUS RING PROJECT AT MICHIGAN STATE UNIVERSITY J. Alberto Rodriguez

Ion Source

Einzel Lens

Mass Separator

Emittance Measurement

System

Quadrupole Triplet

Chopper

Inflector Plates

Faraday Cup

Fast Faraday Cup

Deflector Plates

Injection Diagnostics

Page 9: THE SMALL ISOCHRONOUS RING PROJECT AT MICHIGAN STATE UNIVERSITY J. Alberto Rodriguez

Ion Source

Einzel Lens

Page 10: THE SMALL ISOCHRONOUS RING PROJECT AT MICHIGAN STATE UNIVERSITY J. Alberto Rodriguez

Quadrupole Triplet

Chopper

Inflector Plates

Faraday Cup

Page 11: THE SMALL ISOCHRONOUS RING PROJECT AT MICHIGAN STATE UNIVERSITY J. Alberto Rodriguez

Fast Faraday Cup

Deflector Plates

Page 12: THE SMALL ISOCHRONOUS RING PROJECT AT MICHIGAN STATE UNIVERSITY J. Alberto Rodriguez

• Methodology used in the analysis

• Scaling with bunch length, peak current and energy

• Impact of the beam emittance

• Energy spread within a bunch

• Repeatability of experimental measurements

• Experiments vs. Simulations

SIMULATIONS & EXPERIMENTAL RESULTS

Page 13: THE SMALL ISOCHRONOUS RING PROJECT AT MICHIGAN STATE UNIVERSITY J. Alberto Rodriguez

Methodology used in the analysis

Page 14: THE SMALL ISOCHRONOUS RING PROJECT AT MICHIGAN STATE UNIVERSITY J. Alberto Rodriguez

Scaling with bunch peak current

)( AITTEQ

Page 15: THE SMALL ISOCHRONOUS RING PROJECT AT MICHIGAN STATE UNIVERSITY J. Alberto Rodriguez

Impact of the beam emittance

Page 16: THE SMALL ISOCHRONOUS RING PROJECT AT MICHIGAN STATE UNIVERSITY J. Alberto Rodriguez

Energy spread within a bunch

)( AITTEQ

)(keVE

TTEQ

Page 17: THE SMALL ISOCHRONOUS RING PROJECT AT MICHIGAN STATE UNIVERSITY J. Alberto Rodriguez

Repeatability of experimental measurements

To = 0

To = 1 ms

To = 2 ms

Page 18: THE SMALL ISOCHRONOUS RING PROJECT AT MICHIGAN STATE UNIVERSITY J. Alberto Rodriguez

I = 5 μAI = 9.9 μA

I = 19.9 μA

Scaling with bunch peak current

)( AITTEQ

Page 19: THE SMALL ISOCHRONOUS RING PROJECT AT MICHIGAN STATE UNIVERSITY J. Alberto Rodriguez

Experiments vs. Simulations

Simulations

Experiments

Page 20: THE SMALL ISOCHRONOUS RING PROJECT AT MICHIGAN STATE UNIVERSITY J. Alberto Rodriguez

• The Small Isochronous Ring (SIR) has been completed.

• The control and data acquisition system of SIR has been finalized.

• Extensive simulations have been performed to characterize the impact of bunch length, current, energy and emittance on the bunch dynamics.

• The scaling laws of space charge effects with energy and current have been validated numerically and experimentally.

• Good agreement between experiments and simulations performed with CYCO has been shown.

CONCLUSIONS