“Design Of The Ion Extraction System In A Reaction Microscope”

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“Design Of The Ion Extraction System In A Reaction Microscope” Speaker: Marco Panniello Federico II University Industrial Engineering PhD School “Innovative Technologies For Materials, Sensors And Imaging” 1

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Transcript of “Design Of The Ion Extraction System In A Reaction Microscope”

Page 1: “Design Of The Ion Extraction System In A Reaction Microscope”

“Design Of The Ion Extraction System In A Reaction Microscope”

Speaker:

Marco Panniello

Federico II UniversityIndustrial Engineering PhD School

“Innovative Technologies For Materials, Sensors And Imaging”

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Federico II University Industrial Engineering PhD SchoolInnovative Technologies For Materials, Sensors And Imaging” IntroductionFederico II University

Industrial Engineering PhD School“Innovative Technologies For Materials, Sensors And Imaging”

Context:

Purpose:

Antiprotons Recycler ring for differential cross section measurements.

Design of a suitable geometry for the recoil ion extraction system.

IntroductionDevelopmentConclusions

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IntroductionDevelopment- R.I.M.S.- The Recycler- Working Principles- Geometry U.C.- T.F.C.- Homogeneously- Catch & Resolve- Resolution- Suitable Geometry

Recoil Ion Momentum Spectroscopy

• high precision device

• more appropriate for coincidence measurements than energy or momentum dispersive spectrometers.

• Evolutions:

- COLTRIMS (Cold Target RIMS);

- Reaction Microscopes.

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Conclusions

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The Recycler• The projectile hits the target gas molecules generating

an atomic reaction. The most common effect is the target ionization

• The “recoil” ion is extracted from the collision area and accelerated toward a Time-Position sensible Detector. (MCP).

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• The projectile type is antiproton, currently used for single pass experiments.

• A simple structure called recycler is able to use these antiprotons more than one time.

Conclusions

IntroductionDevelopment- R.I.M.S.- The Recycler- Working Principle- Geometry U.C.- T.F.C.- Homogeneously- Catch & Resolve- Resolution- Suitable Geometry

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Geometry Under Consideration

Conclusions

A simple structure that grants the homogeneous field on Detector axis can be taken as a basic idea.

IntroductionDevelopment- R.I.M.S.- The Recycler- Working Principle- Geometry U.C.- T.F.C.- Homogeneously- Catch & Resolve- Resolution- Suitable Geometry

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Time Focusing Condition

Conclusions

• In the real case we have not a point like volume source, so we have to take in account the consequent time jitter

IntroductionDevelopment- R.I.M.S.- The Recycler- Working Principle- Geometry U.C.- T.F.C.- Homogeneously- Catch & Resolve- Resolution- Suitable Geometry

ΔE/E=18%

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Homogeneous Field

Conclusions

More difficult than you can expect…….IntroductionDevelopment- R.I.M.S.- The Recycler- Working Principle- Geometry U.C.- T.F.C.- Homogeneously- Catch & Resolve- Resolution- Suitable Geometry

ΔE/E=1.4%

ΔE/E=0.27%

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Acceptance vs Resolution

Conclusions

• A good acceptance needs a strongest field

• A good resolution needs a weaker field

• All depend by ion type and Spectrometer geometry

IntroductionDevelopment- R.I.M.S.- The Recycler- Working Principle- Geometry U.C.- T.F.C.- Homogeneously- Catch & Resolve- Resolution- Suitable Geometry

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spectrometer resolution limitations imposed by the detector

As example : 10V/10cm ;

Time resolution Δt = 1ns

= 0.01 a.u.

Position resolution Δr = 0.1mm

= 0.02 a.u.MqUda

rP

)2(6.11

taqUP 3

// 10042.8

Resolution Considerations

Conclusions

IntroductionDevelopment- R.I.M.S.- The Recycler- Working Principle- Geometry U.C.- T.F.C.- Homogeneously- Catch & Resolve- Resolution- Suitable Geometry

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Conclusions10

Suitable Geometry

In addition we have problems depending on the spectrometer, in terms of dimension limitations.

IntroductionDevelopment- R.I.M.S.- The Recycler- Working Principle- Geometry U.C.- T.F.C.- Homogeneously- Catch & Resolve- Resolution- Suitable Geometry

ΔE/E=0.5%

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ConclusionsIntroductionDevelopment- R.I.M.S.- The Recycler- Working Principle- Geometry U.C.- T.F.C.- Homogeneously- Catch & Resolve- Resolution- Suitable Geometry

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Federico II University Industrial Engineering PhD SchoolInnovative Technologies For Materials, Sensors And Imaging”

After several simulation I reached a geometryWith these properties:

Length of acceleration region a = 7 cm

Potential U = 7 V

Maximum Transverse Momentum P = 8.7 a.u.It guarantee an Acceptance of 4π

Transverse momentum resolution0.02 a.u.

Longitudinal Momentum Resolution0.01 a.u.

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Grazie per

l’attenzioneMarco Panniello

END

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“You do not really understand something until you can explain it to

your grandmother”

Albert Einstein

Federico II University Industrial Engineering PhD SchoolInnovative Technologies For Materials, Sensors And Imaging”

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Conclusions13

A Look ForwardIntroductionDevelopment- R.I.M.S.- The Recycler- Working Principle- R.I.M.S. Theory

- P// Reconstruction

- T. F. Condition

- P† Reconstruction

- Resolution- A Look Forward

• Detection of Recoil Ion only is not enough to characterize the reaction completely.

• Hence, it is “sufficient” to measure the momentum vectors of all target fragments.

• Since the reactions product usually consist of ions and electrons, it’s necessary a system to push them towards a detector.• The electron trajectories are easily modified by small

magnetic fields.

• It is possible to detect ions and electrons at the same time using both electric and magnetic fields