“Design Of The Ion Extraction System In A Reaction Microscope” Speaker: Marco Panniello Federico II University Federico II University Industrial Engineering.

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Presentation transcript:

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

Federico II University Federico II University Industrial Engineering PhD School Innovative Technologies For Materials, Sensors And Imaging” Federico II University Federico 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. Introduction Development Conclusions 2

Introduction Development - R.I.M.S. - The Recycler - Working Principles - Geometry U.C. - T.F.C. - Homogeneously - Catch & Resolve - Resolution - Suitable Geometry high precision device more appropriate for coincidence measurements than energy or momentum dispersive spectrometers. Evolutions: - COLTRIMS (Cold Target RIMS); - Reaction Microscopes. 3 Conclusions

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

5 Conclusions A simple structure that grants the homogeneous field on Detector axis can be taken as a basic idea. Introduction Development - R.I.M.S. - The Recycler - Working Principle - Geometry U.C. - T.F.C. - Homogeneously - Catch & Resolve - Resolution - Suitable Geometry

6 Conclusions In the real case we have not a point like volume source, so we have to take in account the consequent time jitter Introduction Development - R.I.M.S. - The Recycler - Working Principle - Geometry U.C. - T.F.C. - Homogeneously - Catch & Resolve - Resolution - Suitable Geometry ΔE/E=18%

7 Conclusions More difficult than you can expect……. Introduction Development - 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%

8 Conclusions A good acceptance needs a strongest field A good resolution needs a weaker field All depend by ion type and Spectrometer geometry Introduction Development - R.I.M.S. - The Recycler - Working Principle - Geometry U.C. - T.F.C. - Homogeneously - Catch & Resolve - Resolution - Suitable Geometry

9 spectrometer resolution limitations imposed by the detector As example : 10V/10cm ; Time resolutionΔt = 1ns = 0.01 a.u. Position resolution Δr = 0.1mm = 0.02 a.u. Conclusions Introduction Development - R.I.M.S. - The Recycler - Working Principle - Geometry U.C. - T.F.C. - Homogeneously - Catch & Resolve - Resolution - Suitable Geometry

Conclusions 10 In addition we have problems depending on the spectrometer, in terms of dimension limitations. Introduction Development - R.I.M.S. - The Recycler - Working Principle - Geometry U.C. - T.F.C. - Homogeneously - Catch & Resolve - Resolution - Suitable Geometry ΔE/E=0.5%

Introduction Development - R.I.M.S. - The Recycler - Working Principle - Geometry U.C. - T.F.C. - Homogeneously - Catch & Resolve - Resolution - Suitable Geometry Conclusions 11 Federico II University Federico II University Industrial Engineering PhD School Innovative Technologies For Materials, Sensors And Imaging” After several simulation I reached a geometry With 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 resolution 0.02 a.u. Longitudinal Momentum Resolution 0.01 a.u.

Grazie per l’attenzione Marco Panniello 12 “You do not really understand something until you can explain it to your grandmother” Albert Einstein Federico II University Federico II University Industrial Engineering PhD School Innovative Technologies For Materials, Sensors And Imaging”

Conclusions 13 Introduction Development - 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