1 / 17

Accelerator technique

Accelerator technique. FYSN 430 Fall 2008. Syllabus. Task: determine all possible parameters for a new accelerator project Known: Scope of physics done with an accelerator Needed Accelerator type Building Devices…. Physics case. Nuclear physics Study of neutron rich isotopes

titus
Download Presentation

Accelerator technique

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Accelerator technique FYSN 430 Fall 2008

  2. Syllabus • Task: determine all possible parameters for a new accelerator project • Known: Scope of physics done with an accelerator • Needed • Accelerator type • Building • Devices…

  3. Physics case • Nuclear physics • Study of neutron rich isotopes • Study of heavy isotopes • Nuclear reactions • Applications • Isotope production with protons • Radiation damage tests (SEE) • Possible future plans ?

  4. Relevant parameters • Accelerated isotopes • Beam energies (low and high) • Beam intensities • Other beam properties • Emittance • Time structure • …

  5. Coulomb barrier for fusion reactions(production of heavy isotopes) • For fusion reactions the repulsive Coulomb barrier has to be overcome Coulomb force Coulomb potential that q1 feels

  6. q2, A2 q1, A1 r2 r1 rC = r1 + r2

  7. Distance at which nuclei touch each other Coulomb energy at rc

  8. Examples Fe + Pb A1 = 56, Q1 = 27 A2 = 208, Q2 = 82 WC = 272.5 MeV or 4.9 MeV/u for Fe C + Sn A1 = 12, Q1 = 6 A2 = 120, Q2 = 50 WC = 49.8 MeV or 4.15 MeV/u for C

  9. Note! Remember also recoil: The compound nucleus moves due to recoil Conservation of momentum: Kinetic energy of the recoil

  10. Total kinetic energy (lab. Frame) needed for the projectile Eproj=Ecoul+Erecoil Usually a small correction Rule of thumb: Eproj, lab/Aproj = 5 MeV/u

  11. Proton induced fission p- induced and n-induced Reaction (e.g.) proton + U • Coulomb wall approx. 15.4 MeV

  12. Mass distribution Higher proton energy

  13. High LET beams

  14. Low energy limit • Are energies below 5 MeV/u interesting? • No fusion • Advantage: Coulomb excitation • Ask the physicists for the lower limit • E.g. 40 MeV 40Ar: 1 MeV/u

  15. Beam intensities • Isotope production • High (100 mA) • Nuclear spectroscopy • A few pna – a few pmA • SEE tests • 100 particles/s (aA) and more

  16. Energy Protons: 1-100 MeV Other ions: 1- nx10 MeV/u Intensity aA – 100 mA Some limits

  17. Possible accelerators • Linear accelerator • Wideröe • Alvarez • Electrostatic (Tandem) • Cyclotron • Super conducting vs. conventional • Synchrotron

More Related