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Recoil charge state distributions in 12C(a,g)16O at DRAGON

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Presentation on theme: "Recoil charge state distributions in 12C(a,g)16O at DRAGON"— Presentation transcript:

1 Recoil charge state distributions in 12C(a,g)16O at DRAGON
Joel Zylberberg Simon Fraser University TRIUMF Student Symposium Aug. 2, 2006

2 TRIUMF Student Symposium 02/08/2006
Outline Astrophysical importance of 12C(a,g)16O The DRAGON to study nuclear astrophysics Yield determination at DRAGON Charge state distributions (CSD’s) Measurements Simulations Conclusions TRIUMF Student Symposium 02/08/2006

3 Astrophysical importance of 12C(a,g)16O
Red giant stars He-Burning 3a  12C 12C(a,g)16O 16O or 12C from He-burning? HST image of red giant Mira TRIUMF Student Symposium 02/08/2006

4 TRIUMF Student Symposium 02/08/2006
The DRAGON At ISAC-TRIUMF a and p capture reactions: He and H targets Recoil mass separator Magnetic dipole: q/m and momentum Electric dipole: q/m and energy TRIUMF Student Symposium 02/08/2006

5 Yield calculations at DRAGON
Beam and recoils in several charge states; DRAGON selects one of them Need to know: Number of recoils Number of beam ions Detector efficiency Charge state fraction  Measuring and modeling CSD’s! TRIUMF Student Symposium 02/08/2006

6 TRIUMF Student Symposium 02/08/2006
Measuring CSD’s FC4: incident beam current FC1: after target (all charge states) FCCH: after dipole (only the selected charge state) Target thickness ~ pressure  repeat at different pressures TRIUMF Student Symposium 02/08/2006

7 Charge-state distributions
Collisions in gas Electron gain/loss Equilibrium eventually reached CSD of C3+ beam in He at 12.8 MeV TRIUMF Student Symposium 02/08/2006

8 TRIUMF Student Symposium 02/08/2006
CSD evolution Coupled differential equations  solve numerically s = charge-changing cross-section Equilibrium condition  That was (fairly) simple. What about the recoils? TRIUMF Student Symposium 02/08/2006

9 TRIUMF Student Symposium 02/08/2006
CSDsim code Want to predict recoil CSD Perform fit to CSD data to get cross-sections for C and O in He Calculate beam CSD numerically In each step: Add recoils Evolve CSD of recoils CSD of 9.6 MeV O3+ beam in He target as a function of target thickness. Data from ERNA (DRAGON-like facility in Germany) [Shurmann et al. NIMA 531 (2004) 428] TRIUMF Student Symposium 02/08/2006

10 TRIUMF Student Symposium 02/08/2006
CSDsim What happens during fusion? 2 main scenarios PU0e: Recoil Picks Up No Electrons (qrecoil = qbeam +2) PU2e: Recoil Same Charge as Beam ion (qrecoil = qbeam) TRIUMF Student Symposium 02/08/2006

11 TRIUMF Student Symposium 02/08/2006
CSDsim Model agrees with data Labels: PU0e - no e- capture during fusion PU2e – recoil picks up both e- during fusion Predictions converge for thick target F6/F5 in recoils: data from DRAGON compared to CSDsim predictions TRIUMF Student Symposium 02/08/2006

12 TRIUMF Student Symposium 02/08/2006
Summary 12C(a,g)16O important in astrophysics DRAGON detects 1 charge state of recoils CSDsim predicts charge state fractions: first successful modeling of recoil CSD No electrons captured during fusion, in this reaction (at this energy) 12C(a,g)16O data analysis improved TRIUMF Student Symposium 02/08/2006

13 TRIUMF Student Symposium 02/08/2006
Acknowledgements Thanks to: D. Hutcheon & the DRAGON group D. Shürmann at ERNA TRIUMF You, for your attention Questions? Comments? HST image of red supergiant Betelgeuse (Alpha Orionis) TRIUMF Student Symposium 02/08/2006

14 TRIUMF Student Symposium 02/08/2006
DRAGON data analysis In this particular reaction  PU0e behavior seen (can be modeled) May not always be PU0e To improve data analysis: Continue studying CSD’s of recoils (see if always PU0e) Use a post-stripper (gas or foil) Use a very thick target Measure recoil CSD each time a new reaction is measured TRIUMF Student Symposium 02/08/2006

15 Changing fusion cross-section
Resonance phenomenon As beam loses energy in target, fusion cross-section changes TRIUMF Student Symposium 02/08/2006


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