1 / 10

Role of mass asymmetry in fusion of super-heavy nuclei

Role of mass asymmetry in fusion of super-heavy nuclei. K. Siwek- Wilczyńska, I. Skwira-Chalot, J. Wilczyński. aim  to compare our model predictions with the measured (Dubna , GSI , Riken) evaporation -residue cross sections for synthesis of super-heavy nuclei in xn reactions .

april-harrison
Download Presentation

Role of mass asymmetry in fusion of super-heavy nuclei

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. Role of mass asymmetry in fusion of super-heavy nuclei K. Siwek- Wilczyńska, I. Skwira-Chalot, J. Wilczyński aim  to compare our model predictions with the measured (Dubna, GSI, Riken) evaporation-residue cross sections for synthesis of super-heavy nuclei in xn reactions. to predict cross sections for the synthesis of new super-heavy nuclei in coldand hotfusion reactions.  to verify the fusion hindrance factor (strongly dependent on the mass asymmetry).

  2. (synthesis) =(capture)×P(fusion) × P(survive) Systematic studies based on experimental data:  (capture) - the „diffused-barrier formula” ( 3 parameters): W. Świątecki, K. Siwek-Wilczyńska, J. Wilczyński Phys. Rev. C 71 (2005) 014602, Acta Phys. Pol. B34(2003) 2049 • Formula derived assuming: • Gaussian shape of the fusion barrier distribution • Classical expression for σfus(E,B)=πR2(1-B/E) A 2 fit to 48 experimental near-barrier fusion excitation functions in the range of 40 < ZCN< 98 resulted in systematics that allow us to predict values of the three parametersB0, w, R (K. Siwek-Wilczyńska, J. Wilczyński Phys. Rev. C 69 (2004) 024611)

  3. For very heavy systems a range of partial waves contributing to CN formation is limited (critical angular momenta for disappearing macroscopic fission barrier). We propose: cap(subcriticall) =cap for E ≤ Bo cap(subcriticall )= cap(E=Bo)*Bo/Ec.m. for E > Bo

  4. P(survive) – Statistical model (Monte Carlo method) Partial widths foremission of light particles – Weisskopf formula where: Upper limit of the final-state excitation energy after emission of a particle i i– crosssection for the production of the compound nucleus in the inverse process mi, si, εi- mass, spin and kinetic energy of the emitted particle ρ, ρi –level densities of the parent and daughter nuclei The fissionwidth (transition state method), E*< 40 MeV Upper limit of the thermal excitation energy at the saddle

  5. – shell correction energy, δshell (g.s.) (Möller et al., At. Data Nucl. Data Tables 59 (1995) 185), δshell(saddle)≈ 0 The level density is calculated using the Fermi-gas-model formula • Shell effects included as proposed by Ignatyuk (A.V. Ignatyuk et al., Sov. J. Nucl. Phys. 29 (1975) 255) where: U - excitation energy, Ed - damping parameter , (W. Reisdorf, Z. Phys. A. – Atoms and Nuclei 300 (1981) 227) Bs , Bk ( W.D. Myers and W.J. Świątecki, Ann. Phys. 84 (1974) 186)

  6. „Experimental” determination of fusion hindrance P(fusion) = σexp.(synthesis)/(σ(capture) P(survival)) Data - 48Ca……70Zn + 208Pb, 209Bi GSI, Riken Lines - calculations using Smoluchowski diffusion equation

  7. Smoluchowski Diffusion Equation • Viscosity of fluid Temperature Driving force W(x,t) = probability to find Brownian particle at positionx at timet Exact solution in a parabolic potential V(x) = -bx2/2 is a sliding, swelling Gaussian. P(fusion) = fraction of Gaussian captured inside the barrier as t→∞ P(fusion) = ½(1-erf√B/T) B = bx02/2 if x0 ≥ 0(injection point), saddle injection point W.J. Świątecki, K. Siwek-Wilczyńska, J. Wilczyński Acta Phys. Pol. B34 (2003)2049, IJMP E13 (2004) 261, Phys.Rev.C71 (2005) 014602

  8. Test of P(fusion) as a function of entrance channel asymmetry and excitation energy Calculations for Z=108 (different mass asymmetries): 26Mg + 248Cm→274-xnHs,58Fe+208Pb→266-xnHs, 136Xe+136Xe →272-xnHs  -Ch. Düllmann et al. Nature 418 (2002) 859, A. Türler et al. Eur. Phys. J. A17 (2003) 505 • S. Hofmann, Rep. Prog. Phys. 61 (1998) 639; and private communication

  9. 136Xe + 136Xe →272Hs experiment underway at Dubna

  10. Summary: • SHE production cross sections • (synthesis) =(capture) × P(fusion) × P(survive) • We have well tested tools for calculating capture cross sections (capture)and statistical decay of very heavy nuclei P(survive). • For P(fusion) we use a simple model based on the Smoluchowski diffusion equation. This model works quite well for cold fusion reactions. • It is essential to test predictions of P(fusion)for hot fusion reactions and more symmetric systems which probably will be used in attempts to synthesize new SHE (Z=120 and beyond), therefore comparison of Mg+Cm, Fe+Pb and Xe+Xe reactionsis very important. Kazimierz, September 27- October 1, 2006

More Related