Understanding the onset of incomplete fusion

The entrance channel effect on the onset and strength of incomplete fusion (ICF) has been studied in the present work. Several inclusive experiments have been performed to measure the ICF strength function in 12C,16O+169Tm systems at near and above barrier energies. Data obtained in these experiments suggest the existence of ICF even at slightly above barrier energies where complete fusion (CF) is supposed to be the sole contributor, and conclusively demonstrate strong projectile structure and energy dependence of ICF. The incomplete fusion strength functions for 160,12,13C+159Tb and 160,12,13C+181Ta systems are analyzed as a function of projectile α-Q-value at a constant νrel = 0.053c. It has been found that one neutron (1n) excess projectile 13C (as compared to 12C) results in less incomplete fusion contribution due to its relatively large negative α-Q-value. In order to understand the onset of ICF at such low energies, the driving input angular momenta (ℓ) involved in the production of different evaporation residues have been deduced from the analysis of experimentally measured spin-distributions for the same projectile-target combinations at the same incident energies. Higher ℓ-values, imparted into the system in non-central interactions, are found to be responsible for low energy ICF. The ICF-αxn/2αxn channels display involvement of higher ℓ-values than that observed in CF-xn/pxn/αxn/2αxn channels at the very same projectile energies. It has been observed that the mean value of ℓ increases with successively opened ICF channels and incident energy.

[1]  I. A. Rizvi,et al.  Influence of projectile breakup on the16O +115In reaction at energies≈4–7 MeV/nucleon , 2013 .

[2]  Vijay R. Sharma,et al.  Effect ofα-Qvalue on incomplete fusion , 2012 .

[3]  Vijay R. Sharma,et al.  Effect of entrance-channel parameters on incomplete fusion reactions , 2012 .

[4]  Rakesh Kumar,et al.  Energy dependence of incomplete fusion processes in the {sup 16}O+{sup 181}Ta system: Measurement and analysis of forward-recoil-range distributions at E{sub lab}<=7 MeV/nucleon , 2010 .

[5]  A. Diaz-Torres Modelling incomplete fusion dynamics of weakly bound nuclei at near-barrier energies , 2010, 1003.5614.

[6]  R. Kumar,et al.  Role of high l values in the onset of incomplete fusion , 2009 .

[7]  R. Kumar,et al.  Disentangling full and partial linear momentum transfer events in the {sup 16}O+{sup 169}Tm system at E{sub proj}{<=}5.4 MeV/nucleon , 2009 .

[8]  Rakesh Kumar,et al.  Probing of incomplete fusion dynamics by spin-distribution measurement , 2009 .

[9]  M. Dasgupta,et al.  Suppression of complete fusion due to breakup in the reactions $^{10,11}$B + $^{209}$Bi , 2008, 0811.3891.

[10]  Rakesh Kumar,et al.  Observation of large incomplete fusion in 16O + 103Rh system at ≈3–5 MeV/nucleon , 2008 .

[11]  R. Kumar,et al.  Spin-distribution measurement: A sensitive probe for incomplete fusion dynamics , 2008 .

[12]  Rakesh Kumar,et al.  Influence of incomplete fusion on complete fusion: Observation of a large incomplete fusion fraction at E ≈ 5 − 7 MeV/nucleon , 2008 .

[13]  Rakesh Kumar,et al.  Observation of complete- and incomplete-fusion components in 159Tb , 169Tm ( 16O , x) reactions: Measurement and analysis of forward recoil ranges at E/A ≈ 5-6 MeV , 2007 .

[14]  M. Dasgupta,et al.  Relating breakup and incomplete fusion of weakly bound nuclei through a classical trajectory model with stochastic breakup. , 2007, Physical review letters.

[15]  M. Dasgupta,et al.  Isomer ratio measurements as a probe of the dynamics of breakup and incomplete fusion , 2006 .

[16]  A. J. Pacheco,et al.  Comprehensive study of reaction mechanisms for the Be9+Sm144 system at near- and sub-barrier energies , 2006 .

[17]  A. J. Pacheco,et al.  Fusion, reaction and break-up cross sections of weakly bound projectiles on 64Zn , 2004 .

[18]  S. Connell,et al.  Incomplete fusion of projectile fragments in the interaction of12C with103Rh up to 33 MeV per nucleon , 2004 .

[19]  Steiner,et al.  Incomplete fusion reactions induced by 12C at 5.5-10 MeV/nucleon. , 1988, Physical review letters.

[20]  Garg,et al.  Gamma-ray multiplicity distribution associated with massive transfer. , 1985, Physical review. C, Nuclear physics.

[21]  O. Hansen,et al.  Dynamics of Incomplete Fusion Reactions from γ -Ray Circular-Polarization Measurements , 1984 .

[22]  W. Galster,et al.  Influence of the mass asymmetry on the onset of incomplete and the limit to complete fusion , 1984 .

[23]  H. Lehr,et al.  Formation and decay of the compound nucleus studied in the reaction20Ne+27Al , 1983 .

[24]  R. Janssens,et al.  Binary l-matched reactions in 14N + 159Tb collisions , 1982 .

[25]  R. Janssens,et al.  INCOMPLETE-FUSION REACTIONS IN THE N-14+TB-159 SYSTEM AND A SUM-RULE MODEL FOR FUSION AND INCOMPLETE-FUSION REACTIONS , 1980 .

[26]  R. Siemssen,et al.  INCOMPLETE FUSION IN C-12+GD-160 COLLISIONS INTERPRETED IN TERMS OF A GENERALIZED CONCEPT OF CRITICAL ANGULAR-MOMENTUM , 1979 .