Study of incomplete fusion reaction dynamics in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" altimg="si1.gif" overflow="scroll"><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">C</mml:mi></mml:mrow><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>13</mml:mn></mml:mrow></mml:mmultiscripts><mml:mo>+</mml:mo><mml:msup><mml:mrow/><mml:mrow><mml:mn>165</mml:mn></mml:mrow></mml:msup><mml:mrow><mml:mi mathvariant="normal">Ho</mml:mi></mml:mrow></mml:math> system and its dependence on various en

Tali, Suhail A.; Kumar, Harish; Ansari, M. Afzal; Ali, Asif; Singh, D.; Ali, Rahbar; Giri, Pankaj K.; Linda, Sneha B.; Parashari, Siddharth; Kumar, R.; Singh, R. P.; Muralithar, S.

doi:10.1016/j.nuclphysa.2017.11.012

Cited by 24 publications

(2 citation statements)

References 34 publications

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“…Prior studies have examined ICF reaction dynamics as a function of various entrance channel parameters viz. μ MA [26], Z P Z T [27] and the Q α -value [23] of the projectile, all of which play, a very important role. To study the present data as a function of the aforementioned entrance channel parameters, the ICF strength function/F ICF (%) has been deduced for the system 14 N + 169 Tm (present work-FRRDs) along with some known systems from the literature as Table 3.…”

Section: Dependency Of Icf Reaction Dynamics On Various Entrance Chan...mentioning

confidence: 99%

“…The forward recoil ranges and cross-section of the identified ERs have been calculated. The F ICF (%) obtained in the present experiment has been plotted as a function of different entrance channel parameters viz Q α -value [23], mass-asymmetry (μ MA = A T A P +A T ) (A P and A T is the projectile and target mass number) [26], Coulomb factor (Z P Z T ) (Z P and Z T is the projectile and target atomic number) [27] for the present system along with literature data. We have also introduced the entrance channel parameter called zeta (ζ) for the first time in ICF reactions to see the combined effect of μ MA and Z P Z T .…”

Section: Introductionmentioning

confidence: 99%

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Study of incomplete fusion reaction dynamics for the system ¹⁴N + ¹⁶⁹Tm using the forward Recoil Range distribution technique

Kumar¹,

Giri²,

Kumar³

et al. 2022

J. Phys. G: Nucl. Part. Phys.

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Studies in the past have demonstrated that complete fusion and incomplete fusion dynamics are both significant just above the Coulomb barrier, yet the dynamics of incomplete fusion are elusive since they are so complex below 10 MeV/nucleon. In order to investigate low-energy incomplete fusion dynamics, we measured the forward recoil range distribution of evaporation residues populated in the system 14N + 169Tm at energy ≈ 5.9 MeV/nucleon. A stack target-catcher activation technique followed by offline-γ- spectroscopy was used to estimate the forward recoil range distribution of the evaporation residues. In order to investigate a new parameter for describing incomplete fusion dynamics, the incomplete fusion fraction (FICF (%)) for the present system was estimated from the range-integrated cross-sections and compared with other systems in the literature. The forward recoil range distribution and range integrated cross-sections of seven evaporation residues have been estimated experimentally. These cross-section results agree well with the experimental results obtained from the excitation functions. On re-investigation of entrance channel systematics for Qα value of projectile, mass-asymmetry (µMA), and Coulomb factor (ZP ZT ), it has been found that the Qα-value systematic for 14N is not valid at all projectile energies. The forward recoil range distribution measurement is one of the direct methods available to probe the complete and incomplete fusion contributions in evaporation residues at low projectile energy. It has also been observed that the dynamics of ICF are not only dependent on the parameters of one entrance channel but on multiple entrance channels. We have also introduced the entrance channel parameter Zeta (ζ) for the first time in Incomplete Fusion reactions to see the combined effect of mass-asymmetry (µMA) and ZP ZT, as this parameter is better suited than µMA and ZP ZT individually and has a linear dependency on FICF (%).

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Section: Dependency Of Icf Reaction Dynamics On Various Entrance Chan...mentioning

confidence: 99%

Section: Introductionmentioning

confidence: 99%

Study of incomplete fusion reaction dynamics for the system ¹⁴N + ¹⁶⁹Tm using the forward Recoil Range distribution technique

Kumar¹,

Giri²,

Kumar³

et al. 2022

J. Phys. G: Nucl. Part. Phys.

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Excitation functions of the p+Nb93 reaction in the energy range 10–22 MeV

et al. 2018

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Excitation function of the p+natAg reactions in the energy range 10–22 MeV

et al. 2018

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Study of incomplete fusion reaction dynamics in C13+165Ho system and its dependence on various en

Cited by 24 publications

References 34 publications

Study of incomplete fusion reaction dynamics for the system ¹⁴N + ¹⁶⁹Tm using the forward Recoil Range distribution technique

Study of incomplete fusion reaction dynamics for the system ¹⁴N + ¹⁶⁹Tm using the forward Recoil Range distribution technique

Excitation functions of the p+Nb93 reaction in the energy range 10–22 MeV

Excitation function of the p+natAg reactions in the energy range 10–22 MeV

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Study of incomplete fusion reaction dynamics in C13+165Ho system and its dependence on various en

Cited by 24 publications

References 34 publications

Study of incomplete fusion reaction dynamics for the system 14N + 169Tm using the forward Recoil Range distribution technique

Study of incomplete fusion reaction dynamics for the system 14N + 169Tm using the forward Recoil Range distribution technique

Excitation functions of the p+Nb93 reaction in the energy range 10–22 MeV

Excitation function of the p+natAg reactions in the energy range 10–22 MeV

Contact Info

Product

Resources

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Study of incomplete fusion reaction dynamics for the system ¹⁴N + ¹⁶⁹Tm using the forward Recoil Range distribution technique

Study of incomplete fusion reaction dynamics for the system ¹⁴N + ¹⁶⁹Tm using the forward Recoil Range distribution technique