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Search: Author = P.K.Giri

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2024GI04      J.Radioanal.Nucl.Chem. 333, 1467 (2024)

P.K.Giri, S.S.Ghugre, R.Raut

Model calculation for α-induced reactions of theranostic applications

NUCLEAR REACTIONS ²⁷Al(α, X)³⁰P, ²⁰⁹Bi(α, X)²¹¹At, ⁷⁵As(α, 3n), ⁵⁰Cr(α, 2n), ^63,65Cu(α, n), ⁷²Ge(α, 3n), ⁸⁵Rb, ⁸⁹Y(α, 3n), ¹⁰⁷Ag, ¹¹⁵Sn(α, n), ¹¹⁶Sn(α, 2n), ²⁰⁹Bi(α, 3n), (α, 2n), E<100 MeV; calculated σ, yields using TALYS. Comparison with available data.

doi: 10.1007/s10967-023-09068-z
Citations: PlumX Metrics

2024SH08      Eur.Phys.J. A 60, (2024)

N.Sharma, Dh.Singh, A.Mahato, R.K.Sahoo, L.Chhura, P.K.Giri, Sn.B.Linda, H.Kumar, S.A.Tali, M.A.Ansari, R.Ali, S.Kumar, I.Ahmed, Yashraj, R.Kumar, K.S.Golda, S.Muralithar, R.P.Singh

Evidence of compound nucleus theory in the population of incompletely fused composite system ¹⁶⁰Dy*

NUCLEAR REACTIONS ¹⁴⁶Nd(¹⁸O, X)¹⁶¹Er/¹⁵⁹Er/¹⁵⁸Er/¹⁶¹Ho/¹⁵⁹Ho/¹⁵⁷Dy/¹⁵⁵Dy, E=68-102 MeV; measured reaction products, Eγ, Iγ. ¹⁶⁰Dy; deduced production σ, T_1/2. Comparison with available data and the predictions of statistical model code PACE-4 based on compound nucleus theory. 15UD Pelletron heavy ion accelerator facility of Inter-University Accelerator Centre (IUAC), New Delhi, India.

doi: 10.1140/epja/s10050-024-01293-8
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2024SH14      J.Radioanal.Nucl.Chem. 333, 1541 (2024)

N.Sharma, Dh.Singh, A.Mahato, P.K.Giri, S.B.Linda, H.Kumar, S.A.Tali, M.A.Ansari, I.Ahmed, S.Kumar, Yashraj, R.Kumar, K.S.Golda, S.Muralithar, R.P.Singh

Role of incomplete fusion in production of ¹⁵⁵Tb

NUCLEAR REACTIONS ¹⁴⁶Nd(¹⁶O, X)¹⁵⁵Tb, E=3-7 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced σ. Comparison with PACE 4 calculations. General Purpose Scattering Chamber (GPSC) of Inter University Accelerator Centr e (IUAC), New Delhi, India.

doi: 10.1007/s10967-023-09111-z
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2024TA01      Nucl.Phys. A1042, 122809 (2024)

S.A.Tali, H.Kumar, M.A.Ansari, D.Singh, R.Ali, P.K.Giri, S.B.Linda, A.Mahato, N.K.Deb, R.Kumar, R.N.Ali

Comprehension of breakup fusion reactions using forward recoil range distribution measurements

NUCLEAR REACTIONS ¹⁶⁵Ho(¹²C, X)¹⁷¹Ta/¹⁷²Ta/¹⁷³Ta/¹⁷¹Hf/¹⁷³Hf/¹⁶⁹Lu/¹⁷⁰Lu/¹⁷¹Lu/¹⁶⁹Yb/¹⁶⁶Tm/¹⁶⁷Tm, E=88 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies and relative intensities, forward recoil range distributions (FRRDs) yields, most probable mean recoil ranges. Comparison with available data. Inter-University Accelerator Center (IUAC), New Delhi by employing the 15UD Pelletron accelerator facilities.

doi: 10.1016/j.nuclphysa.2023.122809
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2023MA05      Phys.Rev. C 107, 014601 (2023)

A.Mahato, D.Singh, N.Sharma, P.K.Giri, S.B.Linda, H.Kumar, S.A.Tali, A.Ali, M.Afzal Ansari, N.K.Deb, N.P.M.Sathik, S.Kumar, R.Kumar, S.Muralithar, R.P.Singh

Disentangling fractional momentum transfer in the ¹⁹F + ¹⁵⁴Sm system

NUCLEAR REACTIONS ¹⁵⁴Sm(¹⁹F, 5n)¹⁶⁸Lu, (¹⁹F, 6n)¹⁶⁷Lu, (¹⁹F, 5np)¹⁶⁷Yb, (¹⁹F, 3nα)¹⁶⁶Tm, (¹⁹F, 4nα)¹⁶⁵Tm, (¹⁹F, 5nα)¹⁶⁴Tm, (¹⁹F, 3n2α)¹⁶²Ho, (¹⁹F, 4n2α)¹⁶¹Ho, E=107 MeV; measured reaction products, evaporation residues (ERs), Eγ, Iγ; deduced ERs yields as a function of range in stopping medium, forward recoil range distributions (FRRDs) for the evaporation residues, range integrated σ, relative contributions of complete and incomplete fusion, mean ranges in stopping medium. Discussed linear momentum transfer from the projectile to target accounting also for projectile breakup α+¹⁵N and 2α+¹¹B. Activation technique. Beam from 15UD Pelletron accelerator facility at Inter University Accelerator Center (IUAC, India). ERs were collected with a stack of 26 aluminium catcher foils of different thicknesses placed immediately after the target. The decay of ERs on the catcher foils measured with HPGe detector.

doi: 10.1103/PhysRevC.107.014601
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2022DE10      Phys.Rev. C 105, 054608 (2022)

N.K.Deb, K.Kalita, H.Al Rashid, A.Das, S.Nath, J.Gehlot, N.Madhavan, R.Biswas, R.N.Sahoo, P.K.Giri, A.Parihari, N.K.Rai, S.Biswas, A.Mahato, B.J.Roy

Investigation of isotopic dependence on the O + Ni fusion cross section near barrier energies

NUCLEAR REACTIONS ⁶¹Ni(¹⁶O, X), E=34.6-49.7 MeV; ⁶¹Ni(¹⁸O, X), E=33.6-52.6 MeV; ⁶²Ni(¹⁸O, X), E=33.9-52.9 MeV; measured reaction products, evaporation residues; deduced fusion σ(Ε), fusion barrier distribution, fusion excitation function. Comparison to other experimental data and one-dimensional barrier penetration model (1DBPM) calculations. Recoil mass spectrometer - the heavy ion reaction analyzer (HIRA) at 15UD Pelletron accelerator facility at theInter-University Accelerator Center (IUAC), New Delhi.

doi: 10.1103/PhysRevC.105.054608
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6433.

2022KU33      J.Phys.(London) G49, 105103 (2022)

S.Kumar, P.K.Giri, R.Kumar, A.Yadav, R.Ali, S.Appannababu, A.Agarwal, S.Mukherjee, P.P.Singh, V.R.Sharma, B.P.Singh, S.Dutt

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

NUCLEAR REACTIONS ¹⁶⁹Tm(¹⁴N, X)¹⁶⁹Os/¹⁷⁹Re/¹⁷⁶W/¹⁷⁵W/¹⁷⁸Re/¹⁷⁷W/¹⁷⁴W, E ∼ 5.9 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced yields, σ, forward recoil range distribution (FRRD) of evaporation residues (ERs). The general purpose scattering chamber (GPSC) facility at Inter-University Accelerator Centre (IUAC), New Delhi.

doi: 10.1088/1361-6471/ac894b
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6441.

2022MA34      Phys.Rev. C 106, 014613 (2022)

A.Mahato, D.Singh, N.Sharma, P.K.Giri, S.B.Linda, H.Kumar, S.A.Tali, M.Afzal Ansari, A.Ali, N.K.Deb, N.P.M.Sathik, S.Kumar, R.Kumar, S.Muralithar, R.P.Singh

Effects of entrance channels on breakup fusion induced by ¹⁹F projectiles

NUCLEAR REACTIONS ¹⁵⁴Sm(¹⁹F, X), (¹⁹F, 4n), (¹⁹F, 5n), (¹⁹F, 6n), (¹⁹F, 5np), (¹⁹F, 3nα), (¹⁹F, 4nα), (¹⁹F, 5nα), (¹⁹F, 3n2α), (¹⁹F, 4n2α)E=78-110 MeV; measured Eγ, Iγ; deduced complete fusion and evaporation residues production σ(E), critical angular momentum, excitation functions for complete, incomplete fusion and total fusion. Incomplete fusion strength functions systematics for ¹⁶O, ¹⁹F, ^20Ne induced reactions. Activation technique measurement with HPGe detector. Comparison to statistical model calculations (PACE-4 code) and coupled channels (CCFULL code). 15UD Pelletron accelerator facility at the Inter-University Accelerator Center (IUAC), New Delhi.

doi: 10.1103/PhysRevC.106.014613
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6439.

2020BI07      Phys.Rev. C 102, 014613 (2020)

S.Biswas, A.Chakraborty, A.Jhingan, D.Arora, B.R.Behera, R.Biswas, N.K.Deb, S.S.Ghugre, P.K.Giri, K.S.Golda, G.Kaur, A.Kumar, M.Kumar, B.Mukherjee, B.K.Nayak, A.Parihari, N.K.Rai, S.Rai, R.Raut, R.N.Sahoo, A.K.Sinha

Quasielastic scattering measurements in the ²⁸Si + ^{142, 150}Nd systems

NUCLEAR REACTIONS ^142,150Nd(²⁸Si, ²⁸Si), (²⁸Si, ²⁸Si'), E=84-136 MeV; measured reaction products, E-ΔE correlation plots, quasielastic scattering σ(E) at the 15 UD Pelletron accelerator of IUAC-New Delhi; deduced barrier distributions. Comparison with coupled-channel calculations using CCFULL code.

doi: 10.1103/PhysRevC.102.014613
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2020DE32      Phys.Rev. C 102, 034603 (2020)

N.K.Deb, K.Kalita, H.Al Rashid, S.Nath, J.Gehlot, N.Madhavan, R.Biswas, R.N.Sahoo, P.K.Giri, A.Das, T.Rajbongshi, A.Parihari, N.K.Rai, S.Biswas, Khushboo, A.Mahato, B.J.Roy, A.Vinayak, A.Rani

Role of neutron transfer in the sub-barrier fusion cross section in ¹⁸O + ¹¹⁶Sn

NUCLEAR REACTIONS ¹¹⁶Sn(¹⁸O, X), E(cm)=44.6-74.3 MeV; measured evaporation residues, time of flight of evaporation residue, fusion σ(E) using the Heavy-Ion Reaction Analyzer (HIRA) array at the 15 UD Pelletron of IUAC-New Delhi; deduced fusion barrier distributions; examined the effects of positive Q-value neutron transfer (PQNT) channels on sub-barrier fusion. Comparisons with coupled-channels calculations using the CCFULL code, including 2+ and 3- excited states of ¹¹⁶Sn, and 2+ excited state of ¹⁸O; analyzed systematics of reduced fusion excitation functions of ^112,116Sn, ¹¹²Cd(¹⁶O, X) and ¹¹⁶Sn, ¹⁴⁸Nd, ⁹²Mo, ⁷⁴Ge(¹⁸O, X) reactions at sub-barrier energies.

doi: 10.1103/PhysRevC.102.034603
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6391.

2020MA22      Eur.Phys.J. A 56, 131 (2020)

A.Mahato, D.Singh, P.K.Giri, S.B.Linda, H.Kumar, S.A.Tali, M.Afzal Ansari, R.Kumar, S.Muralithar, R.P.Singh

Probing of incomplete fusion dynamics in ¹⁴N + ¹²⁴Sn system and its correlation with various entrance channel effects

doi: 10.1140/epja/s10050-020-00126-8
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6384.

2019GI15      Phys.Rev. C 100, 024621 (2019)

P.K.Giri, D.Singh, A.Mahato, S.B.Linda, H.Kumar, S.A.Tali, S.Parasari, A.Ali, M.Afzal Ansari, R.Dubey, R.Kumar, S.Muralithar, R.P.Singh

Systematic study of low-energy incomplete-fusion dynamics in the ¹⁶O + ¹⁴⁸Nd system: Role of target deformation

NUCLEAR REACTIONS ¹⁴⁸Nd(¹⁶O, 3n)¹⁶¹Er, ¹⁴⁸Nd(¹⁶O, 5n)¹⁵⁹Er, ¹⁴⁸Nd(¹⁶O, 6n)¹⁵⁸Er, ¹⁴⁸Nd(¹⁶O, 2np)¹⁶¹Ho, ¹⁴⁸Nd(¹⁶O, 3np)¹⁶⁰Ho, ¹⁴⁸Nd(¹⁶O, 4np)¹⁵⁹Ho, ¹⁴⁸Nd(¹⁶O, 3nα)¹⁵⁷Dy, ¹⁴⁸Nd(¹⁶O, 5nα)¹⁵⁵Dy, ¹⁴⁸Nd(¹⁶O, 4npα)¹⁵⁵Tb, E=67.2, 72.4, 77.4, 84.1, 89.1, 94.7, 99.9 MeV; measured Eγ, Iγ; deduced σ(E), incomplete fusion (ICF) σ(E), effect of target deformation; analyzed previous experimental σ(E) data for many other systems for fraction of incomplete fusion. Measured σ compared with statistical model code PACE-4, and with previous experimental data. Experiment was performed using the 15UD Pelletron accelerator facility at Inter-University Accelerator Centre (IUAC), New Delhi, India.

doi: 10.1103/PhysRevC.100.024621
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6368.

2019GI17      Phys.Rev. C 100, 054604 (2019)

P.K.Giri, A.Mahato, D.Singh, S.B.Linda, H.Kumar, S.A.Tali, M.Afzal Ansari, R.Kumar, S.Muralithar, R.P.Singh

Examination of break-up fusion in the ¹⁶O + ¹⁴⁸Nd system through measurements of forward recoil range distributions and angular distributions

NUCLEAR REACTIONS ¹⁴⁸Nd(¹⁶O, 6n)¹⁵⁸Er, (¹⁶O, 5n)¹⁵⁹Er, (¹⁶O, 4np)¹⁵⁹Ho, (¹⁶O, 3np)¹⁶⁰Ho, (¹⁶O, 5nα)¹⁵⁵Dy, (¹⁶O, 3nα)¹⁵⁷Dy, (¹⁶O, 4npα)¹⁵⁵Tb, E AP 6 MeV/nucleon; measured Eγ, Iγ off-line, σ(θ) and forward recoil range distributions (FRRD) for evaporation residues, yields of evaporation residues using the 15 UD Pelletron facility at IUAC-New Delhi; deduced σ(θ) for total and complete fusion; analyzed incomplete fusion (ICF) fraction for several parameters using data from the present system, and previous experimental data for 16 other systems (six with ¹⁶O beam, four with ¹³C beam and three each for ¹²C and ²⁰Ne beams). Comparison of angular distributions with calculations using PACE4 code.

doi: 10.1103/PhysRevC.100.054604
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6374.

2019KU07      Phys.Rev. C 99, 034610 (2019)

H.Kumar, S.A.Tali, M.Afzal Ansari, D.Singh, R.Ali, A.Ali, S.Parashari, P.K.Giri, S.B.Linda, R.Kumar, R.P.Singh, S.Muralithar

Systematic study of incomplete-fusion dynamics below 8 MeV/nucleon energy

NUCLEAR REACTIONS ¹⁷⁵Lu(¹³C, 4n), (¹³C, 5n), (¹³C, 6n), (¹³C, 4np), (¹³C, 5np), (¹³C, nα), (¹³C, 3nα), (¹³C, 5nα), (¹³C, 2n2α), (¹³C, 3n2α), (¹³C, 4n2α)¹⁸²Ir/¹⁸³Ir/¹⁸⁴Ir/¹⁸²Os/¹⁸³Os/^183mOs/¹⁷⁹Re/¹⁸¹Re/¹⁸³Re/¹⁷⁶Ta/¹⁷⁷Ta/^178mTa, E AP 88 MeV; measured Eγ, Iγ, σ for evaporation residues by γ-activation method, and forward recoil range distributions (FRRDs) at IUAC, New Delhi; deduced most probable mean ranges, normalized peak widths for residues produced via complete fusion (CF), and/or incomplete fusion (ICF), relative contribution of CF and/or ICF components; calculated Fusion l-distributions for ¹⁷⁵Lu(¹²C, X), (¹³C, X), E=88 MeV systems using the CCFULL code. Comparison with results from previous experimental data for incomplete fusion fraction in ¹⁶⁹Tm, ¹⁶⁵Ho, ¹⁵⁹Tb, ¹¹⁵In(¹²C, X), (¹³C, X), (¹⁶O, X), and ²⁰⁹Bi(⁶Li, X), (⁷Li, X) systems, and deduced no systematic trend for dependency on the target deformation parameter β₂ in the study of the incomplete fusion (ICF) process.

doi: 10.1103/PhysRevC.99.034610
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2019SI01      Nucl.Phys. A981, 75 (2019)

D.Singh, P.K.Giri, A.Mahato, S.B.Linda, H.Kumar, M.A.Ansari, R.Ali, S.A.Tali, M.H.Rashid, R.Guin, S.K.Das

Probing of incomplete fusion dynamics and its correlation with various systematic

NUCLEAR REACTIONS ⁵⁹Co(²⁰Ne, xnypzα), E=62-150 MeV; measured activation Eγ, Iγ using HPGe coupled to PC data acquisition system; deduced complete, incomplete fusion σ, using MAESTRO and CANDLE systems (also using older publshed measurements of the authors); calculated σ, ICF fraction vs deformation using PACE-2 code. Cross sections and ICF fractions compared with available data.

doi: 10.1016/j.nuclphysa.2018.10.080
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2019SI31      Eur.Phys.J. A 55, 164 (2019)

D.Singh, P.K.Giri, A.Mahato, S.B.Linda, R.Tripathi, H.Kumar, M.Afzal Ansari, N.P.M.Sathik, R.Ali, R.Kumar, S.Muralithar, R.P.Singh

Probing incomplete fusion dynamics and role of the projectile deformation in the ¹⁹F + ¹⁵⁴Sm system

NUCLEAR REACTIONS ¹⁵⁴Sm(¹⁹F, X)¹⁶⁰Dy/¹⁶²Dy/¹⁶³Dy/¹⁶²Ho; ¹⁵⁴Sm(¹⁹F, X)¹⁶⁵Er/¹⁶⁴Tm/¹⁶⁵Tm/¹⁶⁸Tm; ¹⁵⁴Sm(¹⁹F, X)¹⁶⁷Yb/¹⁵⁸Yb, E=5.1 MeV/nucleon; measured reaction pr oducts populated via complete and incomplete fusion; deduced multiplicity spectra for Z=1, 2 and for α-particles. complete fusion-evaporation α-particle energy profile in forward cone, γ-ray energy spectra, transition intensity distributions for Evaporation Residuals (ER) ¹⁶¹Dy, ¹⁶²Ho, ¹⁶⁵Er, transition intensity distributions, normalized yields for Incomplete Fusion (ICF) populated ¹⁶³Dy and ^164,165Tm from Complete Fusion (CF) together with ICF in interaction; deduced ratios for ¹⁹F+¹⁵⁴Sm and ¹⁶O+¹⁶⁰Gd.

doi: 10.1140/epja/i2019-12860-9
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2019SI43      Int.J.Mod.Phys. E28, 1950069 (2019)

D.Singh, S.B.Linda, P.K.Giri, A.Mahato, H.Kumar, S.A.Tali, M.Afzal Ansari, R.Kumar, S.Muralithar, R.P.Singh

Investigation of breakup fusion in ¹⁶O + ¹²⁴Sn system and its correlation with various entrance channel parameters

NUCLEAR REACTIONS ¹²⁴Sn(¹⁶O, X)¹³⁵Ce/¹³³Ce/¹³³La/¹³³Ba/¹³¹Ba/¹³²Cs/¹²⁹Ba/¹³⁵Cs/¹³¹Xe/¹³¹I, E ∼ 6.2 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced complete fusion (CF) and incomplete fusion (ICF) channels, evaporation residues, N/Z ratio of the target as an important entrance channel parameter which strongly affects the ICF dynamics.

doi: 10.1142/S0218301319500691
Citations: PlumX Metrics

2019TA15      Phys.Rev. C 100, 024622 (2019)

S.A.Tali, H.Kumar, M.Afzal Ansari, A.Ali, D.Singh, R.Ali, P.K.Giri, S.B.Linda, R.Kumar, S.Parashari, S.Muralithar, R.P.Singh

Systematic study of the break-up fusion process in the ¹²C + ¹⁶⁵Ho system and interplay of entrance channel parameters

NUCLEAR REACTIONS ¹⁶⁵Ho(¹²C, 3n)¹⁷⁴Ta, ¹⁶⁵Ho(¹²C, 4n)¹⁷³Ta, ¹⁶⁵Ho(¹²C, 5n)¹⁷²Ta, ¹⁶⁵Ho(¹²C, 6n)¹⁷¹Ta, ¹⁶⁵Ho(¹²C, 3np)¹⁷³Hf, ¹⁶⁵Ho(¹²C, 5np)¹⁷¹Hf, ¹⁶⁵Ho(¹²C, nα)¹⁷²Lu, ¹⁶⁵Ho(¹²C, 2nα)¹⁷¹Lu, ¹⁶⁵Ho(¹²C, 3nα)¹⁷⁰Lu, ¹⁶⁵Ho(¹²C, 4nα)¹⁶⁹Lu, ¹⁶⁵Ho(¹²C, 3npα)¹⁶⁹Yb, ¹⁶⁵Ho(¹²C, 2n2α)¹⁶⁷Tm, ¹⁶⁵Ho(¹²C, 3n2α)¹⁶⁶Tm, E=57.39, 61.78, 66.13, 70.38, 74.59, 78.88, 83.05, 87.38 MeV; measured Eγ, Iγ; deduced σ(E), fraction of incomplete fusion (ICF); analyzed previous experimental σ(E) data for many other systems for fraction of incomplete fusion. Measured σ compared with statistical model code PACE-4, and with previous experimental data. Experiment was performed using the 15UD Pelletron accelerator facility at Inter-University Accelerator Centre (IUAC), New Delhi, India.

doi: 10.1103/PhysRevC.100.024622
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6359.

2018SI14      Phys.Rev. C 97, 064604 (2018)

D.Singh, S.B.Linda, P.K.Giri, A.Mahato, R.Tripathi, H.Kumar, M.Afzal Ansari, N.P.M.Sathik, R.Ali, R.Kumar, S.Muralithar, R.P.Singh

Role of input angular momentum and target deformation on the incomplete-fusion dynamics in the ¹⁶O + ¹⁵⁴Sm system at E_Lab = 6.1 MeV/nucleon

NUCLEAR REACTIONS ¹⁵⁴Sm(¹⁶O, 6n), (¹⁶O, 6np), (¹⁶O, 2p), (¹⁶O, n2p), (¹⁶O, 2npα), (¹⁶O, 3npα), (¹⁶O, 4npα), (¹⁶O, 2pα), (¹⁶O, 2n2α), E=97.5 MeV; measured Eγ, γ(θ), Eα, α(θ), Ep, p(θ), γα-coin, γp-coin and spin distributions, feeding intensity patterns, and average mean driving input angular momenta of complete fusion (CF) and incomplete fusion (ICF) populated evaporation residues, multiplicity spectra recorded for charged particles using the Gamma Detector Array (GDA) and Charged Particle Detector Array at the 15UD Pelletron Accelerator facility of the IUAC-New Delhi. Comparison with earlier experimental data, and with statistical model calculations using PACE4 code. Complete- and incomplete-fusion reactions.

doi: 10.1103/PhysRevC.97.064604
Citations: PlumX Metrics

2018SI15      Phys.Rev. C 97, 064610 (2018)

D.Singh, S.B.Linda, P.K.Giri, A.Mahato, R.Tripathi, H.Kumar, S.A.Tali, S.Parashari, A.Ali, Ra.Dubey, M.Afzal Ansari, R.Kumar, S.Muralithar, R.P.Singh

Measurement of excitation functions of evaporation residues in the ¹⁶O + ¹²⁴Sn reaction and investigation of the dependence of incomplete fusion dynamics on entrance channel parameters

NUCLEAR REACTIONS ¹²⁴Sn(¹⁶O, 3n), (¹⁶O, 5n), (¹⁶O, 7n), (¹⁶O, 6np), (¹⁶O, 3nα), (¹⁶O, 5nα), (¹⁶O, 7nα), (¹⁶O, pα), (¹⁶O, 3npα), (¹⁶O, n2α), (¹⁶O, p2α), E=3-7 MeV/nucleon; measured Iγ, Eγ, evaporation residues populated from complete fusion and incomplete fusion reactions, σ(E) by activation method, and incomplete fusion fractions at 15UD Pelletron heavy ion accelerator facility of IUAC, New Delhi. Comparison with theoretical excitation functions using PACE-4 code, and with previous experimental results. ^{133,133m,135,137,137m}Ce, ¹³³La, ^{129,129m,131,131m,133m}Ba, ¹³¹I, ^131mXe, ^132,135mCs; measured γ spectra from isotopes produced in different reaction channels.

doi: 10.1103/PhysRevC.97.064610
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6341.

2018TA03      Nucl.Phys. A970, 208 (2018)

S.A.Tali, H.Kumar, M.Afzal Ansari, A.Ali, D.Singh, R.Ali, P.K.Giri, S.B.Linda, S.Parashari, R.Kumar, R.P.Singh, S.Muralithar

Study of incomplete fusion reaction dynamics in ¹³C + ¹⁶⁵Ho system and its dependence on various entrance channel parameters

NUCLEAR REACTIONS ¹⁶⁵Ho(¹³C, x), E=4-7 MeV/nucleon; measured ER (Evaporation Residues) activation off-line Eγ, Iγ using HPGe coupled to CAMAC-based data acquisition system CANDLE; deduced γ-ray energy spectra. ¹⁷⁴Ta; deduced T_1/2, σ; calculated σ. ^166,167Tm, ¹⁶⁹Yb, ¹⁷³Hf, ^{169,170,171,172}Lu, ^{172,173,174,175}Ta; deduced state, J, π, γ-ray energy Eγ, branching ratio, σ, incomplete fusion fraction vs A_targ/(A_proj+A_targ); calculated σ. Calculations done using statistical code PACE4. Incomplete fusion fraction compared also with published data from ¹⁶⁵Ho(¹²C, x), (¹⁶O, x), (²⁰Ne, x), E=4-7 MeV/nucleon.

doi: 10.1016/j.nuclphysa.2017.11.012
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6332.

2017SI24      Phys.Lett. B 774, 7 (2017)

D.Singh, S.B.Linda, P.K.Giri, A.Mahato, R.Tripathi, H.Kumar, M.Afzal Ansari, N.P.M.Sathik, R.Ali, R.Kumar, S.Muralithar, R.P.Singh

Spin distribution of evaporation residues formed in complete and incomplete fusion in ¹⁶O+¹⁵⁴Sm system

NUCLEAR REACTIONS ¹⁵⁴Sm(¹⁶O, X)¹⁶²Er/¹⁵⁸Dy/¹⁶³Dy/¹⁵⁹Tb/¹⁶⁴Tm/¹⁶⁵Tm/¹⁶⁵Yb/¹⁶⁶Yb, E=6.2 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced γ-ray energies, normalized yields, feeding intensity profiles of evaporation residues.

doi: 10.1016/j.physletb.2017.09.034
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