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NSR database version of April 27, 2024.

Search: Author = R.Ali

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2024AL04      J.Phys.(London) G51, 015101 (2024)

S.Ali, M.Gull, K.Kumar, T.Ahmad, I.A.Rizvi, A.Agarwal, S.S.Ghugre, R.N.Ali, F.Khan

Systematic study of fusion suppression and its dependency on projectile breakup threshold energy

NUCLEAR REACTIONS ⁹³Nb(²⁰Ne, X)¹⁰⁹Sn/¹⁰⁸Sn/¹⁰⁵Cd/¹⁰⁴Cd/¹⁰⁹In/¹⁰⁸In/¹⁰⁷In/¹⁰⁵In/¹⁰³Ag/¹⁰¹Pd/¹⁰⁰Rh/⁹⁸Rh, E=145 MeV; measured reaction products, Eγ, Iγ; deduced σ and uncertainties, an empirical formula is proposed to interrelate the degree of fusion suppression and breakup threshold energy of the incident projectile. Comparison with the universal fusion function (UFF) to estimate the degree of fusion incompleteness, PACE4 calculations. The K130 cyclotron facility at the Variable Energy Cyclotron Centre (VECC), Kolkata, India.

doi: 10.1088/1361-6471/ad0a3b
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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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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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.

2020SH27      Eur.Phys.J. Special Topics 229, 2555 (2020)

J.A.Sheikh, R.N.Ali

Symmetry projection in atomic nuclei

doi: 10.1140/epjst/e2020-000111-3
Citations: PlumX Metrics

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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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6359.

2018KU04      Eur.Phys.J. A 54, 47 (2018)

H.Kumar, S.A.Tali, M.A.Ansari, D.Singh, R.Ali, Ka.Kumar, N.P.M.Sathik, A.Ali, S.Parashari, R.Dubey, I.Bala, R.Kumar, R.P.Singh, S.Muralithar

Sensitivity of low-energy incomplete fusion to various entrance-channel parameters

NUCLEAR REACTIONS ¹⁷⁵Lu(¹²C, x), E≈88 MeV; measured Eγ, Iγ(t) from catcher Al foils using precalibrated HPGe and FRRD (Forward Recoil Range Distribution), LMT (Linear Momentum Transfer); deduced contributions of IFC (InComplete Fusion) and CF (Complete Fusion) σ, discrete states of ER T_1/2. Compared with available data.

doi: 10.1140/epja/i2018-12483-8
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6332.

2017AL39      Nucl.Phys. A968, 403 (2017)

R.Ali, M.Afzal Ansari, D.Singh, R.Kumar, D.P.Singh, M.K.Sharma, U.Gupta, B.P.Singh, P.D.Shidling, D.Negi, S.Muralithar, R.P.Singh, R.K.Bhowmik

Observed side feeding in incomplete fusion dynamics in ¹⁶O + ¹⁶⁰Gd reaction at energy ∼ 5.6 MeV/A: Spin distribution measurements

NUCLEAR REACTIONS ¹⁶⁰Gd(¹⁶O, x), E≈5.6 MeV/nucleon; measured Eγ, Iγ(θ), Ep, Ip(θ), Eα, Iα(θ), pγ-coin, αγ-coin using GDA (Gamma Detector Array) consisting of 12 n-type Compton suppressed HPGE working together with CPDA (Charged Particle Detector Array); deduced relative spin distributions (relative yields vs spin) of different reaction channels, evaporation residues yrast bands side feeding intensities, mean input angular momentum for different reaction channels.

doi: 10.1016/j.nuclphysa.2017.09.005
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2017FR03      Int.J.Mod.Phys. E26, 1750030 (2017)

H.Fryman-Sinkhorn, E.H.Wang, C.J.Zachary, J.H.Hamilton, A.V.Ramayya, G.H.Bhat, J.A.Sheikh, R.N.Ali, A.A.Wani, A.C.Dai, W.Y.Liang, F.R.Xu, J.K.Hwang, N.T.Brewer, Y.X.Luo, J.O.Rasmussen, S.J.Zhu, G.M.Ter-Akopian, Yu.Ts.Oganessian

Possible very anharmonic one- and two-phonon γ-vibrational bands in ¹⁰³Mo

RADIOACTIVITY ²⁵²Cf(SF); measured decay products, Eγ, Iγ, γ-γ-coin. ¹⁰³Mo; deduced γ-ray energies and intensities, J, π, γ-vibrational bands. Comparison with potential energy surface calculations.

doi: 10.1142/S0218301317500306
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Data from this article have been entered in the XUNDL database. For more information, click here.

2017KU05      Nucl.Phys. A960, 53 (2017)

H.Kumar, S.A.Tali, M.Afzal Ansari, D.Singh, R.Ali, K.Kumar, N.P.M.Sathik, S.Parashari, A.Ali, R.Dubey, I.Bala, R.Kumar, R.P.Singh, S.Muralithar

Investigation of incomplete fusion dynamics at energy 4-8 MeV/nucleon

NUCLEAR REACTIONS ¹⁷⁵Lu(¹²C, xn), (¹²C, xnp), (¹²C, xnα), (¹²C, xn2α), (¹³C, xn), (¹³C, xnp), (¹³C, xnα), (¹³C, xn2α), E=4-8 MeV/nucleon; measured Eγ, Iγ, γγ-coin; deduced residues, γ transitions, γ-ray intensity, T_1/2, levels, J, π, σ, α-decay Q value systematics; calculated σ using statistical (Hauser-Feshbach) model code PACE-4; deduced ICF (InComplete Fusion) fraction systematics with projectile-target mass asymmetry.

doi: 10.1016/j.nuclphysa.2017.01.009
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6303.

2017KU29      Phys.Rev. C 96, 054614 (2017)

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

Low-energy nuclear reaction of the ¹⁴N + ¹⁶⁹Tm system: Incomplete fusion

NUCLEAR REACTIONS ¹⁶⁹Tm(¹⁴N, X)¹⁷⁴W/¹⁷⁵W/¹⁷⁶W/¹⁷⁷W/¹⁷⁸Re/¹⁷⁹Re/¹⁷⁹Os, E=76, 78, 80, 83 MeV; measured Eγ, Iγ; deduced complete fusion (CF) σ(E) for 4n-, p3n-, p4n-, α2n-, α3n-, α4n- and α5n-channels, incomplete fusion (ICF) σ(E), and compared with statistical model code PACE4; discussed several other systems for complete and incomplete fusion strength functions and percentage fraction of ICF.

doi: 10.1103/PhysRevC.96.054614
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6325.

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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2015DA01      Nucl.Phys. A933, 123 (2015)

W.A.Dar, J.A.Sheikh, G.H.Bhat, R.Palit, R.N.Ali, S.Frauendorf

Microscopic study of doublet bands in odd-odd A ∼ 100 nuclei

NUCLEAR STRUCTURE ^98,100Tc, ^104,106Rh, ^104,106Ag; calculated negative parity yrast band, energy, J, π, B(M1), B(E2), deformation, triaxial deformation using microscopic triaxial projected shell model. Compared with data.

doi: 10.1016/j.nuclphysa.2014.10.045
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2015KU09      Acta Phys.Pol. B46, 453 (2015)

R.Kumar, V.R.Sharma, A.Yadav, P.P.Singh, S.Appanababu, A.Aggarwal, B.P.Singh, S.Mukherjee, S.Muralithar, R.Ali, R.K.Bhowmik

Low Energy Incomplete Fusion and the Role of Input Angular Momenta

NUCLEAR REACTIONS ¹⁶⁹Tm(¹⁴N, X), E=4-7 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced σ. Comparison with semi-empirical code MARC.

doi: 10.5506/APhysPolB.46.453
Citations: PlumX Metrics

2014BH01      Nucl.Phys. A922, 150 (2014)

G.H.Bhat, R.N.Ali, J.A.Sheikh, R.Palit

Investigation of doublet-bands in ^{124, 126, 130, 132}Cs odd-odd nuclei using triaxial projected shell model approach

NUCLEAR STRUCTURE ^{124,126,130,132}Cs; calculated rotational bands, triaxial quasiparticle state contribution, B(E2), B(M1) using multi-quasiparticle microscopic triaxial projected shell model (TPSM) approach. Compared to available data.

doi: 10.1016/j.nuclphysa.2013.12.006
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2013SI26      J.Phys.Soc.Jpn. 82, 114201 (2013)

D.Singh, M.A.Ansari, R.Ali, N.P.M.Sathik, B.S.Tomar, M.Ismail

Reaction Mechanism in ¹⁶O Ion Interaction with Light Nuclei ⁴⁵Sc, ⁷⁴Ge and Mass-Asymmetry Effect on Incomplete Fusion Dynamics

NUCLEAR REACTIONS ⁴⁵Sc(¹⁶O, 4np2α)⁴⁸Cr, ⁷⁴Ge(¹⁶O, 4npα)⁸¹Rb, ⁷⁴Ge(¹⁶O, 5np2α)⁷⁶Br, E<120 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with statistical model calculations.

doi: 10.7566/JPSJ.82.114201
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6298.

2012SI03      Nucl.Phys. A879, 107 (2012)

D.Singh, R.Ali, M.Afzal Ansari, B.S.Tomar, M.H.Rashid, R.Guin, S.K.Das

Observation of entrance channel mass-asymmetry effect on incomplete fusion reaction for ²⁰Ne + ¹⁶⁵Ho system

NUCLEAR REACTIONS ¹⁶⁵Ho(²⁰Ne, 3n), (²⁰Ne, 2np), (²⁰Ne, 3np), (²⁰Ne, α), (²⁰Ne, 2nα), (²⁰Ne, 3nα), (²⁰Ne, 4nα), (²⁰Ne, 3npα), (²⁰Ne, 4npα), (²⁰Ne, 6npα), (²⁰Ne, n2pα), (²⁰Ne, 2α), (²⁰Ne, n2α), (²⁰Ne, 2n2α), (²⁰Ne, 3n2α), (²⁰Ne, 4n2α), (²⁰Ne, 3np2α), (²⁰Ne, 3n4α), E=88=165 MeV; measured ER Eγ, Iγ using recoil catcher; deduced direct, cumulative yields, direct σ, ICF σ, total σ, critical angular momentum, mass-asymmetry effect; calculated σ, yields using statistical model with Monte Carlo de-excitation with different level density parameters. ICF fraction compared with literature data for other systems.

doi: 10.1016/j.nuclphysa.2012.01.020
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6181.

2011SI12      Phys.Rev. C 83, 054604 (2011)

D.Singh, R.Ali, M.Afzal Ansari, B.S.Tomar, M.H.Rashid, R.Guin, and S.K.Das

Reaction mechanism in the ²⁰Ne+⁵⁹Co system at 3-7 MeV/nucleon, and observation of entrance-channel mass-asymmetry of the incomplete fusion fraction

NUCLEAR REACTIONS ⁵⁹Co(²⁰Ne, np)⁷⁷Kr, ⁵⁹Co(²⁰Ne, 2np)⁷⁶Kr, ⁵⁹Co(²⁰Ne, n2p)⁷⁶Br, ⁵⁹Co(²⁰Ne, α)⁷⁵Br, ⁵⁹Co(²⁰Ne, nα)^74mBr, ⁵⁹Co(²⁰Ne, npα)⁷³Se, ⁵⁹Co(²⁰Ne, 4npα)⁷⁰Se, ⁵⁹Co(²⁰Ne, n2pα)⁷²As, ⁵⁹Co(²⁰Ne, 2α)⁷¹As, ⁵⁹Co(²⁰Ne, n2α)⁷⁰As, ⁵⁹Co(²⁰Ne, 2n2α)⁶⁹As, ⁵⁹Co(²⁰Ne, np2α)⁶⁹Ge, ⁵⁹Co(²⁰Ne, 3np2α)⁶⁷Ge, ⁵⁹Co(²⁰Ne, 4np2α)⁶⁶Ge, ⁵⁹Co(²⁰Ne, 3α)⁶⁷Ga, ⁵⁹Co(²⁰Ne, n3α)⁶⁶Ga, ⁵⁹Co(²⁰Ne, 2n3α)⁶⁵Ga, ⁵⁹Co(²⁰Ne, 2n4α)⁶¹Cu, E=62-150 MeV; measured Eγ, Iγ, γ-activation methods, production cross sections of evaporation residues in incomplete fusion reactions. Comparison with PACE-2 predictions.

doi: 10.1103/PhysRevC.83.054604
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6185.

2010AL19      J.Phys.(London) G37, 115101 (2010)

R.Ali, D.Singh, M.Afzal Ansari, M.H.Rashid, R.Guin, S.K.Das

Investigation of incomplete fusion in ²⁰Ne + ⁵⁵Mn reactions at 3-8 MeV/nucleon

NUCLEAR REACTIONS ⁵⁵Mn(²⁰Ne, X)⁷⁰Se/⁷⁰As/⁷¹As/⁷²As/⁶⁶Ge/⁶⁷Ge/⁶⁹Ge/⁶⁵Ga/⁶⁶Ga/⁶⁷Ga/⁶³Zn/⁶⁰Cu/⁶¹Cu, E=51-164 MeV; measured reaction products recoils, Eγ, Iγ; deduced σ, angular momentum.Comparison with statistical code PACE-2.

doi: 10.1088/0954-3899/37/11/115101
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6159.

2010SI04      Phys.Rev. C 81, 027602 (2010)

D.Singh, R.Ali, M.Afzal Ansari, K.S.Babu, P.P.Singh, M.K.Sharma, B.P.Singh, R.K.Sinha, R.Kumar, S.Muralithar, R.P.Singh, R.K.Bhowmik

Incomplete fusion dynamics by spin distribution measurements

NUCLEAR REACTIONS ¹²⁴Sn(¹⁶O, X)¹³³Ce/¹³⁴Ce/¹³⁵Ce/¹³³La/¹³⁵La/¹³¹Ba/¹³²Ba/¹³³Ba/^128,130,133Xe/¹³¹Cs/¹²⁷I, E=6.3 MeV/nucleon; measured Eγ, Iγ; deduced spin distributions of evaporation residues formed in xn, pxn, αxn, αpxn and 2αxn reaction channels.

doi: 10.1103/PhysRevC.81.027602
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2009SI10      Phys.Rev. C 79, 054601 (2009)

D.Singh, R.Ali, M.Afzal Ansari, M.H.Rashid, R.Guin, S.K.Das

Reaction mechanisms in the system ²⁰Ne+¹⁶⁵Ho: Measurement and analysis of forward recoil range distributions

NUCLEAR REACTIONS ¹⁶⁵Ho(²⁰Ne, 2np), (²⁰Ne, 3np), (²⁰Ne, α), (²⁰Ne, 2nα), (²⁰Ne, 3npα), (²⁰Ne, 4npα), (²⁰Ne, 6npα), (²⁰Ne, n2pα), (²⁰Ne, 2α), (²⁰Ne, n2α), (²⁰Ne, 2n2α), (²⁰Ne, 3n2α), (²⁰Ne, 4n2α), (²⁰Ne, 3np2α), (²⁰Ne, 3n4α), E=164 MeV; measured Eγ, Iγ, yields, forward recoil range distributions and relative contributions of complete and incomplete fusion channels.

doi: 10.1103/PhysRevC.79.054601
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2008SI05      Chin.J.Phys.(Taiwan) 46, 27 (2008)

D.Singh, M.Afzal Ansari, R.Ali, N.P.M.Sathik, M.Ismail

A Study of Excitation Functions for Some Residues Produced in ¹⁶O+⁷⁴Ge System Below 7 MeV/nucleon

NUCLEAR REACTIONS ⁷⁴Ge(¹⁶O, 4n), (¹⁶O, 2np), (¹⁶O, 3np), (¹⁶O, 4np), (¹⁶O, nα), (¹⁶O, 3nα), (¹⁶O, 2npα), (¹⁶O, 3npα), (¹⁶O, 3n2α), E=60.2-111.6 MeV; measured Eγ, Iγ, cross sections using stacked foil activation.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6092.

2007HA23      Eur.Phys.J. D 44, 439 (2007)

S.-U.Haq, S.Mahmood, M.A.Kalyar, M.Rafiq, R.Ali, M.A.Baig

Photoionization cross section and oscillator strength distribution in the near-threshold region of strontium

ATOMIC PHYSICS Sr(X, X), E not given; measured photoionization cross sections.

doi: 10.1140/epjd/e2007-00219-1
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Note: The following list of authors and aliases matches the search parameter R.Ali: , R.N.ALI