NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = A.Sood Found 32 matches. 2022MA13 Nucl.Phys. A1021, 122421 (2022) I.Majeed Bhat, Mohd.S.M.S.Asnain, V.R.Sharma, A.Yadav, M.K.Sharma, P.P.Singh, D.P.Singh, U.Gupta, R.N.Sahoo, A.Sood, M.Kaushik, R.Kumar, B.P.Singh, R.Prasad Effect of projectile structure on break-up fusion for 14N + 175Lu system at intermediate energies NUCLEAR REACTIONS 175Lu(14N, X)184Pt/185Pt/186Pt/183Ir/184Ir/185Ir/182Os/183Os/181Re/177W/178Ta, E=87.11 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with PACE4 predictions. The Inter University Accelerator, New Delhi, India.
doi: 10.1016/j.nuclphysa.2022.122421
2022MA25 Phys.Rev. C 105, 054607 (2022) I.Majeed Bhat, M.Shuaib, M.S.Asnain, M.K.Sharma, A.Yadav, V.R.Sharma, P.P.Singh, D.P.Singh, S.Gupta, U.Gupta, R.N.Sahoo, A.Sood, M.Kaushik, S.Kumar, R.Kumar, B.P.Singh, R.Prasad Role of precursor nuclei in heavy-ion induced reactions at low energies NUCLEAR REACTIONS 175Lu(14N, 4np), E=79.68, 87.11 MeV; 159Tb(12C, 3np), E=69.15, 77.77 MeV; 159Tb(13C, 4np), E=77.87, 84.59 MeV; measured Eγ, Iγ; deduced σ(E). Separated yields of the isotope produced in the direct reaction from feeding caused by decay of the isotopes from other channels. Pelletron accelerator facility of the Inter-University Accelerator Centre(IUAC), New Delhi. comparison to theoretical estimations. RADIOACTIVITY 184Pt(β+), (EC) [from 175Lu(14N, 5n), E=79.68, 87.11 MeV]; 167Lu(EC) [from 159Tb(13C, 5n), E=77.87, 84.59 MeV; 159Tb(12C, 4n), E=69.15, 77.77 MeV]; measured Eγ, Iγ; deduced T1/2. Comparison to other experimental data.
doi: 10.1103/PhysRevC.105.054607
2021AS08 Phys.Rev. C 104, 034616 (2021) M.S.Asnain, M.Shuaib, I.Majeed, M.K.Sharma, V.R.Sharma, A.Yadav, D.P.Singh, P.P.Singh, U.Gupta, R.N.Sahoo, A.Sood, M.Kaushik, S.Kumar, R.Kumar, B.P.Singh, R.Prasad Effect of non-α-cluster projectile on incomplete-fusion dynamics: Experimental study of the 14N + 181Ta NUCLEAR REACTIONS 181Ta(14N, 3n)192Hg, (14N, 4n)191Hg/191mHg, (14N, 5n)190Hg, (14N, 6n)189Hg/189mHg, (14N, 3np)191Au, (14N, 4np)190Au, (14N, 5np)189Au/189mAu, (14N, 2nα)189Pt, (14N, 4nα)187Pt, (14N, 5nα)186Pt, (14N, 3npα)187Ir, (14N, 4npα)186Ir/186mIr, (14N, 5npα)185Ir, (14N, 4n2α)183Os, (14N, 5np2α)181Re, E=65.53, 67.50, 69.47, 71.54, 73.65, 75.65, 77.08, 79.51, 81.42, 83.05, 85.17, 87.07 MeV; measured off-line Eγ, Iγ, σ(E) for radio-nuclides populated via complete fusion (CF) and/or incomplete fusion (ICF processes) by activation method at the ion-beam facility of the IUAC-New Delhi; deduced total fusion, total complete fusion, and total incomplete fusion σ(E). Comparison with statistical model calculations using PACE4 code. 190Hg; measured nominal half-life from γ-decay curves as an example for the purpose of correct identification of different radioactive nuclei produced through various reaction channels.
doi: 10.1103/PhysRevC.104.034616
2021SO23 J.Phys.(London) G48, 025105 (2021) A.Sood, S.Thakur, A.Sharma, V.R.Sharma, A.Yadav, M.K.Sharma, B.P.Singh, R.Kumar, R.K.Bhowmik, P.P.Singh Disentangling complete and incomplete fusion events in 12C + 169Tm reaction by spin-distribution measurements NUCLEAR REACTIONS 169Tm(12C, X), E=6.7, 7.5 MeV/nucleon; measured reaction products, Eα, Iα, Eγ, Iγ. 176Re, 174Ta, 171Lu; deduced yields, strong entrance-channel dependence of incomplete fusion dynamics.
doi: 10.1088/1361-6471/abc14a
2021SO30 Nucl.Technology 207, s100 (2021) A.Sood, R.A.Forster, B.J.Archer, R.C.Little Neutronics Calculation Advances at Los Alamos: Manhattan Project to Monte Carlo
doi: 10.1080/00295450.2021.1956255
2020MA11 Acta Phys.Pol. B51, 829 (2020) M.Matejska-Minda, P.J.Napiorkowski, R.Kumar, M.Saxena, S.Dutt, A.Agarwal, I.Ahmed, S.Bhattacharya, A.Jhingan, J.Kaur, M.Kicinska-Habior, M.Kumar, S.Kumar, D.Kumar, V.Nanal, R.Palit, N.K.Rai, M.Shuaib, A.Sood, A.Stolarz, T.Trivedi, A.K.Tyagi, R.K.Bhowmik, H.J.Wollersheim Revised Lifetime of the 11/2- State in 45Sc via Coulomb Excitation
doi: 10.5506/APhysPolB.51.829
2020SA32 Phys.Rev. C 102, 024615 (2020) R.N.Sahoo, M.Kaushik, A.Sood, A.Sharma, S.Thakur, Pa.Kumar, M.M.Shaikh, R.Biswas, A.Yadav, M.K.Sharma, J.Gehlot, S.Nath, N.Madhavan, R.G.Pillay, E.M.Kozulin, G.N.Knyazheva, K.V.Novikov, P.P.Singh Role of neutron transfer in sub-barrier fusion NUCLEAR REACTIONS 130Te(35Cl, X), E(cm)=94.0, 95.6, 97.2, 98.8, 100.3, 101.9, 103.5, 105.0 MeV; measured evaporation residues (ERs), ΔE-time spectra, fusion σ(E) using recoil mass separator HIRA at IUAC-New Delhi accelerator facility. Comparison with experimental fusion σ(E) data for 130Te(37Cl, X), and other systems. Coupled-channels analysis using CCFULL code.
doi: 10.1103/PhysRevC.102.024615
2020SO05 Acta Phys.Pol. B51, 775 (2020) A.Sood, P.Kumar, R.N.Sahoo, P.P.Singh, A.Yadav, V.R.Sharma, M.K.Sharma, R.Kumar, R.P.Singh, S.Muralithar, B.P.Singh, R.K.Bhowmik Evidence of Narrow Range High Spin Population in Incomplete Fusion
doi: 10.5506/APhysPolB.51.775
2019MA90 Acta Phys.Pol. B50, 411 (2019) M.Matejska-Minda, R.Kumar, P.J.Napiorkowski, M.Saxena, S.Dutt, A.Agarwal, I.Ahmed, S.Bhattacharya, A.Jhingan, J.Kaur, M.Kicinska-Habior, M.Kumar, S.Kumar, D.Kumar, V.Nanal, R.Palit, N.K.Rai, M.Shuaib, A.Sood, A.Stolarz, T.Trivedi, A.K.Tyagi, R.K.Bhowmik, H.J.Wollersheim Investigation of an Intruder Band in 45Sc via Coulomb Excitation NUCLEAR REACTIONS 45Sc(32S, 32S), E=70 MeV; measured reaction products, Eγ, Iγ, (particle)γ-coin, γγ-coin; deduced γ-ray transitions, levels, J, π.
doi: 10.5506/aphyspolb.50.411
2019SA15 Nucl.Phys. A983, 145 (2019) R.N.Sahoo, M.Kaushik, A.Sood, P.Kumar, V.R.Sharma, A.Yadav, P.P.Singh, M.K.Sharma, R.Kumar, B.P.Singh, S.Aydin, R.Prasad Insights into the low energy incomplete fusion NUCLEAR REACTIONS 169Tm(12C, x), E(cm)=52.98 - 89.25 MeV; measured Eγ, Iγ(t); deduced production σ of evaporation residues. 169Tm(12C, x), E=52.98 - 89.25 MeV;160Gd(12C, x), Ei(cm)=83.7 MeV;103Rh(16O, x), 159Tb(16O, x), E not given; calculated ER production σ using PACE4 and with different level density parameters and using CCFULL; deduced potential parameters, radius parameter from the fit to the data, variation of incomplete fusion fraction with neutron skin thickness and with angular momentum.
doi: 10.1016/j.nuclphysa.2018.12.013
2019SA17 Phys.Rev. C 99, 024607 (2019) R.N.Sahoo, M.Kaushik, A.Sood, P.Kumar, A.Sharma, S.Thakur, P.P.Singh, P.K.Raina, M.M.Shaikh, R.Biswas, A.Yadav, J.Gehlot, S.Nath, N.Madhavan, V.Srivastava, M.K.Sharma, B.P.Singh, R.Prasad, A.Rani, A.Banerjee, U.Gupta, N.K.Deb, B.J.Roy Sub-barrier fusion in the 37Cl + 130Te system NUCLEAR REACTIONS 130Te(37Cl, X), E=121-155 MeV; measured reaction products, evaporation residues, time of flight of evaporation residue, fusion σ(E) using the HIRA recoil mass spectrometer at the 15UD Pelletron accelerator of IUAC-New Delhi; deduced fusion barrier distributions, astrophysical S factor, logarithmic derivative L(E) factor. Comparison with coupled-channels code calculations using CCFULL code. Systematics of reduced fusion excitation functions of 37Cl projectiles on 58,60,62,64Ni, 130Te targets at sub-barrier energies.
doi: 10.1103/PhysRevC.99.024607
2019SO21 Acta Phys.Pol. B50, 291 (2019) A.Sood, P.Kumar, R.N.Sahoo, P.P.Singh, A.Yadav, V.R.Sharma, M.K.Sharma, D.P.Singh, U.Gupta, S.Aydin, R.Kumar, B.P.Singh, R.Prasad Entrance Channel Effects on Fission Fragment Mass Distribution in 12C + 169Tm System NUCLEAR REACTIONS 169Tm(12C, X), E= 77.18, 83.22, 89.25 MeV; measured Eγ, Iγ(t); deduced production σ of evaporation residues, isotopic yieldsmass distribution of fission fragments.
doi: 10.5506/aphyspolb.50.291
2018SA38 Acta Phys.Pol. B49, 585 (2018) R.N.Sahoo, M.Kaushik, A.Sood, P.Kumar, V.R.Sharma, A.Yadav, M.Shuaib, D.P.Singh, P.P.Singh, U.Gupta, M.K.Sharma, R.Kumar, B.P.Singh, S.Aydin, H.J.Wollersheim, R.Prasad Entrance Channel Effect on Incomplete Fusion NUCLEAR REACTIONS 169Tm(12C, x), E=5-7.5 MeV/nucleon; measured evaporation residues (ER) Eγ, Iγ(time); deduced 177Re σER; calculated σER using statistical model code PACE-IV with different level density parameter; calculated total (summed over all ERs) σT, complete and incomplete fusion σCF, σICF. 103Rh, 115In, 159Tb, 169Tm, 197Au(12C, x), E not given;103Rh, 159Tb, 169Tm(16O, x), E not given; measured reaction products Eγ, Iγ; deduced incomplete fusion fraction vs mass asymmetry (relative projectile-target velocity close to 0.05c vs asymmetry).
doi: 10.5506/aphyspolb.49.585
2018TA05 Eur.Phys.J. A 54, 9 (2018) P.Talou, R.Vogt, J.Randrup, M.E.Rising, S.A.Pozzi, J.Verbeke, M.T.Andrews, S.D.Clarke, P.Jaffke, M.Jandel, T.Kawano, M.J.Marcath, K.Meierbachtol, L.Nakae, G.Rusev, A.Sood, I.Stetcu, C.Walker Correlated prompt fission data in transport simulations COMPILATION 235U, 239Pu(n, F), E=thermal;252Cf(SF); compiled average prompt fission neutron multiplicity vs fragment mass, prompt fission neutron σ(En), γ-decay energy spectrum σ(Eγ), γ multiplicity, n-n angular correlation. Calculated σ, yields using FREYA and CGMF codes. Compared with data.
doi: 10.1140/epja/i2018-12455-0
2017SO12 Phys.Rev. C 96, 014620 (2017) A.Sood, P.P.Singh, R.N.Sahoo, P.Kumar, A.Yadav, V.R.Sharma, Mohd.Shuaib, M.K.Sharma, D.P.Singh, U.Gupta, R.Kumar, S.Aydin, B.P.Singh, H.J.Wollersheim, R.Prasad Fission-like events in the 12C + 169Tm system at low excitation energies NUCLEAR REACTIONS 169Tm(12C, X)74mBr/74Kr/75Br/75Ge/75Kr/76Kr/77Kr/78As/79Rb/81Sr/84Br/85Zr/86Y/87Zr/89Rb/93Y/94Ru/95Ru/97Nb/98mNb/101Tc/102mTc/104Tc/104Ag/105Tc/105In/175Re/176Re/177Re/178Re/177W/173Ta/174Ta/175Ta/176Ta/171Lu, E=77.81, 83.22, 89.25 MeV; measured Eγ, Iγ, recoil-catcher activation technique, half-life of 74Kr decay, production σ(E) of fission products and evaporation residues, charge and mass distribution of fission fragments at the pelletron accelerator facility of IUAC-New Delhi; deduced fission as one of the competing modes of deexcitation of complete and/or incomplete fusion composites at low excitation energies. Comparison with calculations using PACE code. 181Ta(16O, X), E*=67.04 MeV; 159Tb(16O, X), E*=57.1 MeV; 169Tm(16O, X), E*=61.06 MeV; 232Th(7Li, X), E*=41.7 MeV; 232Th(11B, X), E*=55.7 MeV; 238U(11B, X), E*=67.4 MeV; 238U(22Ne, X), E*=64.5 MeV; 208Pb(20Ne, X), E*=46.4 MeV; analyzed previous experimental data for isotopic yield distributions.
doi: 10.1103/PhysRevC.96.014620
2014CH44 Nucl.Data Sheets 118, 558 (2014) A.Chapelle, P.Casoli, N.Authier, W.Myers, J.Hutchinson, A.Sood, B.Rooney Joint Neutron Noise Measurements on Metallic Reactor Caliban
doi: 10.1016/j.nds.2014.04.134
2011GA03 Phys.Rev. C 83, 014603 (2011) S.Gautam, A.D.Sood, R.K.Puri, J.Aichelin Isospin effects in the disappearance of flow as a function of colliding geometry NUCLEAR REACTIONS 24Mg(24Mg, X), 24Ne(24Ne, X), 58Cu(58Cu, X), 58Cr(58Cr, X), 72Kr(72Kr, X), 72Zn(72Zn, X), 96Cd(96Cd, X), 96Zr(96Zr, X), 120Nd(120Nd, X), 120Sn(120Sn, X), 135Ho(135Ho, X), 135Ba(135Ba, X), E=40-340 MeV/nucleon; calculated energy of vanishing flow, impact parameter dependence for isobaric pairs in A=48-270 region and N/Z=1.0 and 1.4; deduced dominance of Coulomb potential over symmetry energy. Isospin-dependent quantum molecular dynamics (IQMD) model.
doi: 10.1103/PhysRevC.83.014603
2011GA13 Phys.Rev. C 83, 034606 (2011) S.Gautam, A.D.Sood, R.K.Puri, J.Aichelin Sensitivity of the transverse flow to the symmetry energy NUCLEAR REACTIONS 40Ca(40Ca, X), 48Ca(48Ca, X), 60Ca(60Ca, X), E=100, 400, 800 MeV/nucleon; calculated time evolution of rms radius and rapidity distributions, transverse flow to symmetry energies using isospin-dependent quantum molecular dynamics model (IQMD).
doi: 10.1103/PhysRevC.83.034606
2011SO19 Phys.Rev. C 84, 014611 (2011) N/Z and N/A dependence of the balance energy as a probe of the symmetry energy in heavy-ion collisions NUCLEAR REACTIONS 40Ca(40Ca, X), 44Ca(44Ca, X), 48Ca(48Ca, X), 52Ca(52Ca, X), 56Ca(56Ca, X), 60Ca(60Ca, X), E AP balance energy; calculated N/Z and N/A dependence of balance energy, and effect of momentum-dependent interactions. Isospin-dependent quantum molecular dynamics (IQMD) model.
doi: 10.1103/PhysRevC.84.014611
2010GA17 Phys.Rev. C 82, 014604 (2010) Isospin effects on the mass dependence of the balance energy NUCLEAR REACTIONS 24Ne(24Ne, X), 24Mg(24Mg, X), 26Mg(26Mg, X), 28Mg(28Mg, X), 58Cr(58Cr, X), 58Fe(58Fe, X), 58Ni(58Ni, X), 58Cu(58Cu, X), 65Zn(65Zn, X), 70Zn(70Zn, X), 72Zn(72Zn, X), 72Kr(72Kr, X), 96Zr(96Zr, X), 91Mo(91Mo, X), 98Mo(98Mo, X), 96Cd(96Cd, X), 120Sn(120Sn, X), 117Xe(117Xe, X), 126Xe(126Xe, X), 135Ba(135Ba, X), 120Nd(120Nd, X), 135Ho(135Ho, X), 164Os(164Os, X), 177Os(177Os, X), E=40-150 MeV/nucleon; calculated (Ebal) or energy of vanishing flow (EVF) as a function of combined mass of pairs of isotopic and isobaric systems using isospin-dependent quantum molecular dynamics (IQMD) model. Dominance of Coulomb repulsion over the symmetry energy.
doi: 10.1103/PhysRevC.82.014604
2010KA31 Phys.Rev. C 82, 054611 (2010) Model ingredients and peak mass production in heavy-ion collisions NUCLEAR REACTIONS 20Ne(20Ne, X), E=10-55 MeV/nucleon; 45Sc(40Ar, X), E=35-115 MeV/nucleon; 58Ni(58Ni, X), E=35-105 MeV/nucleon; 93Nb(86Kr, X), E=35-95 MeV/nucleon; 118Sn(129Xe, X), E=45-140 MeV; 197Au(86Kr, X), E=35-400 MeV; 197Au(197Au, X), E=70-150 MeV/nucleon; calculated time evolution of intermediate mass fragments (IMF), mean IMF multiplicity, multiplicities of free nucleons, LCPs, MMFs, HMFs, and IMFs as a function of composite mass of the colliding nuclei, binding energies/nucleon for different fragments using quantum molecular dynamics (QMD) model at different incident energies for different equations of state, different binary cross sections, and different widths of Gaussians. Comparison with experimental data.
doi: 10.1103/PhysRevC.82.054611
2010VE07 Ukr.J.Phys. 55, 1071 (2010) Y.K.Vermani, R.Chugh, A.D.Sood Probing Nuclear Compressibility Via Fragmentation in Au+Au Reactions at 35A MeV NUCLEAR REACTIONS 197Au(197Au, X), E=35 MeV/nucleon; calculated mean nucleon density, multiplicity, rapidity distribution, impact parameter dependence. QMD model.
2009SO11 Phys.Rev. C 79, 064618 (2009) Participant-spectator matter at the energy of vanishing flow
doi: 10.1103/PhysRevC.79.064618
2006DH06 Phys.Rev. C 74, 057901 (2006) J.K.Dhawan, N.Dhiman, A.D.Sood, R.K.Puri From fusion to total disassembly: Global stopping in heavy-ion collisions NUCLEAR REACTIONS 20Ne(20Ne, X), 40Ca(40Ca, X), 58Ni(58Ni, X), 93Nb(93Nb, X), 139La(139La, X), 197Au(197Au, X), E=400 MeV/nucleon; calculated light charged particle and intermediate mass fragments rapidity distributions, anisotropy ratios, stopping features. Quantum molecular dynamics model.
doi: 10.1103/PhysRevC.74.057901
2006SO05 Int.J.Mod.Phys. E15, 899 (2006) The study of participant-spectator matter and collision dynamics in heavy-ion collisions NUCLEAR REACTIONS 40Ca(40Ca, X), E=200 MeV/nucleon; 131Xe(131Xe, X), E=400 MeV/nucleon; calculated time evolution of nucleon trajectories, related features. Participant-spectator model.
doi: 10.1142/S0218301306004685
2006SO06 Phys.Rev. C 73, 067602 (2006) Systematic study of the energy of vanishing flow: Role of equations of state and cross sections NUCLEAR REACTIONS 12C(12C, X), 20Ne(20Ne, X), 40Ca(40Ca, X), 58Ni(58Ni, X), 93Nb(93Nb, X), 131Xe(131Xe, X), 197Au(197Au, X), 238U(238U, X), E ≈ 40-140 MeV; analyzed energy of vanishing flow. Several models compared.
doi: 10.1103/PhysRevC.73.067602
2006SO16 Eur.Phys.J. A 30, 571 (2006) Influence of momentum-dependent interactions on balance energy and mass dependence NUCLEAR REACTIONS 12C(12C, X), 27Al(20Ne, X), (36Ar, X), 27Al, 45Sc, 51V, 58Ni(40Ar, X), 48Ti, 58Ni(64Zn, X), 58Ni(58Ni, X), 93Nb(86Kr, X), (93Nb, X), Sn(129Xe, X), 139La(139La, X), 197Au(197Au, X), E ≈ 0-800 MeV/nucleon; calculated directed transverse momentum, related features; deduced role of momentum-dependent interactions.
doi: 10.1140/epja/i2006-10143-4
2004FO11 Nucl.Instrum.Methods Phys.Res. B213, 82 (2004) R.A.Forster, L.J.Cox, R.F.Barrett, T.E.Booth, J.F.Briesmeister, F.B.Brown, J.S.Bull, G.C.Geisler, J.T.Goorley, R.D.Mosteller, S.E.Post, R.E.Prael, E.C.Selcow, A.Sood MCNPTM Version 5
doi: 10.1016/S0168-583X(03)01538-6
2004SO12 Phys.Rev. C 69, 054612 (2004) Mass dependence of disappearance of transverse in-plane flow NUCLEAR REACTIONS 27Al(20Ne, X), (36Ar, X), (40Ar, X), 45Sc, 51V, 58Ni(40Ar, X), 48Ti(64Zn, X), 58Ni(58Ni, X), (64Zn, X), 93Nb(86Kr, X), (93Nb, X), Sn(129Xe, X), 139La(139La, X), 197Au(197Au, X), E ≈ 30-150 MeV/nucleon; calculated directed transverse in-plane flow, balance energy. Quantum molecular dynamics, comparison with data.
doi: 10.1103/PhysRevC.69.054612
2004SO18 Phys.Lett. B 594, 260 (2004) A.D.Sood, R.K.Puri, J.Aichelin Study of balance energy in central collisions for heavier nuclei NUCLEAR REACTIONS 93Nb(93Nb, X), 139La(139La, X), 197Au(197Au, X), 238U(238U, X), E=35-80 MeV/nucleon; calculated particles average transverse momentum vs time, disappearance of flow, balance energy. Quantum molecular dynamics model.
doi: 10.1016/j.physletb.2004.05.053
2004SO26 Phys.Rev. C 70, 034611 (2004) Nuclear dynamics at the balance energy NUCLEAR REACTIONS 27Al(20Ne, X), (36Ar, X), 27Al, 45Sc, 51V, 58Ni(40Ar, X), 48Ti(64Zn, X), 58Ni, (58Ni, X), (64Zn, X), 93Nb(86Kr, X), (93Nb, X), Sn(129Xe, X), 139La(139La, X), 197Au(197Au, X), E ≈ 40-120 MeV; calculated average and maximum density, temperature, participant-spectator ratios, related features. Quantum molecular dynamics model.
doi: 10.1103/PhysRevC.70.034611
2002SO17 Acta Phys.Hung.N.S. 16, 429 (2002) Study of Equilibrium Using Collision Dynamics NUCLEAR REACTIONS Ca(Ca, X), Sn(Xe, X), Au(197Au, X), E=400 MeV/nucleon; calculated particle rapidity distributions vs centrality; deduced thermalization features. Dynamical quantum molecular dynamics model.
doi: 10.1556/APH.16.2002.1-4.45
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