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NSR database version of May 22, 2024.

Search: Author = A.Sood

Found 32 matches.

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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6422.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6434. Data from this article have been entered in the XUNDL database. For more information, click here.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6406.


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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6389.


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
Citations: PlumX Metrics


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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6360.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6310.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6326.


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6310.


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
Citations: PlumX Metrics


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
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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
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2011SO19      Phys.Rev. C 84, 014611 (2011)

A.D.Sood

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
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2010GA17      Phys.Rev. C 82, 014604 (2010)

S.Gautam, A.D.Sood

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
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2010KA31      Phys.Rev. C 82, 054611 (2010)

S.Kaur, A.D.Sood

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
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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)

A.D.Sood, R.K.Puri

Participant-spectator matter at the energy of vanishing flow

doi: 10.1103/PhysRevC.79.064618
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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
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2006SO05      Int.J.Mod.Phys. E15, 899 (2006)

A.D.Sood, R.K.Puri

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
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2006SO06      Phys.Rev. C 73, 067602 (2006)

A.D.Sood, R.K.Puri

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
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2006SO16      Eur.Phys.J. A 30, 571 (2006)

A.D.Sood, R.K.Puri

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
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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
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2004SO12      Phys.Rev. C 69, 054612 (2004)

A.D.Sood, R.K.Puri

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
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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
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2004SO26      Phys.Rev. C 70, 034611 (2004)

A.D.Sood, R.K.Puri

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
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2002SO17      Acta Phys.Hung.N.S. 16, 429 (2002)

A.Sood, R.K.Puri

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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Note: The following list of authors and aliases matches the search parameter A.Sood: , A.D.SOOD