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NSR database version of May 24, 2024.

Search: Author = A.K.Mohanty

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2021PA41      Phys.Lett. B 823, 136760 (2021)

D.Pandit, D.Mondal, T.K.Ghosh, S.Mukhopadhyay, S.Pal, A.Sen, A.K.Saha, V.N.Jha, S.Saha, C.Bhattacharya, A.K.Mohanty

Search for coherent bremsstrahlung from spontaneous fission at 555 meter deep underground laboratory

RADIOACTIVITY 252Cf(SF); measured decay products, Eγ, Iγ, γ-γ-coin.; deduced a new upper limit for γ-ray emission from the nucleus-nucleus coherent bremsstrahlung in 25-180 MeV energy region, which is two orders of magnitude lower than the previous value.

doi: 10.1016/j.physletb.2021.136760
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33167.

2020SU11      Eur.Phys.J. A 56, 80 (2020)

V.Suman, C.Sunil, S.Pal, V.Nanal, K.Biju, R.G.Thomas, A.K.Mohanty

Double differential neutron yield from 12C incident on thick 12C target at 116 MeV

doi: 10.1140/epja/s10050-020-00082-3
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6381.

2017PA36      Phys.Rev. C 96, 044607 (2017)

S.Paul, C.Sunil, S.Pal, V.Nanal, V.Suman, G.S.Sahoo, A.Shanbhag, S.P.Tripathy, T.Bandyopadhyay, M.Nandy, A.K.Mohanty

Preequilibrium neutron emission from O + Al at 7.5 MeV/nucleon and 8.8 MeV/nucleon

NUCLEAR REACTIONS 27Al(16O, X), E=120, 142 MeV; measured neutron and γ spectra, σ(θ, E) for neutrons, thick target neutron yields at Pelletron-Linac facility in Mumbai; analyzed data in the framework of evaporation and the preequilibrium (PEQ) reaction models PACE4, EMPIRE 3.2, and HION.

doi: 10.1103/PhysRevC.96.044607
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6321.

2016GA05      Eur.Phys.J. A 52, 27 (2016)

P.Garg, D.K.Mishra, P.K.Netrakanti, A.K.Mohanty

Multiplicity fluctuations in heavy-ion collisions using canonical and grand-canonical ensemble

doi: 10.1140/epja/i2016-16027-0
Citations: PlumX Metrics

2016MI15      Phys.Rev. C 94, 014905 (2016)

D.K.Mishra, P.Garg, P.K.Netrakanti, A.K.Mohanty

Effect of resonance decay on conserved number fluctuations in a hadron resonance gas model

doi: 10.1103/PhysRevC.94.014905
Citations: PlumX Metrics

2016PA33      Phys.Rev. C 94, 034607 (2016)

S.Paul, M.Nandy, A.K.Mohanty, Y.K.Gambhir

Preequilibrium neutron emission in heavy ion reaction: Mean field effect and multiple emission

NUCLEAR REACTIONS 165Ho(20Ne, X)185Ir*, E=220, 292, 402, 600 MeV; 165Ho(12C, X)177Ta*, E=300 MeV/nucleon; calculated neutron emission probabilities and neutron multiplicities; deduced percentage contribution of Preequilibrium (PEQ) emission. Comparison with experimental data. 177Ta, 185Ir; calculated neutron, proton and total density distributions using semiphenomenological and RMF approaches. Semiclassical formalism for heavy ion reaction with nuclear density distribution from relativistic mean field (RMF) approach.

doi: 10.1103/PhysRevC.94.034607
Citations: PlumX Metrics

2015PA25      Nucl.Phys. A940, 167 (2015)

A.Parmar, Sonika, B.J.Roy, V.Jha, U.K.Pal, T.Sinha, S.K.Pandit, V.V.Parkar, K.Ramachandran, K.Mahata, S.Santra, A.K.Mohanty

Understanding the two neutron transfer reaction mechanism in 206Pb(18O, 16O)208Pb

NUCLEAR REACTIONS 206Pb(18O, 18O), (18O, 16O), E=79 MeV; measured E(16,18O), I(16,18O, θ) using SSB's (silicon surface barrier) telescopes; deduced σ(θ), one- and two-nucleon transfer probability; calculated σ(θ) using FRES 2.9 CC code.

doi: 10.1016/j.nuclphysa.2015.04.004
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6262.

2015SO17      Phys.Rev. C 92, 024603 (2015)

Sonika, B.J.Roy, A.Parmar, U.K.Pal, H.Kumawat, V.Jha, S.K.Pandit, V.V.Parkar, K.Ramachandran, K.Mahata, A.Pal, S.Santra, A.K.Mohanty, K.Sekizawa

Multinucleon transfer study in 206Pb(18O, x) at energies above the Coulomb barrier

NUCLEAR REACTIONS 206Pb(18O, 20O), (18O, 19O), (18O, 17O), (18O, 16O), (18O, 18N), (18O, 17N), (18O, 16N), (18O, 15N), (18O, 14N), (18O, 16C), (18O, 15C), (18O, 14C), (18O, 13C), (18O, 12C), (18O, 12B), (18O, 11B), (18O, 10B), (18O, 10Be), (18O, 9Be), (18O, 18O)E=139 MeV; measured particle spectra, elastic σ(θ), total kinetic energy loss (TKEL) spectra, angular distributions at Pelletron-LINAC accelerator of BARC-TIFR facility; deduced Q values and angle integrated cross sections. Comparison with fully microscopic time-dependent Hartree-Fock (TDHF) calculations, based on the independent single-nucleon transfer mode. Discussed effect of particle evaporation on the production cross sections, and possible origin of discrepancies.

doi: 10.1103/PhysRevC.92.024603
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6264.

2015YA12      Phys.Rev. C 92, 014611 (2015)

C.Yadav, R.G.Thomas, A.K.Mohanty, S.S.Kapoor

Deduction of compound nucleus formation probability from the fragment angular distributions in heavy-ion reactions

NUCLEAR REACTIONS 182W(32S, X)214Th*, 197Au(18O, X)215Fr*, 197Au(26Mg, X)223Pa*, 197Au(30Si, X)227Np*, 197Au(32S, X)229Am*, 197Au(36S, X)233Am*, 204Pb(11B, X)215Fr*, 208Pb(16O, X)224Th*, 208Pb(19F, X)227Pa*, 208Pb(24Mg, X)232Pu*, 208Pb(28Si, X)236Cm*, 208Pb(32S, X)240Cf*, 232Th(12C, X)244Cm*, 232Th(16O, X)248Cf*, 238U(16O, X)254Fm*, E(cm)/Vb-1.05-1.24 MeV; analyzed fragment angular distributions, mass asymmetry, compound nucleus fissility, and effective fissility; deduced PCN the probability of compound nucleus formation. Pre-equilibrium fission formalism. Relevance to heavy-element formation cross sections.

doi: 10.1103/PhysRevC.92.014611
Citations: PlumX Metrics

2013GA14      J.Phys.(London) G40, 055103 (2013)

P.Garg, D.K.Mishra, P.K.Netrakanti, A.K.Mohanty, B.Mohanty

Unfolding of event-by-event net-charge distributions in heavy-ion collision

doi: 10.1088/0954-3899/40/5/055103
Citations: PlumX Metrics

2012CR01      Ann.Nucl.Energy 47, 160 (2012)

R.Crasta, H.Naik, S.V.Suryanarayana, B.S.Shivashankar, V.K.Mulik, P.M.Prajapati, G.Sanjeev, S.C.Sharma, P.V.Bhagwat, A.K.Mohanty, S.Ganesan, A.Goswami

Measurement of the 232Th(n, γ)233Th and 232Th(n, 2n)231Th reaction cross-sections at neutron energies of 8.04 ± 0.30 and 11.90 ± 0.35 MeV

NUCLEAR REACTIONS 232Th(n, γ), (n, 2n), E=8.04, 11.9 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with available data, ENDF/B-VII.0 and JENDL-4.0 evaluated nuclear libraries, TALYS nuclear model code calculations.

doi: 10.1016/j.anucene.2012.02.010
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33042.

2012KU22      Phys.Rev. C 86, 024607 (2012)

H.Kumawat, V.Jha, V.V.Parkar, B.J.Roy, S.K.Pandit, R.Palit, P.K.Rath, C.S.Palshetkar, SushilK.Sharma, S.Thakur, A.K.Mohanty, A.Chatterjee, S.Kailas

Fusion reaction studies for the 6Li + 90Zr system at near-barrier energies

NUCLEAR REACTIONS 90Zr(6Li, X)90Nb/93mMo/93Tc/93mTc/94Tc/94mTc/95Tc/95mTc, E=13-30 MeV; measured Eγ, Iγ, fusion σ(E) for ground states and isomers. Comparisons with CASCADE, CDCC-1DBPM, BPM+breakup coupling, and absorption model calculations.

doi: 10.1103/PhysRevC.86.024607
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6200.

2010KU10      Phys.Rev. C 81, 054601 (2010)

H.Kumawat, V.Jha, V.V.Parkar, B.J.Roy, S.Santra, V.Kumar, D.Dutta, P.Shukla, L.M.Pant, A.K.Mohanty, R.K.Choudhury, S.Kailas

Inclusive α-production cross section for the 6Li + 90Zr system at energies near the fusion barrier

NUCLEAR REACTIONS 90Zr(6Li, X), E=15, 17, 19, 21, 25, 30 MeV; measured α-spectra, σ and σ(θ). Comparison with DWBA and statistical model calculations.

doi: 10.1103/PhysRevC.81.054601
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6109.

2008KU16      Phys.Rev. C 78, 044617 (2008)

H.Kumawat, V.Jha, B.J.Roy, V.V.Parkar, S.Santra, V.Kumar, D.Dutta, P.Shukla, L.M.Pant, A.K.Mohanty, R.K.Choudhury, S.Kailas

Breakup threshold anomaly in the elastic scattering for the 6Li + 90Zr system

NUCLEAR REACTIONS 90Zr(6Li, 6Li), E=11, 12, 13, 14, 15, 17, 19, 21, 25, 30 MeV; measured angular distributions, σ, optical potentials, normalization factors. Comparison with Continuum Discretized Coupled Channels calculations.

doi: 10.1103/PhysRevC.78.044617
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6068.

2005SA19      Pramana 64, 47 (2005)

S.V.S.Sastry, S.Kailas, A.K.Mohanty, A.Saxena

Adiabatic heavy-ion fusion potentials for fusion at deep sub-barrier energies

NUCLEAR REACTIONS 58,62,64Ni(28Si, X), 58,64Ni(32S, X), (58Ni, X), 58,64Ni, 90,96Zr(36S, X), 112,116,122Sn, 144,148,154Sm(40Ar, X), 90Zr, 93Nb(46Ti, X), (50Ti, X), 64Ni, 100Mo(64Ni, X), 89Y(60Ni, X), 70,76Ge(86Kr, X), E not given; calculated fusion barrier parameters. 58Ni(58Ni, X), E(cm) ≈ 90-110 MeV; 89Y(60Ni, X), E(cm) ≈ 120-140 MeV; calculated fusion excitation functions. Barrier penetration model.

doi: 10.1007/BF02704529
Citations: PlumX Metrics

2003DU14      Pramana 60, 1079 (2003)

D.Dutta, S.V.S.Sastry, A.K.Mohanty, K.Kumar, R.K.Choudhury

Photon production from quark gluon plasma at finite baryon density

NUCLEAR REACTIONS Pb(Pb, X), E=high; analyzed photon yields, sensitivity to baryon density.

doi: 10.1007/BF02707034
Citations: PlumX Metrics

2003SH24      Pramana 60, 1117 (2003)

P.Shukla, A.K.Mohanty

Spinodal decomposition: An alternate mechanism of phase conversion

doi: 10.1007/BF02707042
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2003TH02      Phys.Rev. C 67, 041601 (2003)

R.G.Thomas, R.K.Choudhury, A.K.Mohanty, A.Saxena, S.S.Kapoor

Fission fragment angular distributions: A probe to study heavy-ion fusion dynamics

NUCLEAR REACTIONS 232Th, 238U(16O, F), E(cm) ≈ 70-120 MeV; 232Th(12C, F), (10B, F), (11B, F), E(cm) ≈ 40-80 MeV; 235,236,238U(12C, F), E(cm) ≈ 50-90 MeV; analyzed fission fragment angular distributions, anisotropy; deduced role of pre-equilibrium fission, related reaction mechanism features.

doi: 10.1103/PhysRevC.67.041601
Citations: PlumX Metrics

2002DU17      Nucl.Phys. A710, 415 (2002)

D.Dutta, S.V.S.Sastry, A.K.Mohanty, K.Kumar

Hard photon production from unsaturated quark-gluon plasma at two-loop level

doi: 10.1016/S0375-9474(02)01166-1
Citations: PlumX Metrics

2002MO10      Phys.Rev. C65, 034908 (2002)

A.K.Mohanty, P.Shukla, M.Gleiser

Nonperturbative Effects in a Rapidly Expanding Quark Gluon Plasma

doi: 10.1103/PhysRevC.65.034908
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2001SH37      Phys.Rev. C64, 054910 (2001)

P.Shukla, A.K.Mohanty

Nucleation versus Spinodal Decomposition in a First Order Quark Hadron Phase Transition

doi: 10.1103/PhysRevC.64.054910
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2001SK01      Phys.Rev. D63, 014012 (2001)

P.Skukla, A.K.Mohanty, S.K.Gupta

Dynamical Growth of the Hadron Bubbles during the Quark-Hadron Phase Transition

doi: 10.1103/PhysRevD.63.014012
Citations: PlumX Metrics

2000DU02      Phys.Rev. C61, 034902 (2000)

D.Dutta, A.K.Mohanty, K.Kumar, R.K.Choudhury

Dissipative Phenomena in a Chemically Nonequilibrated Quark Gluon Plasma

doi: 10.1103/PhysRevC.61.034902
Citations: PlumX Metrics

2000DU13      Phys.Rev. C61, 064911 (2000)

D.Dutta, A.K.Mohanty, K.Kumar, R.K.Choudhury

Effect of Baryon Density on Parton Production, Chemical Equilibration, and Thermal Photon Emission from the Quark Gluon Plasma

doi: 10.1103/PhysRevC.61.064911
Citations: PlumX Metrics

2000SH43      Phys.Rev. C62, 054904 (2000)

P.Shukla, A.K.Mohanty, S.K.Gupta, M.Gleiser

Inhomogeneous Nucleation in a Quark-Hadron Phase Transition

doi: 10.1103/PhysRevC.62.054904
Citations: PlumX Metrics

1999DU07      Phys.Rev. C60, 014905 (1999)

D.Dutta, K.Kumar, A.K.Mohanty, R.K.Choudhury

Chemical Equilibration and Thermal Dilepton Production from the Quark Gluon Plasma at Finite Baryon Density

doi: 10.1103/PhysRevC.60.014905
Citations: PlumX Metrics

1999SA32      Phys.Rev. C60, 024610 (1999)

S.Santra, A.K.Mohanty, P.Singh

Effect of Long Range Absorption on Upper Fusion Barriers

NUCLEAR REACTIONS 144Sm(16O, X), E(cm)=55-75 MeV; 92Zr(16O, X), E(cm)=35-50 MeV;calculated fusion σ, barrier distributions; deduced long-range absorption, channel coupling effects. Optical model, barrier penetration model.

doi: 10.1103/PhysRevC.60.024610
Citations: PlumX Metrics

1999SH10      Phys.Rev. C59, 914 (1999); Erratum Phys.Rev. C62, 039901 (2000)

P.Shukla, S.K.Gupta, A.K.Mohanty

Supercooling in Viscous Hydrodynamics for QCD Phase Transition

doi: 10.1103/PhysRevC.59.914
Citations: PlumX Metrics

1997SA44      Phys.Rev. C56, 1516 (1997)

S.V.S.Sastry, A.K.Mohanty, S.K.Kataria

Effect of Nonlocality on Sub-Barrier Fusion Enhancement

NUCLEAR REACTIONS, ICPND 154Sm(16O, X), E(cm)=40-80 MeV; 154Sm(28Si, X), E(cm)=80-160 MeV; 64Ni(58Ni, X), E(cm)=80-110 MeV; 232Th(19F, X), E(cm)=50-130 MeV; analyzed fusion σ, average spin using several models; deduced no fusion enhancement with barrier penetration model plus nonlocal potential.

doi: 10.1103/PhysRevC.56.1516
Citations: PlumX Metrics

1996MO01      Phys.Rev. C53, 887 (1996)

A.K.Mohanty, S.K.Kataria

Hadronization During Quark-Gluon Plasma Phase Transition

doi: 10.1103/PhysRevC.53.887
Citations: PlumX Metrics

1996SA35      Phys.Rev. C54, 3286 (1996)

S.V.S.Sastry, S.K.Kataria, A.K.Mohanty, I.J.Thompson

Optical Model Approach for Heavy Ion Fusion

NUCLEAR REACTIONS, ICPND 208Pb(16O, 16O), (16O, X), E=80-102 MeV; calculated reaction, fusion σ(E); deduced WKB transmission, optical model approaches differences related features. Coupled reaction channels method.

doi: 10.1103/PhysRevC.54.3286
Citations: PlumX Metrics

1995SA53      Pramana 44, 153 (1995)

S.V.S.Sastry, A.K.Mohanty, S.K.Kataria

A New Approach for Heavy Ion Fusion Spin Distribution

NUCLEAR REACTIONS 130Te(32S, 32S), E=108, 128 MeV; calculated σ(θ). 152Sm(16O, X), E=72 MeV; 208Pb(16O, X), E=80, 90 MeV; 232Th(16O, X), E=83, 105 MeV; calculated σ vs L. 232Th(16O, X), E=80-107 MeV; calculated fusion, reaction σ(E).

doi: 10.1007/BF02847695
Citations: PlumX Metrics

1994MO32      Phys.Rev.Lett. 73, 2672 (1994)

A.K.Mohanty, S.K.Kataria

Intermittency in Quark-Gluon-Plasma Phase Transition

doi: 10.1103/PhysRevLett.73.2672
Citations: PlumX Metrics

1994MO40      Pramana 43, 319 (1994)

A.K.Mohanty, S.K.Kataria

Distribution of Fusion Barriers

NUCLEAR REACTIONS 154,148,144Sm, 122Sn(40Ar, X), 92Zr, 154,152,150Sm(16O, X), 64,58Ni(58Ni, X), 64Ni(64Ni, X), 64Ni(32S, X), 68Zn(28Si, X), 59Co(37Cl, X), 51V(45Sc, X), 74Ge(74Ge, X), E not given; analyzed fusion σ(E) data.

doi: 10.1007/BF02846848
Citations: PlumX Metrics

1993MO12      Phys.Rev. C48, 1445 (1993)

A.K.Mohanty, S.K.Kataria, M.S.Samant

Effect of Channel Coupling on Spin Distribution at and above Coulomb Barrier Energies

NUCLEAR REACTIONS 154Sm(16O, X), E=58-68 MeV; 122Sn(40Ar, X), E=108, 113 MeV; 100Mo(64Ni, X), E=130.1, 141.7 MeV; 152Sm(16O, X), E=60, 80 MeV; calculated fusion partial σ energy, l dependence; deduced channel coupling role in spin distribution.

doi: 10.1103/PhysRevC.48.1445
Citations: PlumX Metrics

1993SA53      Pramana 41, 525 (1993)

S.V.S.Sastry, A.K.Mohanty, S.K.Kataria

L-Dependent Heavy Ion Fusion Potentials

NUCLEAR REACTIONS, ICPND 208Pb(16O, X), E=82-90 MeV; calculated fusion optical potential diffuseness parameter vs l, interaction barrier. 64Ni(58Ni, X), E(cm)=88-108 MeV; calculated fusion σ(E). Heavy ion l-dependent fusion potentials, other reactions, aspects studied.

doi: 10.1007/BF02875101
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1992MO19      Phys.Rev. C46, 2012 (1992)

A.K.Mohanty, S.V.S.Sastry, S.K.Kataria, V.S.Ramamurthy

Experimental Determination of Energy-Dependent Barriers for Fusion

NUCLEAR REACTIONS, ICPND 154Sm(16O, X), 59Co(37Cl, X), E(cm)=55-70 MeV; analyzed fusion, average angular momentum vs σ(E). Energy dependent barrier penetration model, other reactions studied.

doi: 10.1103/PhysRevC.46.2012
Citations: PlumX Metrics

1990MO19      Phys.Rev.Lett. 65, 1096 (1990)

A.K.Mohanty, S.V.S.Sastry, S.K.Kataria, V.S.Ramamurthy

Use of an Energy-Dependent Barrier for Heavy-Ion Fusion

NUCLEAR REACTIONS, ICPND 122Sn(40Ar, X), E(cm)=101-109 MeV; calculated fusion σ(E); deduced energy dependent barrier role. Full dynamical coupled-channels model.

doi: 10.1103/PhysRevLett.65.1096
Citations: PlumX Metrics

1990MO28      Phys.Lett. 247B, 215 (1990)

A.K.Mohanty, S.V.S.Sastry, S.K.Kataria, S.Kailas, V.S.Ramamurthy

A New Optical Model Approach for Heavy Ion Fusion

NUCLEAR REACTIONS, ICPND 208Pb(16O, X), E ≈ 76-112 MeV; calculated fusion σ(E). Optical model, energy dependent imaginary potential.

doi: 10.1016/0370-2693(90)90884-9
Citations: PlumX Metrics

1990RA11      Phys.Rev. C41, 2702 (1990)

V.S.Ramamurthy, A.K.Mohanty, S.K.Kataria, G.Rangarajan

Sub-Barrier Fusion in a Macroscopic Model of Nuclear Shape Evolutions

NUCLEAR REACTIONS 144,154Sm(40Ar, X), E(cm) ≈ 100-150 MeV; calculated effective fusion barrier vs E.

doi: 10.1103/PhysRevC.41.2702
Citations: PlumX Metrics

1987AJ01      Phys.Rev.Lett. 58, 1520 (1987)

N.N.Ajitanand, K.N.Iyengar, R.P.Anand, D.M.Nadkarni, A.K.Mohanty

Anomalous behavior of the proton-induced fission cross sections of 235U and 238U at extreme sub-barrier energies

NUCLEAR REACTIONS, ICPND 235,238U(p, F), E=0.5-4.3 MeV; measured fission σ(E). Enriched 235U, natural Uranium targets, solid state track detectors.

doi: 10.1103/PhysRevLett.58.1520
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0241.

1987MO02      Ann.Phys.(New York) 174, 1 (1987)

A.K.Mohanty, J.Sucher

Proton Decay in a Linear Potential Model

NUCLEAR STRUCTURE 1H; calculated decay amplitudes, branching ratios. Nonrelativistic quark model.

doi: 10.1016/0003-4916(87)90078-9
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