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NSR database version of April 24, 2024.

Search: Author = S.Sarkar

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2024BA05      J.Phys.(London) G51, 045201 (2024)

J.Barman, S.Sarkar, R.Chatterjee

Influence of light neutron-rich exotic nuclei in deciding abundance patterns relevant for explosive nucleosynthesis

NUCLEAR REACTIONS 18C, 19N(n, γ), 19C, 20N(γ, n), E<10 MeV; calculated neutron capture rates and photodisintegration constants under the aegis of the post-form distorted wave Born approximation (FRDWBA); deduced impact on abundance calculations in a neutrino-driven wind environment of a core-collapse supernova at two critical temperatures. Comparison with available data.

doi: 10.1088/1361-6471/ad2275
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2024GU02      Nucl.Phys. A1042, 122806 (2024)

A.Gupta, S.Sharma, S.Das, A.Adhikari, A.Mondal, M.Chowdhury, Ch.D.Bagdia, L.Tribedi, V.Nanal, A.Bisoi, M.S.Sarkar, S.Sarkar

Lifetime measurement of the Ex = 2485.3 keV level of 25Al populated through 24Mg(p, γ)25Al resonance reaction

NUCLEAR REACTIONS 24Mg(p, γ), E=220-265 keV; measured reaction products, Eγ, Iγ. 25Al; deduced γ-ray energies, energy levels, J, π, resonance state T1/2, spectroscopic factor, γ-ray branching ratio, resonance parameters. Comparison with theoretical calculations. Doppler shift attenuation (DSA) method, the 14.5 GHz electron cyclotron resonance (ECR) ion accelerator at TIFR, Mumbai.

doi: 10.1016/j.nuclphysa.2023.122806
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2024KA08      Eur.Phys.J. A 60, (2024)

P.Kalikotay, S.Ghosh, N.Chaudhuri, P.Roy, S.Sarkar

Electrical conductivity and shear viscosity of a pion gas in a thermo-magnetic medium

doi: 10.1140/epja/s10050-024-01291-w
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2024RA07      Phys.Rev. C 109, 024318 (2024)

R.Rahaman, A.Bisoi, A.Das, Y.Sapkota, A.Gupta, S.Ray, S.Sarkar, Yashraj, A.Sharma, Bh.Rohila, I.Ahmed, K.Katre, S.Dutt, S.Kumar, R.P.Singh, R.Kumar, S.Muralithar

Spectroscopic study of 40K

doi: 10.1103/PhysRevC.109.024318
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2024SA07      Phys.Rev. C 109, 024301 (2024)

Sh.Sarkar, P.K.Rath, V.Nanal, R.G.Pillay, PushpendraP.Singh, Y.Iwata, K.Jha, P.K.Raina

Calculation of nuclear matrix elements for 0νββ decay of 124Sn using the nonclosure approach in the nuclear shell model

doi: 10.1103/PhysRevC.109.024301
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2023BA27      Phys.Rev. C 108, 025812 (2023)

R.Barman, S.Sarkar, R.Chatterjee

Structure effects of exotic nuclei in the A ≈ 30 mass region relevant for determining abundance patterns in explosive nucleosynthesis

NUCLEAR REACTIONS 33Na, 36Mg(n, γ), T=0.01-10 GK;34Na, 37Mg(γ, n), T=0.5-10 GK;32,33,34,35Na, 32,33,34,35,36Mg, 34,35,36Al(n, γ), 32,33,34Na(α, n), 32,33,34,35,36Na, 32,33,34,35,36,37Mg, 34,35,36,37Al(γ, n), T=0.62, 3.4 GK; calculated reaction rates. Calculations based on finite-range distorted-wave Born approximation (FRDWBA) theory and TALYS code. Performed abundance calculations for a network of neutron-rich Na, Mg, and Al isotopes. Comparison with JINA-REACLIB database and TALYS calculations.

doi: 10.1103/PhysRevC.108.025812
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2023GU13      Phys.Rev. C 108, 015805 (2023)

A.Gupta, C.Lahiri, S.Sarkar

Allowed β- decay of bare atoms with A ≈ 60 - 80 in stellar environments

RADIOACTIVITY 59Fe, 60,61Co, 63,65,66Ni, 64,66,67Cu, 69,72Zn, 70Ga, 75,78Ge, 81Se(β-); calculated decay rates, bound state decay rate, continuum state decay rate, logft, T1/2, T1/2 of bare atoms as functions of density and temperature in stellar S-process environment, ratio of neutral to bare atom half-life, branchings. 59Fe, 69Zn(β-); calculated Gamow-Teller transition matrix elements, quenching factors. Shell model calculations. Comparison to available experimental data.

NUCLEAR STRUCTURE 59Fe, 59Co, 69Zn, 69Ga, 78Ge, 78As; calculated levels, J, π. Shell-model calculations with fpd6, fpd6n and jun45 interactions. Comparison to experimental data.

doi: 10.1103/PhysRevC.108.015805
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2023MO27      Eur.Phys.J. A 59, 287 (2023)

R.Mondal, N.Chaudhuri, S.Ghosh, S.Sarkar, P.Roy

Ellipticity of dilepton production from a hot and magnetized hadronic medium

doi: 10.1140/epja/s10050-023-01201-6
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2023SA42      Universe 9, 444 (2023)

S.Sarkar, Y.Iwata

Effect of Spin-Dependent Short-Range Correlations on Nuclear Matrix Elements for Neutrinoless Double Beta Decay of 48Ca

RADIOACTIVITY 48Ca(2β-); calculated nuclear matrix elements (NMEs) for the light neutrino-exchange mechanism in neutrinoless double beta employing an extensive interacting nuclear shell model employing the effective shell model Hamiltonian GXPF1A, encompassing the entire fp model space through the closure approximation; deduced the impact of spin-dependent short-range correlations (SRCs).

doi: 10.3390/universe9100444
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2022AD11      Nucl.Phys. A1027, 122495 (2022)

A.Adhikari, D.Pramanik, S.Sarkar, M.Sarkar, A.Bisoi, S.Ray, S.Rajbanshi, S.Saha, J.Sethi, B.S.Naidu, R.Donthi, V.Nanal, R.Palit

Experimental evidences of shape co-existence in 154Ho

NUCLEAR REACTIONS 141Pr(16O, 3n)154Ho, E=82 MeV; measured reaction products, Eγ, Iγ, γ-γ-coin.; deduced γ-ray energies and relative intensities, partial level scheme, J, π, mixing ratios for the mixed transitions and parities. The Indian National Gamma Array (INGA) setup at BARC-TIFR Pelletron facility, Tata Institute of Fundamental Research, Mumbai.

doi: 10.1016/j.nuclphysa.2022.122495
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2022CH30      Eur.Phys.J. A 58, 82 (2022)

N.Chaudhuri, A.Mukherjee, S.Ghosh, S.Sarkar, P.Roy

Insignificance of the anomalous magnetic moment of the quarks in presence of chiral imbalance

doi: 10.1140/epja/s10050-022-00731-9
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2022SA15      Phys.Rev. C 105, 044304 (2022)

Y.Sapkota, R.Rahaman, A.Bisoi, A.Adhikari, A.Gupta, A.Das, H.Ghosh, S.Sarkar, D.Pramanik, S.Das, S.Sharma, S.Ray, S.Rajbanshi, S.Dar, S.Nandi, S.Bhattacharya, T.Bhattacharjee, G.Mukherjee, S.Bhattacharyya, S.Samanta, S.Das, S.Chatterjee, R.Raut, S.S.Ghugre

Structural evolution and K mixing in 49V

NUCLEAR REACTIONS 48Ti(α, 2np), E=48 MeV; measured Eγ, Iγ, γγ-coin, γ(θ). 49V; deduced levels, J, π, branching ratios, δ, DCO-ratios, B(M&1), B(E2), T1/2 of several high-spin states, neutron and proton single-parti&&cle states occupation numbers, negative-parity bands structure; calculated leve total Routhian surface (TRS) plots in (β2, γ) plane, single-particle proton and neutron energies in a rotating frame. 50Cr; calculated levels, J, π, spectroscopic factors. Lifetimes of the levels extracted with line-shape analysis of Doppler-shifted spectra. Comparison of experimental results to large basis shell model (LBSM) calculations with KB3GPN effective interaction. Indian National Gamma Array (INGA) at K-130 cyclotron of Variable Energy Cyclotron Centre, Kolkata (VECC).

doi: 10.1103/PhysRevC.105.044304
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2022SA33      Eur.Phys.J. A 58, 139 (2022)

S.Sarkar, P.Mali, A.Mukhopadhyay

Transverse sphericity based event classification in Au+Au collision at Elab = 30A GeV in a multi phase transport model

doi: 10.1140/epja/s10050-022-00784-w
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2022SA34      Eur.Phys.J. A 58, 136 (2022)

S.Sarkar, P.Mali, A.Mukhopadhyay

System size dependence of harmonic flow parameters in a multiphase transport model at Elab = 30A GeV

doi: 10.1140/epja/s10050-022-00790-y
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2021DA02      Nucl.Phys. A1006, 122079 (2021)

S.Das, A.Adhikari, S.S.Alam, S.Sharma, S.Aich, A.Gupta, Y.Sapkota, A.Das, A.Saha, S.K.Dey, D.Pramanik, A.Bisoi, I.Ray, T.Bhattacharjee, C.C.Dey, S.Sarkar, M.S.Sarkar

Decay spectroscopy of 117, 118Sn

RADIOACTIVITY 117,118Sb(EC), 117Sn(IT) [from In(α, X), E=32 MeV]; measured decay products, Eγ, Iγ, γ-γ-coin.; deduced γ-ray energies and intensities, J, π, level T1/2. Comparison with available data, shell model calculations.

doi: 10.1016/j.nuclphysa.2020.122079
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2020AL17      Eur.Phys.J. A 56, 269 (2020)

S.S.Alam, D.Banerjee, T.Bhattacharjee, P.Blaha, D.Kumar, A.Saha, M.S.Sarkar, S.Sarkar, S.K.Das

Measurement of electric quadrupole moment in neutron rich 131, 132I

RADIOACTIVITY 131,132Te(β-) [from U(α, F), E=40 MeV]; measured decay products, quadrupole frequencies, Eγ, Iγ; deduced γ-ray energies, J, π, electric quadrupole moments, deformation parameters, evolution of collectivity. Comparison with a large basis shell model calculations.

doi: 10.1140/epja/s10050-020-00281-y
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2020CH31      Eur.Phys.J. A 56, 213 (2020)

N.Chaudhuri, S.Ghosh, S.Sarkar, P.Roy

Effects of quark anomalous magnetic moment on the thermodynamical properties and mesonic excitations of magnetized hot and dense matter in PNJL model

doi: 10.1140/epja/s10050-020-00222-9
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2020DA05      Phys.Rev. C 101, 044310 (2020)

A.Das, A.Bisoi, M.S.Sarkar, S.Sarkar, S.Ray, D.Pramanik, R.Kshetri, S.Nag, P.Singh, K.Selvakumar, A.Goswami, S.Saha, J.Sethi, T.Trivedi, B.S.Naidu, R.Donthi, V.Nanal, R.Palit

High spin states of 37Ar

NUCLEAR REACTIONS 27Al(12C, np), E=40 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO and ADO), γγ(linear polarization) using the INGA array at the 14UD Pelletron accelerator of TIFR-Mumbai. 37Ar; deduced high-spin levels, J, π, γ-branching ratios, multipolarities, mixing ratios, B(E1), B(M1), B(E2), B(M2). Comparison with large basis shell model calculations using OXBASH code with SDPFMW interaction, and with simple two-level mixing calculation. Comparison with previous experimental results.

NUCLEAR STRUCTURE 37Ar; calculated levels, J, π, γ-branching ratios, wave functions amplitudes and partitions for the positive- and negative-parity states, B(E1), B(M1), B(E2), B(M2), level half-lives, 0p-0h configuration mixing in yrast levels. Large basis shell model calculations using OXBASH code with SDPFMW interaction, and simple two-level mixing calculations. Comparison with experimental data.

doi: 10.1103/PhysRevC.101.044310
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2020JH02      Nucl.Phys. A1004, 122038 (2020)

K.Jha, P.Kumar, S.Sarkar, P.K.Raina, S.Aydin

A way forward towards the improvement of tensor force in pf-shell

NUCLEAR STRUCTURE 40,42,44,46,48,50,52,54Ca, 56,57Ni; analyzed available data; deduced level energies, J, π, core softness, yrast bands using GXPF1B effective interaction.

doi: 10.1016/j.nuclphysa.2020.122038
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2020KA23      Eur.Phys.J. A 56, 79 (2020)

P.Kalikotay, N.Chaudhuri, S.Ghosh, U.Gangopadhyaya, S.Sarkar

Viscous coefficients and thermal conductivity of a πKN gas mixture in the medium

doi: 10.1140/epja/s10050-020-00074-3
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2020KA65      Pramana 94, 100 (2020)

K.Kar, S.Sarkar

The linear term in the isobaric-mass-multiplet equation for fp-shell nuclei in the framework of spectral distribution theory

doi: 10.1007/s12043-020-01957-2
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2020RA14      Phys.Rev. C 102, 024315 (2020)

R.Rahaman, A.Bisoi, Y.Sapkota, A.Adhikari, A.Das, S.Sarkar, M.S.Sarkar, A.Goswami, S.Ray, M.R.Basu, D.Kanjilal, S.Nag, K.Selvakumar, N.Madhavan, S.Muralithar, R.K.Bhowmik

Spectroscopic study of 38K above the 31.67 μs isomer

NUCLEAR REACTIONS 12C(28Si, np)38K, E=110 MeV; measured Eγ, Iγ, γγ(θ)(DCO and ADO), γγ(linear polarization) using the INGA array at 15UD Pelletron accelerator of IUAC-New Delhi. 38K; deduced high-spin levels above the 31.67-μs isomer, J, π, multipolarities, mixing ratios. 35Cl; measured γγ(θ)(DCO and ADO ratios) for six γ rays. Comparison with large-basis shell-model calculations using the code OXBASH.

NUCLEAR STRUCTURE 38K; calculated levels, J, π, B(M1), B(E2), B(E3), spectroscopic factors, structure of the wave functions for excited states using large-basis shell-model calculations using the code OXBASH with different particle restrictions in sd- and pf -shell orbitals. Comparison with experimental data.

doi: 10.1103/PhysRevC.102.024315
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2020SA03      Phys.Rev. C 101, 014307 (2020)

S.Sarkar, P.Kumar, K.Jha, P.K.Raina

Sensitivity of nuclear matrix elements of 0νββ of 48Ca to different components of the two-nucleon interaction

RADIOACTIVITY 48Ca(2β-); calculated nuclear matrix elements (NMEs) for light neutrino-exchange mechanism of 0νββ with central (C), spin-orbit (SO), and tensor force (T) components in the shell-model framework using GXPF1A interaction and the GX1R, a modified fp model-space interaction.

NUCLEAR STRUCTURE 46,48Ca, 48Ti; calculated levels, J, π using shell-model with GXPF1A and GX1R interactions. Comparison with experimental data.

doi: 10.1103/PhysRevC.101.014307
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2020SA35      Phys.Rev. C 102, 034317 (2020)

S.Sarkar, Y.Iwata, P.K.Raina

Nuclear matrix elements for the Λ mechanism of 0νββ decay of 48Ca in the nuclear shell-model: Closure versus nonclosure approach

RADIOACTIVITY 48Ca(2β); calculated nuclear matrix elements (NMEs) for the 0νββ decay mode, distribution of NMEs as function of neutrino momentum transfer, radial distribution of NMEs as function of internucleon distance, contribution from spin-parity of virtual intermediate states of 48Sc, contribution through different coupled spin-parity of two initial neutrons or two final created protons, Fermi, Gamow-Teller, tensor, and total 0νββ NMEs as function of cutoff excitation energy of states of virtual intermediate nucleus 48Sc. Interacting shell-model with the GXPF1A effective interaction of pf shell in Miller-Spencer, CD-Bonn, and AV18 SRC parametrizations, and using closure, running closure, running nonclosure, and mixed methods.

doi: 10.1103/PhysRevC.102.034317
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2019AL03      Phys.Rev. C 99, 014306 (2019)

S.S.Alam, T.Bhattacharjee, D.Banerjee, A.Saha, S.Das, M.S.Sarkar, S.Sarkar

Lifetimes and transition probabilities for the low-lying states in 131I and 132Xe

RADIOACTIVITY 131mTe[from 238U(α, F), E=40 MeV]; 132I(β-)[from decay of 132Te formed in 238U(α, F), E=40 MeV]; measured Eγ, Iγ, γγ-coin, level half-lives by γγ(t) fast-timing method, and half-life of 1797-keV nanosecond isomer in 131I by slope method using the VENTURE array of CeBr3 scintillators and VENUS arrays of six Compton-suppressed Clover HPGe detectors at the K-130 cyclotron facility of VECC, Kolkata. 131I, 132Xe; deduced levels, J, π, configurations, B(E1), B(E2), B(E3). Systematics of E1 decays from 11/2- levels in 121,123,125,127,131I, and 13/2- and 15/2- levels in 129Sb, 131,133I. Comparison with large-basis shell model calculations using the NUSHELLX code.

NUCLEAR STRUCTURE 131I, 132Xe; calculated levels, J, π, dominant particle partitions, configurations, and level half-lives using the large-basis shell model (LBSM) with the NUSHELLX code. Comparison with experimental data.

doi: 10.1103/PhysRevC.99.014306
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2019GU33      Phys.Rev. C 100, 064313 (2019)

A.Gupta, C.Lahiri, S.Sarkar

Bound and continuum state β- decay of bare atoms: Enhancement of decay rate and changes in β- decay branching

RADIOACTIVITY 63,66Ni, 85,85mKr, 93Zr, 95,95mNb, 99Tc, 106Ru, 107Pd, 110Ag, 113,115Cd, 121,121m,123,123mSn, 124Sb, 134,136Cs, 148,148mPm, 151Sm, 152,152m,155Eu, 171Tm, 191Os, 207Tl, 210Pb, 227Ac, 228Ra, 241Pu(β-); calculated β-decay half-lives for the fully-ionized (bare) ions, logft, individual contributions to β--decay rates for bound and continuum states in neutral atoms and fully-ionized (bare) ions; deduced that transition branchings for the bare atom differ from that of the neutral atom for all Z and A in A=60-240 mass region. Comparison with experimental values of half-lives for neutral atoms in the NNDC databases, and with theoretical values from 1987Ta16.

doi: 10.1103/PhysRevC.100.064313
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2019KU14      Phys.Rev. C 100, 024328 (2019)

P.Kumar, S.Sarkar, P.P.Singh, P.K.Raina

Proton-neutron force and proton single-particle strength in Sc, F, and Li isotopes

NUCLEAR STRUCTURE Z=3, N=2-8; Z=9, N=8-20; Z=21, N=20-40; calculated effective single-particle energies (ESPEs) of 0p proton orbitals in Li, 0d1s proton orbitals in F, and 0f1p proton orbitals in Sc isotopes, contribution of central, spin-orbit, and tensor forces of proton-neutron interaction to proton single-particle energy gaps. 9Li, 23,25F, 49,53,55Sc; calculated levels, J, π, proton transfer spectroscopic factors. Shell model calculations with CKHeN interaction. Comparison with experimental data.

doi: 10.1103/PhysRevC.100.024328
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2018AH05      Eur.Phys.J. A 54, 224 (2018)

F.Ahmed, F.Rahaman, S.Sarkar

Black holes/naked singularities in four-dimensional non-static space-time and energy-momentum distributions

doi: 10.1140/epja/i2018-12650-y
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2018BI04      Phys.Rev. C 97, 044317 (2018)

A.Bisoi, A.Das, M.S.Sarkar, S.Sarkar

Cluster states at low excitation energy in 34S

NUCLEAR STRUCTURE 34S, 35Cl, 36Ar; calculated levels, J, π, superdeformed states in 35Cl and 36Ar. 34S; calculated spectroscopic factors for one-nucleon transfer from 35Cl and two-nucleon transfers from 36Ar to obtain parentage of states in 34S from core (normal and superdeformed) states in 35Cl and 36Ar, and from core states in 32S, 30Si+α cluster structures. Large basis shell-model (LBSM) calculations with SDPFMWPN interaction using OXBASH computer code. Comparison with experimental data.

doi: 10.1103/PhysRevC.97.044317
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2018GH01      Nucl.Phys. A969, 237 (2018)

S.Ghosh, S.Mitra, So.Sarkar

Medium effects on the electrical conductivity of a hot pion gas

doi: 10.1016/j.nuclphysa.2017.10.008
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2018MA41      Eur.Phys.J. A 54, 99 (2018)

M.Mandal, A.Mukherjee, S.Ghosh, P.Roy, S.Sarkar

ρ0 - w mixing in the presence of a weak magnetic field

doi: 10.1140/epja/i2018-12527-1
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2018RA05      Phys.Rev. C 97, 035201 (2018)

M.Rahaman, S.Ghosh, S.Ghosh, S.Sarkar, J.-e.Alam

Contribution of a kaon component in the viscosity and conductivity of a hadronic medium

doi: 10.1103/PhysRevC.97.035201
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2018SA22      Nucl.Phys. A976, 1 (2018)

A.Saha, T.Bhattacharjee, S.S.Alam, D.Banerjee, M.S.Sarkar, S.Sarkar, J.B.Gupta, P.Das, S.Bhattacharya, D.Pandit, R.Guin, S.K.Das, S.R.Banerjee

Spectroscopy of low lying states in 150Sm

NUCLEAR REACTIONS 150Nd(p, n)150Sm, E=8.0 MeV; measured Eγ, Iγ, γγ-coin using VENUS array of six Compton-suppressed Clover HPGe. 150Sm deduced γ transitions, levels, J, π, spin and parity using NNDC logft calculator and angular correlations; estimated possible M2 admixture, B(E1).

doi: 10.1016/j.nuclphysa.2018.05.005
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2018SA26      Phys.Rev. C 97, 064916 (2018)

S.Sarkar, C.Chattopadhyay, S.Pal

Radiative heavy quark energy loss in an expanding viscous QCD plasma

doi: 10.1103/PhysRevC.97.064916
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2017SA03      Phys.Rev. C 95, 014908 (2017)

S.Sarkar, P.Mali, A.Mukhopadhyay

Simulation study of elliptic flow of charged hadrons produced in Au + Au collisions at energies available at the Facility for Antiproton and Ion Research

doi: 10.1103/PhysRevC.95.014908
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2017SA49      Phys.Rev. C 96, 024913 (2017)

S.Sarkar, P.Mali, A.Mukhopadhyay

Azimuthal anisotropy in particle distribution in a multiphase transport model

doi: 10.1103/PhysRevC.96.024913
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2016BI02      Phys.Rev. C 93, 034324 (2016)

S.Biswas, R.Palit, A.Navin, M.Rejmund, A.Bisoi, M.S.Sarkar, S.Sarkar, S.Bhattacharyya, D.C.Biswas, M.Caamano, M.P.Carpenter, D.Choudhury, E.Clement, L.S.Danu, O.Delaune, F.Farget, G.de France, S.S.Hota, B.Jacquot, A.Lemasson, S.Mukhopadhyay, V.Nanal, R.G.Pillay, S.Saha, J.Sethi, P.Singh, P.C.Srivastava, S.K.Tandel

Structure of 13252Te80: The two-particle and two-hole spectrum of 13250Sn82

NUCLEAR REACTIONS 232Th(7Li, F)132Te, E=5.4 MeV/nucleon; 9Be(238U, F), E=6.2 MeV/nucleon; measured Eγ, Iγ, γγ-coin, γγ(t), (fragment)γ-, (fragment)γγ-coin, γγ(θ) using INGA array at TIFR-BARC Pelletron LINAC facility for (7Li, F) reaction, and EXOGAM-VAMOS++ system at GANIL for (238U, F) reaction. 132Te; deduced high-spin levels, J, π, multipolarity, configurations, proton and neutron wavefunction amplitudes, p-n correlations at high spin. Comparison with shell-model calculations using jj55pna and modified jj55pna interactions. Systematics of positive-parity level energies in 122,124,126,128,130,132,134,136Te.

NUCLEAR STRUCTURE 132Te; calculated levels, J, π, proton and neutron wavefunction amplitudes, decomposition of the total angular momentum of positive- and negative-parity states using shell model jj55pna and modified jj55pna interactions. Comparison with experimental values. 132Te, 130Sn; 130Te, 128Sn; 128Te, 126Sn; deduced energy differences between the experimental and calculated energy levels of positive-parity as a function of spin, with calculations using shell model.

doi: 10.1103/PhysRevC.93.034324
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2016GA37      Phys.Rev. C 94, 044914 (2016)

U.Gangopadhyaya, S.Ghosh, S.Sarkar, S.Mitra

In-medium viscous coefficients of a hot hadronic gas mixture

doi: 10.1103/PhysRevC.94.044914
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2016GH06      Phys.Rev. C 93, 054904 (2016)

S.Ghosh, S.K.Singh, S.Chatterjee, J.Alam, S.Sarkar

Initial conditions from the shadowed Glauber model for Pb + Pb collisions at √ sNN = 2.76 TeV

doi: 10.1103/PhysRevC.93.054904
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2016MI12      Nucl.Phys. A951, 75 (2016)

S.Mitra, S.Ghosh, S.K.Das, S.Sarkar, J.-e.Alam

Diffusion of hidden charm mesons in hadronic medium

doi: 10.1016/j.nuclphysa.2016.03.035
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2016PR06      Phys.Rev. C 94, 024311 (2016)

D.Pramanik, S.Sarkar, M.S.Sarkar, A.Bisoi, S.Ray, S.Dasgupta, A.Chakraborty, Krishichayan, R.Kshetri, I.Ray, S.Ganguly, M.K.Pradhan, M.R.Basu, R.Raut, G.Ganguly, S.S.Ghugre, A.K.Sinha, S.K.Basu, S.Bhattacharya, A.Mukherjee, P.Banerjee, A.Goswami

Shape coexistence in 153Ho

NUCLEAR REACTIONS 139La(20Ne, 6n), E=139 MeV; measured Eγ, Iγ, delayed Iγ, γγ-coin, γγ(θ)(DCO), γγ(linear polarization), half-life of an isomer by RF-γ(t) using INGA array at VECC cyclotron facility. 153Ho; deduced high-spin levels, J, π, multipolarity, mixing ratio, B(E2), indication of shape coexistence, alignment plots, energy versus angular momentum plots. TRS calculations. Comparison with theoretical calculations using particle-rotor model.

doi: 10.1103/PhysRevC.94.024311
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2015KA10      J.Phys.(London) G42, 055110 (2015)

K.Kar, S.Sarkar

Study of isospin nonconservation in the framework of spectral distribution theory

doi: 10.1088/0954-3899/42/5/055110
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2015SA35      Pramana 85, 403 (2015)

M.Saha-Sarkar, S.Sarkar

136Sn and three-body forces

NUCLEAR STRUCTURE 136,138Sn; calculated energy levels, J, π, B(E2) using the CD-Bonn potential-based realistic CWG and and the empirical SMPN along with the CWG3M interactions; deduced three-body forces.

doi: 10.1007/s12043-015-1055-z
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2014BI03      Phys.Rev. C 89, 024303 (2014)

A.Bisoi, M.S.Sarkar, S.Sarkar, S.Ray, D.Pramanik, R.Kshetri, S.Nag, K.Selvakumar, P.Singh, A.Goswami, S.Saha, J.Sethi, T.Trivedi, B.S.Naidu, R.Donthi, V.Nanal, R.Palit

High spin spectroscopy in 34Cl

NUCLEAR REACTIONS 27Al(12C, nα), E=40 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO), γγ(linear polarization), level half-lives by DSAM using INGA array at TIFR accelerator facility. 34Cl; deduced high-spin levels, J, π, multipolarity, mixing ratio, B(E2). Comparison with large-basis shell-model calculations.

NUCLEAR STRUCTURE 34Cl; calculated levels, J, π, wave functions, γ-branching ratios, B(M1), B(E2), B(M2) using large-basis shell-model (LBSM) calculations for different truncation schemes. OXBASH computer code. Comparison with experimental data.

doi: 10.1103/PhysRevC.89.024303
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2014BI16      Phys.Rev. C 90, 024328 (2014)

A.Bisoi, M.S.Sarkar, S.Sarkar, S.Ray, D.Pramanik, R.Kshetri, S.Nag, K.Selvakumar, P.Singh, A.Goswami, S.Saha, J.Sethi, T.Trivedi, B.S.Naidu, R.Donthi, V.Nanal, R.Palit

Collective excitations in 33S

NUCLEAR REACTIONS 27Al(12C, npα)33S, E=40 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO), γγ(linear polarization), level half-lives by DSAM using INGA array at TIFR Pelletron facility. 33S; deduced levels, J, π, branching ratios, multipolarity, mixing ratio, B(M1), B(E1), B(E2), configurations. Comparison with large-scale shell model calculations.

NUCLEAR STRUCTURE 33S; calculated levels, J, π, configurations, wave functions, B(E1), B(M1), B(E2), alignment plot using large-basis shell model approach. Comparison with experimental data.

doi: 10.1103/PhysRevC.90.024328
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2014GH03      Phys.Rev. C 89, 045201 (2014)

S.Ghosh, G.Krein, S.Sarkar

Shear viscosity of a pion gas resulting from ρππ and σππ interactions

doi: 10.1103/PhysRevC.89.045201
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2014MA93      Phys.Rev. C 90, 055803 (2014)

C.Manuel, S.Sarkar, L.Tolos

Thermal conductivity due to phonons in the core of superfluid neutron stars

doi: 10.1103/PhysRevC.90.055803
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2013BI10      Phys.Rev. C 88, 034303 (2013)

A.Bisoi, M.S.Sarkar, S.Sarkar, S.Ray, M.R.Basu, D.Kanjilal, S.Nag, K.Selvakumar, A.Goswami, N.Madhavan, S.Muralithar, R.K.Bhowmik

Superdeformation and α-cluster structure in 35Cl

NUCLEAR REACTIONS 12C(28Si, pα)35Cl, E=110 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO), level half-lives by DSAM using INGA array at IUAC, Delhi facility. 35Cl; deduced high-spin levels, J, π, multipolarity, superdeformed band, B(E2), B(E1), configuration, average transition quadrupole moment and deformation parameter for SD band, alignment plot. Comparison with large-scale shell model calculations. Correlation of theoretical spectroscopic factors for SD band members in 35Cl with those of 36Ar.

doi: 10.1103/PhysRevC.88.034303
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2013GH01      Eur.Phys.J. A 49, 97 (2013)

S.Ghosh, S.Sarkar

Analysis of w self-energy at finite temperature and density in the real-time formalism

doi: 10.1140/epja/i2013-13097-4
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2013GH03      Nucl.Phys. A917, 71 (2013)

S.Ghosh, S.Mitra, S.Sarkar

Effect of in-medium spectral density of D and D* mesons on the J/ψ dissociation in hadronic matter

doi: 10.1016/j.nuclphysa.2013.08.010
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2012MA25      Phys.Rev. C 85, 067901 (2012)

M.Mandal, P.Roy, S.Mitra, S.Sarkar

Effect of running coupling on photon emission from quark gluon plasma

doi: 10.1103/PhysRevC.85.067901
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2012MI14      Phys.Rev. C 85, 064917 (2012)

S.Mitra, S.Ghosh, S.Sarkar

Effect of a spectral modification of the ρ meson on the shear viscosity of a pion gas

doi: 10.1103/PhysRevC.85.064917
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2012MO07      Phys.Rev. C 85, 031903 (2012)

P.Mohanty, V.Roy, S.Ghosh, S.Das, B.Mohanty, S.Sarkar, J.-e.Alam, A.Chaudhuri

Elliptic flow of thermal dileptons as a probe of QCD matter

doi: 10.1103/PhysRevC.85.031903
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2012NA13      Phys.Rev. C 85, 064906 (2012)

J.K.Nayak, J.-e.Alam, T.Hirano, S.Sarkar, B.Sinha

Muon pairs from In + In collision at energies available at the CERN Super Proton Synchrotron

doi: 10.1103/PhysRevC.85.064906
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2011GH01      Phys.Rev. C 83, 018201 (2011)

S.Ghosh, S.Sarkar, S.Mallik

Baryonic loop in the ρ-meson self-energy

doi: 10.1103/PhysRevC.83.018201
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2011GH04      Nucl.Phys. A862-863, 294c (2011)

S.Ghosh, S.Sarkar, J.Alam

The ρ meson in hot hadron matter and low mass dilepton spectra

doi: 10.1016/j.nuclphysa.2011.05.082
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2011GH07      Nucl.Phys. A870-871, 94 (2011)

S.Ghosh, S.Sarkar

ρ self-energy at finite temperature and density in the real-time formalism

doi: 10.1016/j.nuclphysa.2011.09.001
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2011SA31      Nucl.Phys. A862-863, 13c (2011)

S.Sarkar

Hadrons at finite temperature

doi: 10.1016/j.nuclphysa.2011.05.015
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2011WI09      Phys.Rev. C 84, 014329 (2011); Pub.Note JOUR PRVCA 84 029903 (2011)

K.Wimmer, U.Koster, P.Hoff, Th.Kroll, R.Krucken, R.Lutter, H.Mach, Th.Morgan, S.Sarkar, M.Saha-Sarkar, W.Schwerdtfeger, P.C.Srivastava, P.G.Thirolf, P.Van Isacker

Identification of the slow E3 transition 136Csm136Cs with conversion electrons

NUCLEAR REACTIONS U(p, X)136mCs, E=1.4 GeV; measured Eγ, Iγ, E(ce), I(ce), γ(ce)-coin, isomer half-life, conversion coefficients. 136Cs; deduced levels, J, π, multipolarity, level scheme of isomer decay, B(E3), B(M4). Comparison with shell-model calculations.

doi: 10.1103/PhysRevC.84.014329
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2010GH03      Phys.Rev. C 82, 045202 (2010)

S.Ghosh, S.Sarkar, S.Mallik

Relativistic spectral function of nucleons in hot nuclear matter

doi: 10.1103/PhysRevC.82.045202
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2010OS05      Nucl.Phys. A835, 271c (2010)

E.Oset, S.Sarkar, B.X.Sun, M.J.Vicente Vacas, A.Ramos, P.Gonzalez, J.Vijande, A.Martinez Torres, K.Khemchandani

Baryon Resonances

doi: 10.1016/j.nuclphysa.2010.01.202
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2010SA05      Phys.Rev. C 81, 039803 (2010)

S.Sarkar, M.S.Sarkar

Comment on "High spin structure of the neutron-rich nuclei 137I and 139Cs"

doi: 10.1103/PhysRevC.81.039803
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2010SA14      Phys.Rev. C 81, 064328 (2010)

S.Sarkar, M.S.Sarkar

New shell closure for neutron-rich Sn isotopes

NUCLEAR STRUCTURE 132,134,136,138,140Sn; calculated energies of first 2+ states, effective single-particle energies (ESPE) of the neutron single-particle orbitals, decomposition of the wave functions for 0+ states. 140Sn, 142Te, 144Xe, 146Ba, 148Ce; calculated effective single-particle energies (ESPE) of the proton single-particle orbitals. Shell model calculations with CWG3M interaction by including a three-body monopole term in the CWG interaction. Comparison with energies of first 2+ states in 16,18,20,22,24O, 40,42,44,46,48Ca. Predicted decreasing trend for energies of first 2+ states in 136,138Sn, and a shell closure at 140Sn.

doi: 10.1103/PhysRevC.81.064328
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2010SA31      Eur.Phys.J. A 44, 431 (2010)

S.Sarkar, B.-X.Sun, E.Oset, M.J.Vicente Vacas

Dynamically generated resonances from the vector octet-baryon decuplet interaction

doi: 10.1140/epja/i2010-10956-4
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2008MA11      Phys.Rev. C 77, 032201 (2008)

S.Mallik, J.N.De, S.K.Samaddar, S.Sarkar

S-matrix approach to equation of state of nuclear matter

doi: 10.1103/PhysRevC.77.032201
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2008NA21      Phys.Rev. C 78, 034903 (2008)

J.K.Nayak, J.Alam, S.Sarkar, B.Sinha

Thermal photon to dilepton ratio in high energy nuclear collisions

doi: 10.1103/PhysRevC.78.034903
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2008SA32      Phys.Rev. C 78, 024308 (2008); Erratum Phys.Rev. C 78, 029903 (2008)

S.Sarkar, M.S.Sarkar

Structure of even-even A = 138 isobars and the yrast spectra of semi-magic Sn isotopes above the 132Sn core

NUCLEAR STRUCTURE 138Sn, 138Te, 138Xe, 138Ba; calculated binding energies, levels, J, π, B(E2), configuration mixing, magnetic dipole moments, electric quadrupole moments. Large scale untruncated shell model. Comparison with experimental data.

doi: 10.1103/PhysRevC.78.024308
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2007CH74      Phys.Rev. C 76, 044327 (2007)

A.Chakraborty, Krishichayan, S.Mukhopadhyay, S.Ray, S.N.Chintalapudi, S.S.Ghugre, N.S.Pattabiraman, A.K.Sinha, S.Sarkar, U.Garg, S.Zhu, M.S.Sarkar

High-spin structure and band termination in 103Cd

NUCLEAR REACTIONS 72Ge(35Cl, 3np), E=135 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ), multipolarities. 103Cd deduced levels, J, π, angular momentum, bands; calculated shell-model configurations. Gammasphere array.

doi: 10.1103/PhysRevC.76.044327
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2007KS01      Nucl.Phys. A781, 277 (2007)

R.Kshetri, M.S.Sarkar, I.Ray, P.Banerjee, S.Sarkar, R.Raut, A.Goswami, J.M.Chatterjee, S.Chattopadhyay, U.Datta Pramanik, A.Mukherjee, C.C.Dey, S.Bhattacharya, B.Dasmahapatra, S.Bhowal, G.Gangopadhyay, P.Datta, H.C.Jain, R.K.Bhowmik, S.Muralithar R.P.Singh, R.Kumar

High spin structure of 35Cl and the sd-fp shell gap

NUCLEAR REACTIONS 12C(28Si, pα), E=70, 88 MeV; measured Eγ, Iγ, γγ-coin, DSA. 35Cl deduced levels J, π, δ, T1/2. INGA array, shell model calculations.

doi: 10.1016/j.nuclphysa.2006.10.084
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2007OS01      Nucl.Phys. A782, 259c (2007)

E.Oset, S.Sarkar, M.J.Vicente Vacas, M.Kaskulov, L.Roca, V.K.Magas, A.Ramos, H.Toki

Recent developments in chiral dynamics of hadrons and hadrons in a nuclear medium

doi: 10.1016/j.nuclphysa.2006.10.026
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2007RA20      Phys.Rev. C 76, 034315 (2007)

I.Ray, M.R.Basu, R.Kshetri, M.S.Sarkar, S.Sarkar, P.Banerjee, S.Chattopadhyay, C.C.Dey, A.Goswami, J.M.Chatterjee, A.Mukherjee, S.Bhattacharya, B.Dasmahapatra, P.Datta, H.C.Jain, R.K.Bhowmik, S.Muralithar, R.P.Singh

Indication of the onset of collectivity in 30P

NUCLEAR REACTIONS 16O(16O, np), E=40 MeV; measured Eγ, Iγ, γγ-coinc, polarization assymetry. 30P deduced levels, J, π, branching ratios.

doi: 10.1103/PhysRevC.76.034315
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2007RZ01      Phys.Rev. C 75, 054319 (2007)

T.Rzaca-Urban, K.Pagowska, W.Urban, A.Zlomaniec, J.Genevey, J.A.Pinston, G.S.Simpson, M.S.Sarkar, S.Sarkar, H.Faust, A.Scherillo, I.Tsekhanovich, R.Orlandi, J.L.Durell, A.G.Smith, I.Ahmad

First observation of excited states in the 138I nucleus

RADIOACTIVITY 138I [from 248Cm(SF)]; measured prompt and delayed Eγ, Iγ. Deduced level energies, J, π.

doi: 10.1103/PhysRevC.75.054319
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2007RZ03      Eur.Phys.J. A 32, 5 (2007)

T.Rzaca-Urban, W.Urban, M.S.Sarkar, S.Sarkar, J.L.Durell, A.G.Smith, B.J.Varley, I.Ahmad

First observation of medium-spin excitations in the 138Cs nucleus

RADIOACTIVITY 138Cs(IT) [from 248Cm(SF)]; measured Eγ, Iγ, γγ-coinc. 138Cs deduced levels, J, π.

doi: 10.1140/epja/i2007-10362-1
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2006DO29      Phys.Rev.C 74, 065204 (2006)

M.Doring, E.Oset, S.Sarkar

Radiative decay of the Λ*(1520)

doi: 10.1103/PhysRevC.74.065204
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2006GH03      Chin.Phys.Lett. 23, 1441 (2006)

D.Ghosh, A.Dev, S.Sarkar, P.K.Haldar

Pronounced Fluctuations of Target Fragments in Forward Hemisphere Only in Ultra Relativistic Nuclear Collision

NUCLEAR REACTIONS Ag, Br(32S, X), E=200 GeV/nucleon; analyzed fragments multiplicity and angular distributions, dynamical fluctuations.

doi: 10.1088/0256-307X/23/6/023
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2006GH13      Fizika(Zagreb) B 15, 207 (2006)

D.Ghosh, A.Deb, S.Sarkar, S.D.Sengupta, A.Gupta, A.Kumar

Measurement of charge of projectile fragments-search for fractionally-charged projectile fragments and energy 14.5 AGeV

NUCLEAR REACTIONS Ag, Br(28Si, X), E=14.5 GeV/nucleon; measured fragment charge distributions. No fractional charge seen. Lacunarity method.


2006HY01      Phys.Rev. C 73, 035209 (2006); Erratum Phys.Rev. C 75, 029901 (2007)

T.Hyodo, S.Sarkar, A.Hosaka, E.Oset

Coupling of (K-bar)* N to the Λ(1520)

doi: 10.1103/PhysRevC.73.035209
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2006KR07      Eur.Phys.J. A 29, 151 (2006)

Krishichayan, A.Chakraborty, S.Mukhopadhyay, S.Ray, N.S.Pattabiraman, S.S.Ghugre, R.Goswami, A.K.Sinha, S.Sarkar, U.Garg, P.V.Madhusudhana Rao, S.K.Basu, B.K.Yogi, L.Chaturvedi, A.Dhal, R.K.Sinha, M.S.Sarkar, S.Saha, R.Singh, R.K.Bhowmik, A.Jhingan, N.Madhavan, S.Muralithar, S.Nath, R.P.Singh, P.Sugathan

Spin-parity measurements in the neutron-rich N ∼ 20 34P and 36S nuclei

NUCLEAR REACTIONS 115In(34S, X)34P/36S/146Tb/145Gd/146Gd, E=140 MeV; measured Eγ, Iγ, γγ-coin, γ-ray polarization. 34P, 36S deduced levels, J, π, configurations.

doi: 10.1140/epja/i2006-10084-x
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2006KS01      Phys.Rev. C 74, 034314 (2006)

R.Kshetri, M.S.Sarkar, S.Sarkar

Evolution of collectivity in neutron-rich nuclei in the 132Sn region

NUCLEAR STRUCTURE 137,139Te, 137,139I, 139,141Xe, 139Cs, 141Ba; calculated levels, J, π, configurations. Particle rotor model, comparison with data.

doi: 10.1103/PhysRevC.74.034314
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2006OS03      Pramana 66, 731 (2006)

E.Oset, D.Cabrera, V.K.Magas, L.Roca, S.Sarkar, M.J.Vicente Vacas, A.Ramos

Chiral dynamics of baryon resonances and hadrons in a nuclear medium

doi: 10.1007/BF02704803
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2006RO18      Phys.Rev. C 73, 045208 (2006)

L.Roca, S.Sarkar, V.K.Magas, E.Oset

Unitary coupled channel analysis of the Λ(1520) resonance

NUCLEAR REACTIONS 1H(K-, 2π0X), (K-, π+π-X), E not given; analyzed hyperon production σ. 1H(γ, K+K-), E=2.8-4.8 GeV; 1H(π-, K0K-), E at 2.9-3.3 GeV/c; analyzed invariant mass distributions. Resonance production data discussed.

doi: 10.1103/PhysRevC.73.045208
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2006UR02      Eur.Phys.J. A 27, 257 (2006)

W.Urban, M.Saha-Sarkar, S.Sarkar, T.Rzaca-Urban, J.L.Durell, A.G.Smith, J.A.Genevey, J.A.Pinston, G.S.Simpson, I.Ahmad

New information on the T1/2 = 47 s isomer in the 136I nucleus

RADIOACTIVITY 248Cm(SF); measured Eγ, Iγ, γγ-coin. 136I deduced levels, J, π, ICC, configurations. Eurogam2 array.

doi: 10.1140/epja/i2005-10273-1
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2005CH65      Phys.Rev. C 72, 054309 (2005)

A.Chakraborty, Krishichayan, S.S.Ghugre, R.Goswami, S.Mukhopadhyay, N.S.Pattabiraman, S.Ray, A.K.Sinha, S.Sarkar, P.V.Madhusudhana Rao, U.Garg, S.K.Basu, M.B.Chatterjee, M.S.Sarkar, L.Chaturvedi, A.Dhal, R.K.Sinha, I.M.Govil, R.K.Bhowmik, A.Jhingan, N.Madhavan, S.Muralithar, S.Nath, R.P.Singh, P.Sugathan

Spectroscopy of 90Nb at high spin

NUCLEAR REACTIONS 63Cu(31P, n3p), E=120, 125 MeV; measured prompt and delayed Eγ, Iγ, γγ-, (recoil)γ-coin. 90Nb deduced levels, J, π, configurations, isomeric states T1/2, B(E2). Large-basis shell model calculations.

doi: 10.1103/PhysRevC.72.054309
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2005HO02      Astropart.Phys. 23, 1 (2005)

D.Hooper, A.Taylor, S.Sarkar

The impact of heavy nuclei on the cosmogenic neutrino flux

NUCLEAR REACTIONS 1H, 4He, 16O, 56Fe(γ, νX), E(cm)=high; calculated neutrino spectra arising from nuclear interactions with cosmic microwave background.

doi: 10.1016/j.astropartphys.2004.11.002
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2005SA11      Nucl.Phys. A750, 294 (2005); Erratum Nucl.Phys. A780, 90 (2006)

S.Sarkar, E.Oset, M.J.Vicente Vacas

Baryonic resonances from baryon decuplet-meson octet interaction

doi: 10.1016/j.nuclphysa.2005.01.006
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2005SA26      Eur.Phys.J. A 24, 287 (2005)

S.Sarkar, E.Oset, M.J.Vicente Vacas

Study of a possible S = + 1 dynamically generated baryonic resonance

doi: 10.1140/epja/i2005-10006-6
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2005SA39      Nucl.Phys. A755, 665c (2005)

S.Sarkar, E.Oset, M.J.Vicente Vacas

Baryonic Resonances from Baryon Decuplet-Meson Octet Interactions and the Exotic Resonance S = 1, I = 1, JP = 3/2-

doi: 10.1016/j.nuclphysa.2005.03.091
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2005SA41      Phys.Rev. C 72, 015206 (2005)

S.Sarkar, E.Oset, M.J.Vicente Vacas

Chiral coupled channel dynamics of the Λ(1520) and the K-p → π0π0Λ reaction

NUCLEAR REACTIONS 1H(K-, π0X), E at 350-750 MeV/c; calculated hyperon production associated σ, invariant mass spectra, resonance features. Chiral coupled channels approach.

doi: 10.1103/PhysRevC.72.015206
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2005SA72      Fizika(Zagreb) B 14, 357 (2005)

S.Sarkar, T.D.Goswami

A study of high-energy nuclear disintegration

NUCLEAR REACTIONS C, N, O, Ag, Br(K-, X), E at 1.8 GeV/c; C, N, O, Ag, Br(p, X), E at 20 GeV/c; analyzed data; deduced intermittency exponents, anomalous fractal dimension.


2004AL33      Phys.Rev. C 70, 054901 (2004)

J.-e.Alam, B.Mohanty, A.Rahaman, S.Sarkar, B.Sinha

Lepton interferometry in relativistic heavy ion collisions: A case study

NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=200 GeV/nucleon; calculated electron transverse momentum spectra, two-electron correlation functions, dependence on source radius.

doi: 10.1103/PhysRevC.70.054901
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2004AL34      J.Phys.(London) G30, 1967 (2004)

J.Alam, S.K.Ghosh, P.Roy, S.Sarkar

Role of in-medium hadrons in photon-nucleus reactions: shadowing and dilepton spectrum

NUCLEAR REACTIONS C, Fe, Pb(γ, ee+), E=1.1, 1.5, 2 GeV; calculated dilepton invariant mass spectra, in-medium effects.

doi: 10.1088/0954-3899/30/12/015
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2004CH18      Phys.Rev. C 69, 044303 (2004)

J.M.Chatterjee, M.Saha-Sarkar, S.Bhattacharya, S.Sarkar, R.P.Singh, S.Murulithar, R.K.Bhowmik

In search of collectivity in 95, 97Mo nuclei

NUCLEAR REACTIONS 82Se(18O, 5n), (18O, 3n), E=60 MeV; measured Eγ, Iγ, γγ-coin. 95,97Mo deduced levels, J, π, δ, rotational bands. Comparison with model predictions.

doi: 10.1103/PhysRevC.69.044303
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2004CH35      Phys.Rev. C 70, 014311 (2004)

A.Chakraborty, Krishichayan, S.S.Ghugre, R.Goswami, S.Mukhopadhyay, N.S.Pattabiraman, S.Ray, A.K.Sinha, S.Sarkar, P.V.M.Rao, U.Garg, S.K.Basu, L.Chaturvedi, A.Dhal, R.K.Sinha, I.M.Govil, M.B.Chatterjee, M.S.Sarkar, R.K.Bhowmik, A.Jhingan, N.Madhavan, S.Muralithar, S.Nath, R.P.Singh, P.Sugathan

Lifetime measurements of microsecond isomers in the N = 48 nuclei 88Zr and 90Mo using recoil-isomer tagging

NUCLEAR REACTIONS 63Cu(31P, xnyp)90Mo/88Zr, E=120 MeV; measured prompt and delayed Eγ, Iγ, γγ-, (recoil)γ-coin. 90Mo, 88Zr deduced isomeric states T1/2, B(E2). Recoil-isomer tagging, comparison with model predictions.

doi: 10.1103/PhysRevC.70.014311
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2004GH20      Pramana 63, 963 (2004)

D.Ghosh, A.Deb, A.K.Mallick, S.Sarkar, K.Purkait, R.Sengupta

Strong pionic intermittency in 'cold' events in 12C-AgBr interactions at 4.5 A GeV

NUCLEAR REACTIONS Ag, Br(12C, X), E=4.5 GeV/nucleon; analyzed fragments pseudorapidity and multiplicity distributions, scaled factorial moments; deduced intermittency.

doi: 10.1007/BF02704334
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2004KR14      Phys.Rev. C 70, 044315 (2004)

Krishichayan, A.Chakraborty, S.S.Ghugre, R.Goswami, S.Mukhopadhyay, N.S.Pattabiraman, S.Ray, A.K.Sinha, S.Sarkar, P.V.M.Rao, U.Garg, S.K.Basu, B.K.Yogi, L.Chaturvedi, A.Dhal, R.K.Sinha, M.S.Sarkar, S.Saha, R.Singh, R.K.Bhowmik, A.Jhingan, N.Madhavan, S.Muralithar, S.Nath, R.P.Singh, P.Sugathan

High-spin states in the odd-odd nucleus 146Tb

NUCLEAR REACTIONS 115In(34S, 3n), E=140 MeV; measured Eγ, Iγ, γγ-coin, γ-ray polarization. 146Tb deduced high-spin levels, J, π, configurations.

doi: 10.1103/PhysRevC.70.044315
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2004MA08      Phys.Rev. C 69, 015204 (2004)

S.Mallik, S.Sarkar

Pion parameters in nuclear medium from chiral perturbation theory and virial expansion

doi: 10.1103/PhysRevC.69.015204
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2004MA95      Eur.Phys.J. A 22, 371 (2004)

S.Mallik, A.Nyffeler, M.C.M.Rentmeester, S.Sarkar

On the nucleon self-energy in nuclear matter

doi: 10.1140/epja/i2004-10049-1
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2004SA35      Eur.Phys.J. A 21, 61 (2004)

S.Sarkar, M.S.Sarkar

Shell model calculations with modified empirical Hamiltonian in the 132Sn region

NUCLEAR STRUCTURE 134,135,136,137Sn, 134,135,136,137Sb, 134,135,136,137Te, 135,136,137I, 136,137Xe, 137Cs; calculated binding energies. 135Sb, 137I, 136,137Te; calculated levels, J, π. 134Sn, 135Sb, 134,136Te; calculated transitions B(E2). Shell model, modified Hamiltonian, comparison with data.

doi: 10.1140/epja/i2003-10198-7
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2003AL14      Phys.Rev. C 67, 054901 (2003)

J.-e.Alam, P.Roy, S.Sarkar, B.Sinha

Spectral redshift versus broadening from photon and dilepton spectra

NUCLEAR REACTIONS Pb(Pb, X), E=high; calculated pion and proton spectra, photon yields, dilepton spectra. In-medium spectral shift and broadening of vector mesons. Comparison with data.

doi: 10.1103/PhysRevC.67.054901
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2003AL15      Phys.Rev. C 67, 054902 (2003)

J.-e.Alam, B.Mohanty, P.Roy, S.Sarkar, B.Sinha

Photon interferometry and size of the hot zone in relativistic heavy ion collisions

NUCLEAR REACTIONS Pb(Pb, X), E=158 MeV/nucleon; analyzed single-photon spectra; calculated two-photon correlation functions. 197Au(197Au, X), E=high; calculated photon spectra, two-photon correlation functions.

doi: 10.1103/PhysRevC.67.054902
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