NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = R.Chatterjee Found 66 matches. 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
2024SH11 Few-Body Systems 65, 17 (2024) Shubhchintak, G.Singh, R.Chatterjee, M.Dan Radiative Neutron Capture Rate of 11B(n, γ)12B Reaction from the Coulomb Dissociation of 12B NUCLEAR REACTIONS 11B(n, γ), E(cm)<2.5 MeV; 208Pb(12B, X), E(cm)<10 MeV; calculated σ(E), σ, reaction rates. Comparison with available data.
doi: 10.1007/s00601-024-01888-3
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
2023DA06 Phys.Rev. C 107, 044908 (2023) P.Dasgupta, R.Chatterjee, G.-Li.Ma Production and anisotropic flow of thermal photons in collisions of α-clustered carbon with heavy nuclei at relativistic energies
doi: 10.1103/PhysRevC.107.044908
2022TH03 Eur.Phys.J. A 58, 13 (2022) San.Thakur, S.K.Saha, S.Noor Alam, R.Chatterjee, S.Chattopadhyay Longitudinal asymmetry in heavy ion collisions at RHIC
doi: 10.1140/epja/s10050-022-00667-0
2021CH55 Phys.Rev. C 104, 054313 (2021) V.Choudhary, W.Horiuchi, M.Kimura, R.Chatterjee Enormous nuclear surface diffuseness of Ne and Mg isotopes in the island of inversion NUCLEAR STRUCTURE 20,21,22,23,24,25,26,27,28,29,30,31,32,33,34Ne, 24,25,26,27,28,29,30,31,32,33,34,35,36,37,38,39,40Mg; calculated nuclear surface diffuseness as a function of neutron number, occupation numbers; analyzed nuclear surface diffuseness parameters and rms point matter radii from experimental elastic scattering differential cross sections at 350-, 500- and 800-MeV incident energies. 29Ne; calculated valence neutron density distribution. Microscopic antisymmetrized molecular dynamics (AMD) model, and two-parameter Fermi density distribution for the diffuseness parameters and matter radii.
doi: 10.1103/PhysRevC.104.054313
2021CH62 Phys.Rev. C 104, 064907 (2021) Ratio of photon anisotropic flow in relativistic heavy ion collisions
doi: 10.1103/PhysRevC.104.064907
2021DA10 Eur.Phys.J. A 57, 134 (2021) P.Dasgupta, G.-L.Ma, R.Chatterjee, L.Yan, S.Zhang, Y.-G.Ma Thermal photons as a sensitive probe of α-cluster in C + Au collisions at the BNL Relativistic Heavy Ion Collider
doi: 10.1140/epja/s10050-021-00441-8
2021DA12 Eur.Phys.J. A 57, 203 (2021) A description of the structure and electromagnetic breakup of 11Be with microscopic inputs NUCLEAR STRUCTURE 10,11Be; calculated proton and neutron densitydistributions, energy levels, J, π, one-neutron separation energy, spectroscopic factors using AMD and AMD+RGM.
doi: 10.1140/epja/s10050-021-00526-4
2021MA27 Nucl.Phys. A1010, 122194 (2021) Manju, M.Dan, G.Singh, J.Singh, Shubhchintak, R.Chatterjee Exploring the structure of 29Ne NUCLEAR REACTIONS 208Pb(29Ne, X), E=244 MeV/nucleon; calculated several reaction observables to quantify its structural parameters, one-neutron removal σ, σ(θ, E). 28,29Ne; deduced moderate halo.
doi: 10.1016/j.nuclphysa.2021.122194
2021TH09 Nucl.Phys. A1014, 122263 (2021) S.Thakur, S.K.Saha, P.Dasgupta, R.Chatterjee, S.Chattopadhyay PT dependence of the correlation between initial spatial anisotropy and final momentum anisotropies in relativistic heavy ion collisions
doi: 10.1016/j.nuclphysa.2021.122263
2020CH34 Phys.Rev. C 102, 034619 (2020) V.Choudhary, W.Horiuchi, M.Kimura, R.Chatterjee Imprint of a nuclear bubble in nucleon-nucleus diffraction NUCLEAR REACTIONS 22O, 24Ne, 26Mg, 28Si, 30S, 32Ar, 34Ca(p, p), E=325, 550, 800 MeV; calculated reaction probabilities, σ(θ, E) for various bubble parameters using Glauber model. 22O, 24Ne, 26Mg, 28Si, 30S, 32Ar, 34Ca, 34Si; calculated density distributions, rms matter radii, quadrupole deformation parameters β and γ, bubble parameters, neutron and proton occupation probabilities using antisymmetrized molecular dynamics (AMD); deduced prominent bubble structure of 22O.
doi: 10.1103/PhysRevC.102.034619
2019DA05 Phys.Rev. C 99, 035801 (2019) M.Dan, G.Singh, R.Chatterjee, Shubhchintak Neutron capture rates of 18C NUCLEAR REACTIONS 208Pb(19C, X), E=67 MeV/nucleon; calculated σ(E) of elastic Coulomb breakup using finite-range distorted-wave Born approximation (FRDWBA) theory, and compared with experimental data. 18C(n, γ), E=0-0.8 MeV; calculated capture σ(E) and reaction rate using FRDWBA theory, and compared with a previous rates based on Hauser-Feshbach estimates. Relevance to accurate prediction of nucleosynthesis paths such as the r process.
doi: 10.1103/PhysRevC.99.035801
2019MA19 Eur.Phys.J. A 55, 5 (2019) Manju, J.Singh, Shubhchintak, R.Chatterjee Low-lying dipole strengths for probable p-wave one-neutron halos in the medium mass region NUCLEAR STRUCTURE 31Ne, 34Na, 37Mg; calculated p-wave one-neutron halo nuclei at zero deformation radius, dipole strength distribution vs energy in continuum for low-lying state with and without correction factor using relative energy spectra in Coulomb dissociation of 31Ne, 34Na, 37Mg on 208Pb at 100, 234, 244 MeV/nucleon as a base to calculate dipole strength distribution. FRDWBA theory.
doi: 10.1140/epja/i2019-12679-4
2018CH52 Prog.Part.Nucl.Phys. 103, 67 (2018) Breakup reactions of light and medium mass neutron drip line nuclei
doi: 10.1016/j.ppnp.2018.06.001
2018DA04 Phys.Rev. C 97, 034902 (2018) P.Dasgupta, R.Chatterjee, S.K.Singh, J.Alam Effects of initial-state nucleon shadowing on the elliptic flow of thermal photons
doi: 10.1103/PhysRevC.97.034902
2018DA19 Phys.Rev. C 98, 024911 (2018) P.Dasgupta, S.De, R.Chatterjee, D.K.Srivastava Photon production from Pb + Pb collisions at √ sNN = 5.02 TeV at the CERN Large Hadron Collider and at √ sNN = 39 TeV at the proposed Future Circular Collider facility
doi: 10.1103/PhysRevC.98.024911
2018SR02 Phys.Rev. C 97, 064910 (2018) D.K.Srivastava, R.Chatterjee, S.A.Bass Transport dynamics of parton interactions in pp collisions at energies available at the CERN Large Hadron Collider
doi: 10.1103/PhysRevC.97.064910
2018SR04 Phys.Rev. C 98, 054910 (2018) D.K.Srivastava, R.Chatterjee, S.A.Bass Landau-Pomeranchuk-Midgal effect and charm production in pp collisions at energies available at the CERN Large Hadron Collider using the parton cascade model
doi: 10.1103/PhysRevC.98.054910
2017CH30 Phys.Rev. C 96, 014911 (2017) R.Chatterjee, P.Dasgupta, D.K.Srivastava Anisotropic flow of thermal photons at energies available at the BNL Relativistic Heavy Ion Collider and at the CERN Large Hadron Collider
doi: 10.1103/PhysRevC.96.014911
2017DA14 Phys.Rev. C 95, 064907 (2017) P.Dasgupta, R.Chatterjee, D.K.Srivastava Spectra and elliptic flow of thermal photons from full-overlap U+U collisions at energies available at the BNL Relativistic Heavy Ion Collider
doi: 10.1103/PhysRevC.95.064907
2017SH28 Phys.Rev. C 96, 025804 (2017) Shubhchintak, R.Chatterjee, R.Shyam Determination of the 36Mg (n, γ) 37Mg reaction rate from Coulomb dissociation of 37Mg NUCLEAR REACTIONS 208Pb(37Mg, X), E=244 MeV/nucleon; calculated Coulomb dissociation (CD) cross section in the framework of a finite-range distorted-wave Born approximation theory with the inclusion of the projectile deformation effects. 36Mg(n, γ)37Mg, E=0.01-3 MeV; calculated direct capture (DC) σ(E) to the ground state of 37Mg. 37Mg; calculated asymptotic normalization constant (ANC) for the deformed 37Mg wave function. 36Mg(n, γ)37Mg, T=0.05-3 GK; calculated capture rates as a function of temperature and S(n). 36Mg(α, n)39Si, T=0.05-3 GK; compared reaction rates for this reaction using Hauser-Feshbach (HF) method with those for 36Mg(n, γ)37Mg.
doi: 10.1103/PhysRevC.96.025804
2017SI15 Phys.Rev. C 95, 065806 (2017) G.Singh, Shubhchintak, R.Chatterjee Structural effects of 34Na in the 33Na (n, γ) 34Na radiative capture reaction NUCLEAR REACTIONS 33Na(n, γ), E(cm)=0-5 MeV; calculated capture σ(E) as function of deformation parameter β2, valence neutron binding energy, and as function of astrophysical temperatures of T9=0.05 to 10, kinematic factor as function of incident neutron energy, virtual photon number as function of the center-of-mass energy of the two photo-dissociated fragments. Quantum mechanical theory of finite-range distorted-wave Born approximation upgraded to include deformation effects. Comparison with reaction rate for 33Na(α, n)36Al reaction calculated using Hauser-Feshbach (HF) theory and the NON-SMOKER code.
doi: 10.1103/PhysRevC.95.065806
2017SR06 Phys.Rev. C 96, 064906 (2017) D.K.Srivastava, S.A.Bass, R.Chatterjee Production of charm quarks in a parton cascade model for relativistic heavy ion collisions at √ sNN = 200 GeV
doi: 10.1103/PhysRevC.96.064906
2016BA56 Phys.Rev. C 94, 044901 (2016) S.Basu, S.Chatterjee, R.Chatterjee, T.K.Nayak, B.K.Nandi Specific heat of matter formed in relativistic nuclear collisions
doi: 10.1103/PhysRevC.94.044901
2016CH28 Phys.Rev. C 94, 014903 (2016) R.Chatterjee, D.K.Srivastava, T.Renk Triangular flow of thermal photons from an event-by-event hydrodynamic model for 2.76A TeV Pb + Pb collisions at the CERN Large Hadron Collider
doi: 10.1103/PhysRevC.94.014903
2016SH18 Phys.Rev. C 93, 059802 (2016) Shubhchintak, Neelam, R.Chatterjee Reply to "Comment on `Structure effects in the 15N(n, γ)16N radiative capture reaction from the Coulomb dissociation of 16N" NUCLEAR REACTIONS 15N(n, γ)16N, E(cm)<0.5 MeV; analyzed branching ratio and spectroscopic factors to various states in 16N, total nonresonant cross section compared with experimental data.
doi: 10.1103/PhysRevC.93.059802
2016SI19 Eur.Phys.J. A 52, 209 (2016) J.Singh, L.Fortunato, A.Vitturi, R.Chatterjee Electric multipole response of the halo nucleus 6He NUCLEAR STRUCTURE 6He; calculated halo nucleus configuration of 0+1 gs, radius, mean-square distance between valence neutrons, distance between their centre and the core, monopole E0, dipole E1, octupole E3 transition strength distributions, B(E1), B(E3), levels, J, π. Model using different continuum components of weakly bound 6He halo nucleus with unbound 5He spd waves. Compared with published calculations.
doi: 10.1140/epja/i2016-16209-8
2016SI21 Phys.Rev. C 94, 024606 (2016) G.Singh, Shubhchintak, R.Chatterjee Elastic Coulomb breakup of 34Na NUCLEAR REACTIONS 208Pb(34Na, 34Na), (34Na, 33Na), E=100 MeV/nucleon; calculated triple differential cross section for the breakup process, total cross-section, parallel momentum distribution, angular distributions, average momenta, energy-angular distributions, total one-neutron removal cross section. 34Na; calculated relative energy spectra due to Coulomb dissociation; analyzed ground state configurations in the context of 'island of inversion', neutron halo structure, configuration. Quantum mechanical Coulomb breakup theory with finite range distorted wave Born approximation (DWBA). Relevance to production of seed nuclei in the alternate r-process paths in nucleosynthesis.
doi: 10.1103/PhysRevC.94.024606
2015NE14 Phys.Rev. C 92, 044615 (2015) Neelam, Shubhchintak, R.Chatterjee Structure effects in the 15N (n, γ) 16N radiative capture reaction from the Coulomb dissociation of 16N NUCLEAR REACTIONS Pb(16N, X), E=100 MeV/nucleon; calculated relative energy spectra in Coulomb breakup of 16N on Pb, total one-neutron removal sections for four low-lying states in 16N; deduced photodisintegration cross sections for 15N(γ, n) reaction four low-lying (2-, 0-, 3-, 1-) states of 16N using quantum mechanical Coulomb breakup theory under the post-form finite range distorted wave Born approximation (FRDWBA). 15N(n, γ), E(cm)<0.5 MeV; deduced σ(E) from principle of detailed balance, astrophysical nuclear reaction rates for T9=0.05-3. 16N; calculated spectroscopic factors for four low-lying levels. Comparison of astrophysical reaction rates with other theoretical results and NACRE database.
doi: 10.1103/PhysRevC.92.044615
2015SH20 Nucl.Phys. A939, 101 (2015) Shubhchintak, Neelam, R.Chatterjee, R.Shyam, K.Tsushima Coulomb breakup of 37Mg and its ground state structure NUCLEAR REACTIONS Pb(37Mg, x), E=244 MeV/nucleon; calculated pure Coulomb one-neutron removal σ, σ(E), σ(E, θ) vs neutron separation energy and vs deformation, parallel momentum distribution using FR DWBA.
doi: 10.1016/j.nuclphysa.2015.03.011
2014FO20 Phys.Rev. C 90, 064301 (2014) L.Fortunato, R.Chatterjee, J.Singh, A.Vitturi Pairing in the continuum: The quadrupole response of the Borromean nucleus 6He NUCLEAR STRUCTURE 6He; calculated levels, J, π, B(E2) strength distribution, Borromean character of the bound ground state. Shell model calculations in a basis of two-particle states built out of continuum p states of the unbound 5He nucleus, and using a simple pairing contact-delta interaction. Comparison with experimental results.
doi: 10.1103/PhysRevC.90.064301
2014SH02 Nucl.Phys. A922, 99 (2014) Deformation effects in the Coulomb breakup of 31Ne NUCLEAR REACTIONS Pb(31Ne, X), E=234 MeV/nucleon; calculated, analyzed Coulomb breakup σ, σ(θ) data vs deformation and 1n Q using. Compared to data.
doi: 10.1016/j.nuclphysa.2013.11.010
2014SH16 Phys.Rev. C 90, 017602 (2014) Breakdown of the N=8 magic number near the neutron drip line from parallel momentum distribution analyses NUCLEAR REACTIONS Au(10Be, X), E=100 MeV/nucleon; analyzed FWHM of parallel momentum distribution (PMD) using postform finite range distorted wave Born approximation (FRDWBA) and the adiabatic model (AD). Discussed breakdown of N=8 magic number away from the valley of stability.
doi: 10.1103/PhysRevC.90.017602
2013CH26 Nucl.Phys. A904-905, 849c (2013) R.Chatterjee, H.Holopainen, T.Renk, K.J.Eskola Influence of initial state fluctuations on the production of thermal photons
doi: 10.1016/j.nuclphysa.2013.02.149
2013CH31 Nucl.Phys. A913, 116 (2013) R.Chatterjee, R.Shyam, K.Tsushima, A.W.Thomas Structure and Coulomb dissociation of 23O within the quark-meson coupling model NUCLEAR REACTIONS Pb(23O, n22O), E=422 MeV/nucleon; calculated Coulomb dissociation σ(E), longitudinal momentum distribution using QMC (quark-meson coupling) model. Compared with available data. NUCLEAR STRUCTURE 23N, 23O, 31Ne, 35Mg, 37Na, 45S, 49Ar; calculated valence neutron separation energy, 23O density distribution, neutron, proton radii using QMC (quark-meson coupling) model. Compared with available data.
doi: 10.1016/j.nuclphysa.2013.06.004
2013CH41 Phys.Rev. C 88, 034901 (2013) R.Chatterjee, H.Holopainen, I.Helenius, T.Renk, K.J.Eskola Elliptic flow of thermal photons from an event-by-event hydrodynamic model
doi: 10.1103/PhysRevC.88.034901
2013CH46 Nucl.Phys. 910-911, 207c (2013) R.Chatterjee, H.Holopainen, T.Renk, K.J.Eskola Centrality and initial formation time dependence of the emission of thermal photons from fluctuating initial conditions at RHIC and LHC
doi: 10.1016/j.nuclphysa.2012.12.010
2012CH24 Phys.Rev. C 85, 064910 (2012) R.Chatterjee, H.Holopainen, T.Renk, K.J.Eskola Collision centrality and τ0 dependence of the emission of thermal photons from a fluctuating initial state in an ideal hydrodynamic calculation
doi: 10.1103/PhysRevC.85.064910
2011CH24 Phys.Rev. C 83, 054908 (2011) R.Chatterjee, H.Holopainen, T.Renk, K.J.Eskola Enhancement of thermal photon production in event-by-event hydrodynamics
doi: 10.1103/PhysRevC.83.054908
2011DE23 Nucl.Phys. A862-863, 290c (2011) S.De, D.K.Srivastava, R.Chatterjee Equation of state of strongly interacting matter and intensity interferometry of thermal photons
doi: 10.1016/j.nuclphysa.2011.06.008
2010CH30 Pramana 75, 127 (2010) Progress in all-order breakup reaction theories
doi: 10.1007/s12043-010-0072-1
2009CH05 Phys.Rev. C 79, 021901 (2009) Elliptic flow of thermal photons and formation time of quark gluon plasma at energies available at the BNL Relativistic Heavy Ion Collider (RHIC)
doi: 10.1103/PhysRevC.79.021901
2009CH12 Phys.Rev. C 79, 034906 (2009) R.Chatterjee, D.K.Srivastava, S.Jeon Single photons from relativistic collisions of lead nuclei at energies available at the CERN Super Proton Synchrotron (SPS): A reanalysis
doi: 10.1103/PhysRevC.79.034906
2009CH53 Nucl.Phys. A830, 503c (2009) Formation Time of QGP from Thermal Photon Elliptic Flow
doi: 10.1016/j.nuclphysa.2009.10.043
2009GA37 Nucl.Phys. A830, 579c (2009) C.Gale, R.Chatterjee, D.K.Srivastava, S.Jeon A Reanalysis of Single Photon Data at CERN SPS
doi: 10.1016/j.nuclphysa.2009.10.052
2009MA11 Eur.Phys.J. A 39, 107 (2009) A.Mason, R.Chatterjee, L.Fortunato, A.Vitturi Electric and magnetic response to the continuum for A = 7 isobars in a dicluster model NUCLEAR STRUCTURE 7Li, 7Be; calculated radius, magnetic moment, B(E2), B(M1), differential reduced transition probability. Comparison with data. NUCLEAR REACTIONS 7Li, 7Be(γ, α), E not given; calculated dissociation σ. 3H, 3He(α, γ), E not given; analyzed S-factor and radiative capture σ.
doi: 10.1140/epja/i2008-10685-3
2009SR02 Phys.Rev. C 80, 054914 (2009), Erratum Phys.Rev. C 81, 029901 (2010) Interference of thermal photons from quark and hadronic phases in relativistic collisions of heavy nuclei
doi: 10.1103/PhysRevC.80.054914
2008BA35 Phys.Rev. C 78, 035804 (2008) P.Banerjee, R.Chatterjee, R.Shyam Coulomb dissociation of 9Li and the rate of the 8Li(n, γ)9Li reaction NUCLEAR REACTIONS Pb, U(9Li, X), E(cm)=28.5 MeV/nucleon; measured σ. 8Li(n, γ); deduced astrophysical capture rates.
doi: 10.1103/PhysRevC.78.035804
2008CH08 Eur.Phys.J. A 35, 213 (2008) R.Chatterjee, L.Fortunato, A.Vitturi Role of higher multipole excitations in the electromagnetic dissociation of one-neutron halo nuclei NUCLEAR REACTIONS 208Pb(11Be, n10Be), E=10, 20, 30, 72, 400 MeV/nucleon; 208Pb(19C, n18C), E=67 MeV/nucleon; calculated relative energy spectra, σ, σ(θ) using finite-range DWBA and first-order Coulomb dissociation models.
doi: 10.1140/epja/i2007-10538-7
2008MA57 Int.J.Mod.Phys. E17, 2310 (2008) A.Mason, R.Chatterjee, L.Fortunato, A.Vitturi Electric and magnetic properties for dicluster nuclei 7Li and 7Be NUCLEAR STRUCTURE 7Li, 7Be; calculated radii, dipole magnetic moments, B(E2), B(M1), s-factors. Energy Weighted Molecular Sum Rules (EWMSR) checks.
doi: 10.1142/S0218301308011525
2007CH43 Phys.Rev. C 75, 054909 (2007) R.Chatterjee, D.K.Srivastava, Ul.Heinz, C.Gale Elliptic flow of thermal dileptons in relativistic nuclear collisions NUCLEAR REACTIONS Au(Au, X), E(cm)=200 GeV/nucleon; calculated transverse momentum and invariant mass dependence of elliptic flow of thermal dileptons.
doi: 10.1103/PhysRevC.75.054909
2007CH51 Phys.Rev. C 75, 064604 (2007) Beam energy dependence of Coulomb-nuclear interference in the breakup of 11Be NUCLEAR REACTIONS 44Ti(11Be, X), E=20-40 MeV/nucleon; 208Pb(11Be, X), E=69 MeV/nucleon; calculated breakup cross section and neutron energy distribution within the post-form DWBA.
doi: 10.1103/PhysRevC.75.064604
2007HE03 Nucl.Phys. A783, 379c (2007) U.Heinz, R.Chatterjee, E.Frodermann, C.Gale, D.K.Srivastava Elliptic Flow of Thermal Photons/Dileptons NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=200 GeV/nucleon; calculated elliptic flow for thermal photons and dileptons.
doi: 10.1016/j.nuclphysa.2006.11.090
2006CH08 Nucl.Phys. A764, 528 (2006) R.Chatterjee, J.Okolowicz, M.Ploszajczak Description of the 17F(p, γ)18Ne radiative capture reaction in the continuum shell model NUCLEAR REACTIONS 17F(p, γ), E=0-1 MeV; calculated astrophysical S factor, E1, E2, M1 contributions, reaction rate. Continuum shell model. NUCLEAR STRUCTURE 18Ne; analyzed level energies, widths, spectroscopic factors. Continuum shell model.
doi: 10.1016/j.nuclphysa.2005.10.002
2006CH22 Phys.Rev.Lett. 96, 202302 (2006) R.Chatterjee, E.S.Frodermann, U.Heinz, D.K.Srivastava Elliptic Flow of Thermal Photons in Relativistic Nuclear NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=200 GeV/nucleon; calculated thermal photon elliptic flow, transverse momentum dependence. Hydrodynamic model.
doi: 10.1103/PhysRevLett.96.202302
2006LA25 Phys.Rev. C 74, 044901 (2006) B.Layek, R.Chatterjee, D.K.Srivastava Azimuthal flow of decay photons in relativistic nuclear collisions
doi: 10.1103/PhysRevC.74.044901
2005RO41 Eur.Phys.J. A 25, Supplement 1, 173 (2005) J.Rotureau, R.Chatterjee, J.Okolowicz, M.Ploszajczak Microscopic theory of the two-proton radioactivity RADIOACTIVITY 18Ne(2p); calculated excited state decay widths and branching ratios for sequential and di-proton cluster emission. Real-energy continuum shell model.
doi: 10.1140/epjad/i2005-06-121-2
2003CH65 Phys.Rev. C 68, 044604 (2003) Full quantal theory of one-neutron halo breakup reactions NUCLEAR REACTIONS 9Be, 44Ti, 197Au(11Be, n10Be), E=41 MeV/nucleon; calculated relative energy spectra, parallel momentum distributions, total one-neutron removal σ, Coulomb-nuclear interference terms. DWBA approach.
doi: 10.1103/PhysRevC.68.044604
2002CH60 Phys.Rev. C 66, 061601 (2002) Coulomb-nuclear interference in the breakup of 11Be NUCLEAR REACTIONS 9Be, 44Ti, 197Au(11Be, n10Be), E=41 MeV/nucleon; 208Pb(11Be, n10Be), E=72 MeV/nucleon; calculated breakup σ(θ), σ(E); deduced Coulomb-nuclear interference effects. Post-form DWBA, comparisons with data.
doi: 10.1103/PhysRevC.66.061601
2001CH04 Phys.Rev. C63, 017303 (2001) Structure of the Exotic Nucleus 14B in the Ground State NUCLEAR REACTIONS 197Au(14B, n13B), E=60 MeV/nucleon; calculated fragment parallel momentum distributions, relative energy, neutron σ(θ). 14B deduced ground state configuration. DWBA approach.
doi: 10.1103/PhysRevC.63.017303
2001CH58 Nucl.Phys. A692, 476 (2001) R.Chatterjee, P.Banerjee, R.Shyam Four-Body DWBA Calculations of the Coulomb Breakup of 6He NUCLEAR REACTIONS 197Au(6He, 2nα), E=63.2 MeV/nucleon; U, Pb(6He, 2nα), E= 24 MeV/nucleon; calculated α spectra. Pb(6He, 2nα), E=240 MeV/nucleon; calculated nn, nα relative energy spectra. Four-body postform DWBA approach, comparisons with data.
doi: 10.1016/S0375-9474(01)00651-0
2000CH27 Nucl.Phys. A675, 477 (2000) R.Chatterjee, P.Banerjee, R.Shyam Projectile Structure Effects in the Coulomb Breakup of One-Neutron Halo Nuclei NUCLEAR REACTIONS 197Au(11Be, n10Be), E=37, 44 MeV/nucleon; calculated neutron spectra, energy distributions and average momenta of 10Be, neutron angular distributions. Pb(11Be, n10Be), E=72 MeV/nucleon; calculated relative energy spectra. U, Ta(11Be, n10Be), E=63 MeV/nucleon; Ta(19C, n18C), E=88, 914 MeV/nucleon; Ta(15C, n14C), E=84 MeV/nucleon; calculated parallel momentum distributions. Pb(19C, n18C), E=67 MeV/nucleon; calculated relative energy spectrum. Comparison with data and other models. Reaction mechanisms of halo nuclei.
doi: 10.1016/S0375-9474(00)00179-2
1996CH29 Nucl.Phys. A606, 27 (1996) Surfing Arnold's Web
doi: 10.1016/0375-9474(96)00212-6
1996DA34 Appl.Radiat.Isot. 47, 643 (1996) S.K.Das, A.G.C.Nair, R.K.Chatterjee, R.Guin, S.K.Saha The Performance of the 172Hf-172Lu Generator RADIOACTIVITY 172Hf(EC) [from Yb(α, X), E=45 MeV]; measured γ spectra; deduced 172Hf-172Lu generator development, performance related features.
doi: 10.1016/0969-8043(96)00025-5
1995GH09 Phys.Rev. C52, 2092 (1995) D.Ghosh, M.Lahiri, A.Deb, S.Das, K.Purkait, B.Biswas, J.Roychowdhury, R.Chatterjee, A.K.Zafri Factorial Correlator Study in 32S-Ag/Br Interaction at 200A GeV
doi: 10.1103/PhysRevC.52.2092
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