NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = S.Kaur Found 27 matches. 2024KU04 Phys.Rev. C 109, 014613 (2024) V.Kumar, K.Mahata, S.Dhuri, A.Shrivastava, K.Ramachandran, S.Pandit, V.V.Parkar, A.Chavan, A.Kumar, S.Kaur, P.C.Rout Observation of asymmetric fission in 204Pb at low excitation energies
doi: 10.1103/PhysRevC.109.014613
2023KA03 Phys.Rev. C 107, 014613 (2023) S.Kaur, N.Kaur, R.Kaur, B.B.Singh, S.K.Patra Fusion enhancement within a collective clusterization approach applied to the isotopic chain of neutron-rich light-mass compound nuclei NUCLEAR REACTIONS 12C(12C, X)24Mg, 12C(13C, X)25Mg, 12C(14C, X)26Mg, 12C(15C, X)27Mg, E(cm)=10-15 MeV; calculated fusion σ, fragment mass distribution from Mg compound nucleus fragmentation, fragmentation potential, cluster preformation probability, scattering potential, variation of neck length parameter. Calculations in the framework of dynamical cluster decay model (DCM). Comparison to experimental data.
doi: 10.1103/PhysRevC.107.014613
2023MO07 Phys.Lett. B 839, 137833 (2023) A.Mollaebrahimi, C.Hornung, T.Dickel, D.Amanbayev, G.Kripko-Koncz, W.R.Plass, S.Ayet S.Andres, S.Beck, A.Blazhev, J.Bergmann, H.Geissel, M.Gorska, H.Grawe, F.Greiner, E.Haettner, N.Kalantar-Nayestanaki, I.Miskun, F.Nowacki, C.Scheidenberger, S.Bagchi, D.L.Balabanski, Z.Brencic, O.Charviakova, P.Constantin, M.Dehghan, J.Ebert, L.Grof, O.Hall, M.N.Harakeh, S.Kaur, A.Kankainen, R.Knobel, D.A.Kostyleva, N.Kurkova, N.Kuzminchuk, I.Mardor, D.Nichita, J.-H.Otto, Z.Patyk, S.Pietri, S.Purushothaman, M.P.Reiter, A.-K.Rink, H.Roesch, A.Spataru, G.Stanic, A.State, Y.K.Tanaka, M.Vencelj, H.Weick, J.S.Winfield, M.I.Yavor, J.Zhao Studying Gamow-Teller transitions and the assignment of isomeric and ground states at N = 50 NUCLEAR REACTIONS Be(124Xe, X), E=800 MeV/nucleon; measured reaction products, ToF. 94Ru, 94Rh, 94mRh, 96,97,97mRu, 97Pd, 97,97mAg, 98Pd, 98Cd, 99Ag, 100Pd, 100Ag, 100Cd, 101In; deduced mass excess and Q-values. Comparison with AME2020 evaluation. The FRS Ion Catcher (FRS-IC) at GSI, Germany.
doi: 10.1016/j.physletb.2023.137833
2022DH03 Phys.Rev. C 106, 014616 (2022) S.Dhuri, K.Mahata, A.Shrivastava, K.Ramachandran, S.K.Pandit, V.Kumar, V.V.Parkar, P.C.Rout, A.Kumar, A.Chavan, S.Kaur, T.Santhosh Measurement of mass and total kinetic energy distributions for the 12C + 174Lu system NUCLEAR REACTIONS 175Lu(12C, F), E=58, 65, 70, 75 MeV; measured reaction products; deduced fission fragment mass and total kinetic energy (TKE) distributions. Comparison to the systematics based on liquid drop (LD) behavior. Two position-sensitive multiwire proportional chambers (MWPCs) at BARC-TIFR Pelletron-LINAC facility, Mumbai.
doi: 10.1103/PhysRevC.106.014616
2022KA06 Nucl.Phys. A1018, 122361 (2022) S.Kaur, R.Kaur, B.B.Singh, S.K.Patra Decay analysis of 24, 25Mg* compound nuclei NUCLEAR REACTIONS 12C(12C, X)24Mg, 12C(13C, X)25Mg, E not given; analyzed available data; deduced preformation probabilities, σ, level density parameters.
doi: 10.1016/j.nuclphysa.2021.122361
2022KA13 Nucl.Instrum.Methods Phys.Res. B521, 33 (2022) S.Kaur, V.Ayri, A.Kumar, M.Czyzycki, A.G.Karydas, S.Puri Measurements of L-shell X-ray production cross sections for Sn and Sb using 6-14 keV synchrotron radiation NUCLEAR REACTIONS Sn, Sb(γ, γ'), E=6-14 keV; measured reaction products, X-rays; deduced L-shell X-ray production σ. Comparison with theoretical calculations.
doi: 10.1016/j.nimb.2022.04.010
2022KA26 Nucl.Phys. A1027, 122491 (2022) Systematic study of probable target-projectile combinations for the synthesis of Z = 120 isotopes using the Skyrme energy density formalism NUCLEAR REACTIONS 252Cf(48Ti, X), 250Cf(50Ti, X), 250Cm(50Cr, X), 248Cm(52Cr, X), 226Rn(74Ge, X), 168Re(132Te, X), 164Dy(136Xe, X), 240Pu(60Fe, X), 242Pu(58Fe, X), 236U(64Ni, X), 238U(62Ni, X), 232Th(68Zn, X), 230Th(70Zn, X), 228Rn(72Ge, X)300120, 238U(64Ni, X), 244Pu(58Fe, X), 254Fm(48Ca, X), 248Cm(54Cr, X), 252Cf(50Ti, X), 236U(66Ni, X), 232Th(70Zn, X), 226Rn(76Ge, X), 242Pu(60Fe, X), 274Hs(28Mg, X), 228Th(74Zn, X), 174Yb(128Sn, X), 170Er(132Te, X), 166Dy(136Xe, X)302120, 250Cm(54Cr, X), 244Pu(60Fe, X), 228Rn(76Ge, X), 232Th(72Zn, X), 256Fm(48Ca, X), 250Cf(54Ti, X), 230Th(74Zn, X)304120, E not given; analyzed available data; deduced target-projectile combinations are taken in reference to the minima's of the fragmentation potential calculated using the Quantum Mechanical Fragmentation Theory (QMFT), nuclear interaction potential within the Skyrme energy density formalism (SEDF) using the GSkI force parameters.
doi: 10.1016/j.nuclphysa.2022.122491
2022KA35 Phys.Rev.Lett. 129, 142502 (2022) S.Kaur, R.Kanungo, W.Horiuchi, G.Hagen, J.D.Holt, B.S.Hu, T.Miyagi, T.Suzuki, F.Ameil, J.Atkinson, Y.Ayyad, S.Bagchi, D.Cortina-Gil, I.Dillmann, A.Estrade, A.Evdokimov, F.Farinon, H.Geissel, G.Guastalla, R.Janik, R.Knobel, J.Kurcewicz, Y.A.Litvinov, M.Marta, M.Mostazo, I.Mukha, C.Nociforo, H.J.Ong, T.Otsuka, S.Pietri, A.Prochazka, C.Scheidenberger, B.Sitar, P.Strmen, M.Takechi, J.Tanaka, I.Tanihata, S.Terashima, J.Vargas, H.Weick, J.S.Winfield Proton Distribution Radii of 16-24O: Signatures of New Shell Closures and Neutron Skin NUCLEAR REACTIONS 12C(16O, X), (18O, X), (19O, X), (20O, X), (21O, X), (22O, X), (23O, X), (24O, X), E<1 GeV/nucleon; measured reaction products. 16,18,20,21,22,23,24O; deduced charge changing σ, root mean square proton and matter radii, neutron skin thickness, shell closure. Comparison with with ab initio calculations employing the chiral NNLO sat interaction, shell model predictions. The fragment separator FRS at GSI.
doi: 10.1103/PhysRevLett.129.142502
2022PA33 Eur.Phys.J.Plus 137, 1115 (2022) D.Pathak, P.Singh, H.Parshad, S.Monga, S.Kaur, H.Kaur Systematics of the spontaneous and simultaneous emission of 2α-particles RADIOACTIVITY 146,148Nd, 148,150,152Sm, 152,154Gd, 156,158Dy, 162,164,166Er, 168,170,172,174Yb, 174,176,178,180Hf, 180,182,184,186W, 184,186,188,190,192Os, 190,192,194,196Pt, 196,198,200Hg, 204,206Pb, 194Rn, 210Rn, 216,218Rn, 210Ra, 216,218,220Ra, 218,220,222Th, 232Th, 220,222,224U, 234U, 238U, 314,316126(2α); calculated T1/2, Q-values employing tunneling and the periodic-orbit and BCS theories within microscopic-macroscopic formalism.
doi: 10.1140/epjp/s13360-022-03309-y
2022SP03 Nucl.Instrum.Methods Phys.Res. B522, 32 (2022) A.Spataru, C.Hornung, T.Dickel, E.Haettner, S.Pietri, S.Ayet San Andres, S.Bagchi, D.L.Balabanski, J.Bergmann, J.Ebert, A.Finley, H.Geissel, F.Greiner, O.Hall, S.Kaur, W.Lippert, I.Miskun, J.-H.Otto, W.R.Plass, A.Prochazka, S.Purushothaman, C.Rappold, A.-K.Rink, C.Scheidenberger, Y.K.Tanaka, H.Toernqvist, H.Weick, J.S.Winfield First coupling of the FRS particle identification and the FRS-Ion Catcher data acquisition systems: The case of 109In NUCLEAR REACTIONS 9Be(124Xe, X)109In, E=600 MeV/nucleon; measured reaction products; deduced mass-to-charge spectrum of ground state and two isomeric states. The FRagment Separator (FRS) and the Multiple-Reflection Time-Of-Flight Mass-Spectrometer (MR-TOF-MS) particle identification (PID) systems at GSI.
doi: 10.1016/j.nimb.2022.04.003
2020BA27 Phys.Rev.Lett. 124, 222504 (2020) S.Bagchi, R.Kanungo, Y.K.Tanaka, H.Geissel, P.Doornenbal, W.Horiuchi, G.Hagen, T.Suzuki, N.Tsunoda, D.S.Ahn, H.Baba, K.Behr, F.Browne, S.Chen, M.L.Cortes, A.Estrade, N.Fukuda, M.Holl, K.Itahashi, N.Iwasa, G.R.Jansen, W.G.Jiang, S.Kaur, A.O.Macchiavelli, S.Y.Matsumoto, S.S.Momiyama, I.Murray, T.Nakamura, S.J.Novario, H.J.Ong, T.Otsuka, T.Papenbrock, S.Paschalis, A.Prochazka, C.Scheidenberger, P.Schrock, Y.Shimizu, D.Steppenbeck, H.Sakurai, D.Suzuki, H.Suzuki, M.Takechi, H.Takeda, S.Takeuchi, R.Taniuchi, K.Wimmer, K.Yoshida Two-Neutron Halo is Unveiled in 29F NUCLEAR REACTIONS C(29F, X), E=255 MeV/nucleon; C(27F, X), E=250 MeV/nucleon; measured reaction products, En, In. 27,29F; deduced two-neutron Borromean halo. Comparison with theoretical calculations.
doi: 10.1103/PhysRevLett.124.222504
2020HO03 Phys.Lett. B 802, 135200 (2020) C.Hornung, D.Amanbayev, I.Dedes, G.Kripko-Koncz, I.Miskun, N.Shimizu, S.Ayet S.Andres, J.Bergmann, T.Dickel, J.Dudek, J.Ebert, H.Geissel, M.Gorska, H.Grawe, F.Greiner, E.Haettner, T.Otsuka, W.R.Plass, S.Purushothaman, A.-Ka.Rink, C.Scheidenberger, H.Weick, S.Bagchi, A.Blazhev, O.Charviakova, D.Curien, A.Finlay, S.Kaur, W.Lippert, J.-H.Otto, Z.Patyk, S.Pietri, Y.K.Tanaka, Y.Tsunoda, J.S.Winfield Isomer studies in the vicinity of the doubly-magic nucleus 100Sn: Observation of a new low-lying isomeric state in 97Ag RADIOACTIVITY 97Ag, 101,103,105,107,109In(IT) [from 9Be(124Xe, X), E=600 MeV/nucleon]; measured decay products, mass-to-charge spectra; deduced mass excess, excitation energies. Comparison with shell model calculations.
doi: 10.1016/j.physletb.2020.135200
2020KA20 Phys.Rev. C 101, 034614 (2020) R.Kaur, S.Kaur, B.B.Singh, B.S.Sandhu, S.K.Patra Clustering effects in the exit channels of 13, 12C + 12C reactions within the collective clusterization mechanism of the dynamical cluster decay model NUCLEAR REACTIONS 12C(12C, X)24Mg*, (12C, 6Li), (12C, 7Li), (12C, 7Be), (12C, 8Be), (12C, 9Be), (12C, X)25Mg*, (13C, 6Li), (13C, 7Li), (13C, 7Be), (13C, 8Be), (13C, 9Be), E*=53.9 MeV; calculated fragmentation potential, fragment preformation probability, l-summed preformation probability, scattering potential, barrier potential, penetration probability, and σ(25Mg*)/σ(24Mg*). Dynamical cluster decay model (DCM). Comparison with experimental data, and with other theoretical predictions. Discussed role of α-clustering in heavy-ion reactions.
doi: 10.1103/PhysRevC.101.034614
2019AN10 Phys.Rev. C 99, 064313 (2019), Erratum Phys.Rev. C 107, 029901 (2023) S.A.S.Andres, C.Hornung, J.Ebert, W.R.Plass, T.Dickel, H.Geissel, C.Scheidenberger, J.Bergmann, F.Greiner, E.Haettner, C.Jesch, W.Lippert, I.Mardor, I.Miskun, Z.Patyk, S.Pietri, A.Pihktelev, S.Purushothaman, M.P.Reiter, A.-K.Rink, H.Weick, M.I.Yavor, S.Bagchi, V.Charviakova, P.Constantin, M.Diwisch, A.Finlay, S.Kaur, R.Knobel, J.Lang, B.Mei, I.D.Moore, J.-H.Otto, I.Pohjalainen, A.Prochazka, C.Rappold, M.Takechi, Y.K.Tanaka, J.S.Winfield, X.Xu High-resolution, accurate multiple-reflection time-of-flight mass spectrometry for short-lived, exotic nuclei of a few events in their ground and low-lying isomeric states ATOMIC MASSES 93,94Ru, 94Rh, 96,97Pd, 100Ag, 107Cd, 114,116,133,134Te, 114,134Sb, 117,119,133,134I, 119Xe, 124,125,126Cs, 211,212,213Fr, 211Po, 212,213,218,220Rn, 212,217At; 134mSb, 133mTe, 133m,134mI, 134mXe, 211mPo; measured mass excess and isomer energies using multiple-reflection time-of-flight mass spectrometry (MR-TOF-MS) with the FRS Ion Catcher at GSI. Isotopes produced in 9Be(238U, F), E=300, 1000 MeV/nucleon; 9Be(124Xe, X), E=600 MeV/nucleon reactions using FRS separator at GSI. Comparison with AME-2016 evaluation. Systematics of S(2n) values in N=123-136 Pb, Bi, Po, At, Rn, Fr, Ra, Ac, Th isotopes, and compared with theoretical predictions.
doi: 10.1103/PhysRevC.99.064313
2019BA11 Phys.Lett. B 790, 251 (2019) S.Bagchi, R.Kanungo, W.Horiuchi, G.Hagen, T.D.Morris, S.R.Stroberg, T.Suzuki, F.Ameil, J.Atkinson, Y.Ayyad, D.Cortina-Gil, I.Dillmann, A.Estrade, A.Evdokimov, F.Farinon, H.Geissel, G.Guastalla, R.Janik, S.Kaur, R.Knobel, J.Kurcewicz, Yu.A.Litvinov, M.Marta, M.Mostazo, I.Mukha, C.Nociforo, H.J.Ong, S.Pietri, A.Prochazka, C.Scheidenberger, B.Sitar, P.Strmen, M.Takechi, J.Tanaka, Y.Tanaka, I.Tanihata, S.Terashima, J.Vargas, H.Weick, J.S.Winfield Neutron skin and signature of the N = 14 shell gap found from measured proton radii of 17-22N NUCLEAR REACTIONS C(14N, X), (15N, X), (17N, X), (18N, X), (19N, X), (20N, X), (21N, X), (22N, X), E=851-932 MeV/nucleon; measured reaction products. 14,15,17,18,19,20,21,22N; deduced σ, root mean square point proton and matter radii, unconventional shell gap at N = 14 arising from the attractive proton–neutron tensor interaction. Comparison with ab initio calculations.
doi: 10.1016/j.physletb.2019.01.024
2019KA05 Phys.Rev. C 99, 014614 (2019) M.Kaur, B.B.Singh, S.Kaur, R.K.Gupta N/Z dependence of decay channels in A=80 compound nuclei NUCLEAR REACTIONS 40Ca(40Ca, X)80Zr*, E(cm)=62.14 MeV; 64Zn(16O, X)80Sr*, E(cm)=48.0 MeV; 48Ca(32S, X)80Kr*, E(cm)=39.8 MeV; calculated radial scattering potential profiles, fragmentation potential, preformation and penetration probability probabilities as function of fragment mass and angular momentum, fusion σ for emission of light particles, intermediate mass fragments, and symmetric mass fragments. Dynamical cluster-decay model. Comparison with experimental values of fusion σ.
doi: 10.1103/PhysRevC.99.014614
2019RA06 Phys.Rev. C 99, 021301 (2019) J.S.Randhawa, R.Kanungo, M.Holl, J.D.Holt, P.Navratil, S.R.Stroberg, G.Hagen, G.R.Jansen, M.Alcorta, C.Andreoiu, C.Barnes, C.Burbadge, D.Burke, A.A.Chen, A.Chester, G.Christian, S.Cruz, B.Davids, J.Even, G.Hackman, J.Henderson, S.Ishimoto, P.Jassal, S.Kaur, M.Keefe, D.Kisliuk, R.Krucken, J.Liang, J.Lighthall, E.McGee, J.Measures, M.Moukaddam, E.Padilla-Rodal, A.Shotter, I.J.Thompson, J.Turko, M.Williams, O.Workman Observation of excited states in 20Mg sheds light on nuclear forces and shell evolution NUCLEAR REACTIONS 2H(20Mg, d), (20Mg, d'), E=8.5 MeV/nucleon, [secondary 20Mg beam produced in Si(p, X), E=480 MeV fragmentation reaction using SiC target at ISAC-II facility]; measured scattered deuteron spectra, differential σ(θ) using annular single-sided silicon strip detector array and CsI(Tl) detectors (IRIS reaction spectroscopy facility) at TRIUMF. 20Mg; deduced levels, J, π, proton-unbound resonances. Comparison with ab initio calculations using the valence-space in-medium similarity renormalization-group (VS-IMSRG) approach.
doi: 10.1103/PhysRevC.99.021301
2018KA53 Phys.Rev. C 98, 064612 (2018) R.Kaur, M.Kaur, V.Singh, S.Kaur, B.B.Singh, B.S.Sandhu Investigating the fusion enhancement for neutron-rich mid-mass nuclei using the dynamical cluster-decay model NUCLEAR REACTIONS 28Si(39K, X)67As*,28Si(40K, X)68As*,28Si(41K, X)69As*,28Si(45K, X)73As*,28Si(46K, X)74As*,28Si(47K, X)75As*, E(cm)=36.8-42.6 MeV; calculated fragment potentials and l-summed preformation probability as a function of fragment mass number, scattering potentials for the compound nuclei decaying through one-proton and one-neutron channels, barrier lowering as function of incident energy, summed penetration probabilities, fusion σ(E), -summed fragment cross sections using dynamical cluster-decay model (DCM). Comparison with available experimental data.
doi: 10.1103/PhysRevC.98.064612
2017TA30 Phys.Lett. B 774, 268 (2017) J.Tanaka, R.Kanungo, M.Alcorta, N.Aoi, H.Bidaman, C.Burbadge, G.Christian, S.Cruz, B.Davids, A.Diaz Varela, J.Even, G.Hackman, M.N.Harakeh, J.Henderson, S.Ishimoto, S.Kaur, M.Keefe, R.Krucken, K.G.Leach, J.Lighthall, E.Padilla-Rodal, J.S.Randhawa, P.Ruotsalainen, A.Sanetullaev, J.K.Smith, O.Workman, I.Tanihata Halo-induced large enhancement of soft dipole excitation of 11Li observed via proton inelastic scattering NUCLEAR REACTIONS 1H(11Li, p'), E=66 MeV; measured reaction products, Ep, Ip. 11Li; deduced σ(θ), B(E1). DWBA calculations.
doi: 10.1016/j.physletb.2017.09.079
2015KA12 Acta Phys.Pol. B46, 463 (2015) Structural Effects on the Peak Production of Fragments NUCLEAR REACTIONS 93Nb(86Kr, X), E=50 MeV/nucleon; calculated reaction fragment parameters, time evolution, multiplicities.
doi: 10.5506/APhysPolB.46.463
2014KA18 Acta Phys.Pol. B45, 463 (2014) Isospin Effects on the Transverse Momentum Spectra of Protons and Neutrons
doi: 10.5506/APhysPolB.45.463
2014KA24 Phys.Rev. C 89, 057603 (2014) Systematic study of isospin effects in the dlike/Plike ratio and entropy production
doi: 10.1103/PhysRevC.89.057603
2014KA43 Phys.Rev. C 90, 037602 (2014) Role of model ingredients in the production of light particles and entropy
doi: 10.1103/PhysRevC.90.037602
2014KU27 Chin.Phys.Lett. 31, 112501 (2014) Proximity Approach to Study the Fusion Barriers for Proton and Helium Induced Reactions
doi: 10.1088/0256-307X/31/11/112501
2013KA05 Phys.Rev. C 87, 014620 (2013) Isospin effects on the energy of peak mass production NUCLEAR REACTIONS Ne(Ne, X), Ca(Ca, X), 34Al(34Al, X), 34Cl(34Cl, X), Ni(Ni, X), 60Mn(60Mn, X), 60Zn(60Zn, X), Zr(Zr, X), Sn(Sn, X), Xe(Xe, X), 120Pd(120Pd, X), E=8-40 MeV/nucleon; calculated peak center-of-mass energy and average multiplicity of intermediate mass fragments (IMFs). A=24-34 for Ne+Ne, A=40-60 for Ca+Ca, A=56-84 for Ni+Ni, A=80-120 for Zr+Zr, A=100-150 for Sn+Sn, and A=110-162 for Xe+Xe systems. Isospin-dependent quantum molecular dynamics (IQMD) model. Comparison with experimental data.
doi: 10.1103/PhysRevC.87.014620
2010KA31 Phys.Rev. C 82, 054611 (2010) Model ingredients and peak mass production in heavy-ion collisions NUCLEAR REACTIONS 20Ne(20Ne, X), E=10-55 MeV/nucleon; 45Sc(40Ar, X), E=35-115 MeV/nucleon; 58Ni(58Ni, X), E=35-105 MeV/nucleon; 93Nb(86Kr, X), E=35-95 MeV/nucleon; 118Sn(129Xe, X), E=45-140 MeV; 197Au(86Kr, X), E=35-400 MeV; 197Au(197Au, X), E=70-150 MeV/nucleon; calculated time evolution of intermediate mass fragments (IMF), mean IMF multiplicity, multiplicities of free nucleons, LCPs, MMFs, HMFs, and IMFs as a function of composite mass of the colliding nuclei, binding energies/nucleon for different fragments using quantum molecular dynamics (QMD) model at different incident energies for different equations of state, different binary cross sections, and different widths of Gaussians. Comparison with experimental data.
doi: 10.1103/PhysRevC.82.054611
1987KA31 Phys.Rev. C36, 1016 (1987); Erratum Phys.Rev C42, 1158 (1990) Spin Density and the Real Part of the Heavy-Pion Potential NUCLEAR REACTIONS 60Ni, 48Ca, 90Zr(16O, 16O), (40Ca, 40Ca), E not given; calculated potential vs internucleus distance; deduced spin-density term contribution. Vautherin-Brink energy density functional method.
doi: 10.1103/PhysRevC.36.1016
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