NSR Query Results
Output year order : Descending NSR database version of May 2, 2024. Search: Author = V.S.Bhasin Found 20 matches. 2007BH05 Nucl.Phys. A790, 257c (2007) Efimov effect in 2n-core halo nuclei and appearance of resonant states in n-19C scattering NUCLEAR REACTIONS 19C(n, n), E(cm)=0.8-3 keV; calculated σ; deduced resonance parameters. Efimov states.
doi: 10.1016/j.nuclphysa.2007.03.041
2006MA48 Phys.Rev.Lett. 97, 062503 (2006) I.Mazumdar, A.R.P.Rau, V.S.Bhasin Efimov States and their Fano Resonances in a Neutron-Rich Nucleus NUCLEAR REACTIONS 19C(n, n), E ≈ 1-3.5 keV; calculated σ vs neutron binding energy, Fano resonance features. NUCLEAR STRUCTURE 19,20C; calculated excited states energies, Efimov states.
doi: 10.1103/PhysRevLett.97.062503
2006SI21 Pramana 66, 377 (2006) A.K.Sisodiya, V.S.Bhasin, R.S.Kaushal On diquark clustering in quark-gluon plasma
doi: 10.1007/BF02704391
2006SI24 J.Phys.(London) G32, 1193 (2006) A.K.Sisodiya, R.S.Kaushal, D.Parashar, V.S.Bhasin Diquark interactions in quark-gluon plasma and their role in diquark stars
doi: 10.1088/0954-3899/32/8/009
2004AR12 Phys.Rev. C 69, 061301 (2004) V.Arora, I.Mazumdar, V.S.Bhasin Movement of Efimov states in 20C causing resonance in n-19C scattering near scattering threshold NUCLEAR STRUCTURE 20C; calculated three-body and two-body ground and excited states energies. Efimov states. NUCLEAR REACTIONS 19C(n, n), E(cm)=0.8-3 keV; calculated σ; deduced resonance parameters.
doi: 10.1103/PhysRevC.69.061301
2004KU27 Pramana 63, 509 (2004) Three-body analysis of 11Li and its β-decay to deuteron channel and to halo analog state 11Be (18.3 MeV) NUCLEAR STRUCTURE 11Li; calculated ground and excited states energies, radii, halo structure, β-decay observables for transition to analog state. 11Be calculated wave functions, excited state configuration. Three-body model.
doi: 10.1007/BF02704480
2002KU10 Phys.Rev. C65, 034007 (2002) Excited States of 11Li in a Three Body Model NUCLEAR STRUCTURE 11Li; calculated ground and excited states energies. Three body model.
doi: 10.1103/PhysRevC.65.034007
2002SA07 Phys.Rev. C65, 034012 (2002) A.B.Santra, B.K.Jain, V.S.Bhasin Production of d* Dibaryon in Proton-Deuteron Collisions NUCLEAR REACTIONS 2H(p, p'), E=0-1 GeV; calculated d* dibaryon production σ, angular distribution.
doi: 10.1103/PhysRevC.65.034012
2000MA28 Phys.Rev. C61, 051303 (2000) I.Mazumdar, V.Arora, V.S.Bhasin Three-Body Analysis of the Occurrence of Efimov States in 2n Halo Nuclei Such as 19B, 22C, and 20C NUCLEAR STRUCTURE 19B, 20,22C; calculated three-body ground and excited states energies; deduced role of Efimov effect.
doi: 10.1103/PhysRevC.61.051303
1999AW02 Phys.Rev. C60, 014307 (1999) Charge Symmetry Breaking Effects in Neutron-Proton Scattering using the Quark Model NUCLEAR REACTIONS 1H(polarized n, n), E=319, 418, 493 MeV; calculated σ(θ), asymmetry; deduced charge symmetry breaking mechanism. Quark model.
doi: 10.1103/PhysRevC.60.014307
1999BH06 Pramana 53, 567 (1999) A Three Body Approach to Study the Structural Properties of 2-n Halo Nuclei and the Search for Efimov States NUCLEAR STRUCTURE 11Li; calculated binding energy, related properties. Three-body approach to halo nuclei.
doi: 10.1007/s12043-999-0033-8
1997MA32 Phys.Rev. C56, R5 (1997) Efimov Effect in the Nuclear Halo 14Be Nucleus NUCLEAR STRUCTURE 14Be; calculated levels, binding energies, three-body energy as a function of two-body scattering length. Three-body calculations, Efimov effect.
doi: 10.1103/PhysRevC.56.R5
1996AW01 Phys.Rev. C53, 50 (1996); Erratum Phys.Rev. C56, 2891 (1997) Charge Symmetry Breaking Effects in Nucleon-Nucleon Scattering Derived from the Quark Model
doi: 10.1103/PhysRevC.53.50
1994DA14 Phys.Rev. C50, R550 (1994) S.Dasgupta, I.Mazumdar, V.S.Bhasin Three-Body Model for 11Li with Separable Potentials NUCLEAR STRUCTURE 11Li; calculated spectator, correlation functions. Three-body model.
doi: 10.1103/PhysRevC.50.R550
1989BA20 Pramana 32, 13 (1989) Nucleon-Nucleon Interaction with Tensor Forces in the Quark Compound Bag Model NUCLEAR STRUCTURE 2H; calculated μ, radius, quadrupole moment, D-state probability, electromagnetic form factors. Quark compound bag model.
doi: 10.1007/BF02845936
1985BH04 Phys.Rev. C32, 1187 (1985) Nucleon-Nucleon Interaction in the Quark Compound Bag Model NUCLEAR REACTIONS 1n(p, p), E ≈ 10-420 MeV; calculated 1S0 phase shift vs E. Quark compound bag model. NUCLEAR STRUCTURE 2H; calculated electromagnetic form factor. Quark compound bag model.
doi: 10.1103/PhysRevC.32.1187
1980AN11 Phys.Rev. C21, 2010 (1980) J.D.Anand, V.S.Bhasin, V.K.Gupta Photoproduction of Pions from Deuterons at Medium Energies NUCLEAR REACTIONS 2H(γ, pπ-), E=210-700 MeV; calculated production σ, σ(θ). Impulse approximation, different deuteron wave functions.
doi: 10.1103/PhysRevC.21.2010
1980GU15 Phys.Rev. C22, 721 (1980) V.K.Gupta, J.D.Anand, V.S.Bhasin Effect of Neutron-Neutron Final State Interaction in Pion Photoproduction by Deuterons Near Threshold Energies NUCLEAR REACTIONS 2H(γ, π+), E=20 MeV above threshold; calculated production σ; deduced role of neutron-neutron final state interaction. Impulse approximation, two-body center of mass correction.
doi: 10.1103/PhysRevC.22.721
1977BH04 Phys.Lett. 69B, 297 (1977) Pion Production on 3He by Protons in the Energy Range 300 to 400 MeV NUCLEAR REACTIONS 3He(p, π+), E=300-400 MeV; calculated σ.
doi: 10.1016/0370-2693(77)90550-0
1973BH04 Phys.Lett. 46B, 309 (1973) Pion Production in the Reaction pd → tπ NUCLEAR REACTIONS 2H(p, πt), E=340-670 MeV; calculated σ(E;θ).
doi: 10.1016/0370-2693(73)90126-3
Back to query form |