NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = D.N.Basu Found 60 matches. 2023SI13 Pramana 97, 85 (2023) V.Singh, J.Lahiri, M.Kanti Dey, D.N.Basu Radiative neutron capture reaction rates for nucleosynthesis: The creation of the first r-process peak
doi: 10.1007/s12043-023-02574-5
2021SI17 Acta Phys.Pol. B52, 453 (2021) New Thermonuclear Reaction Rate Equations for Radiative Neutron Capture NUCLEAR REACTIONS 6Li, 10B, 12C, 14N(n, γ), E=thermal-0.86 MeV; calculated σ, reaction rates using TALYS nuclear model code.
doi: 10.5506/aphyspolb.52.453
2019SI16 Nucl.Phys. A986, 98 (2019) V.Singh, D.Atta, M.A.Khan, D.N.Basu Astrophysical S-factor for deep sub-barrier fusion reactions of light nuclei NUCLEAR REACTIONS 2,3H(p, x), E=3-1000 keV;3H, 3He(d, x), E=30-1000 keV;6,7Li(p, x), E=20-1000 keV; calculated fusion σ using selective resonant tunneling model; compared with published data; deduced fusion astrophysical S-factor.
doi: 10.1016/j.nuclphysa.2019.03.010
2019SI20 Nucl.Phys. A987, 260 (2019) Theoretical exploration of S-factors for nuclear reactions of astrophysical importance NUCLEAR REACTIONS C, O, Ne, Mg, Si(C, x), O, Ne, Mg(O, x), Ne, Mg(Ne, x), Mg(Mg, x), E(cm)=2-30 MeV[used all possible combinations of neutron-rich isotopes of given elements]; calculated S-factor using newly developed robust analytical model based on reaction theory for non-resonant fusion σ near Coulomb barrier, based on tunneling through barrier; compared to data.
doi: 10.1016/j.nuclphysa.2019.05.005
2018MU08 Phys.Rev. C 97, 065804 (2018) S.Mukhopadhyay, J.Lahiri, D.Atta, K.Imam, D.N.Basu Gravitational waves from isolated neutron stars: Mass dependence of r-mode instability
doi: 10.1103/PhysRevC.97.065804
2017MA43 Eur.Phys.J. A 53, 151 (2017) K.Madhuri, D.N.Basu, T.R.Routray, S.P.Pattnaik Crustal moment of inertia of glitching pulsars with the KDE0v1 Skyrme interaction
doi: 10.1140/epja/i2017-12338-x
2016KH11 Phys.Rev. C 94, 054605 (2016); Erratum Phys.Rev. C 97, 019903 (2018) F.A.Khan, D.Bhowmick, D.N.Basu, M.Farooq, A.Chakrabarti Comparison of yields of neutron-rich nuclei in proton- and photon-induced 238U fission NUCLEAR REACTIONS 238U(p, F), E=12, 35, 13-63 MeV; calculated mass-yield distributions, variation of symmetric and asymmetric Gaussian parameters with excitation energies, total fission σ(E). 238U(p, F), E=12 MeV; 238U(γ, F), E=13.5 MeV; calculated ratio of cross sections, contour plots for σ(Z, N), plot of atomic number Z vs neutron number N for exotic nuclei (Z=25-60, N=50-105) of fragments, σ for production of 80Zn, 96Kr, 106Zr, 133Sn, 143Xe, 154Ce and for r-process nuclei 80Ge, 86Se, 96Sr, 101Zr, 117Pd, 122Cd, 133Te, 138Xe, 148Ce in the two fission processes. Two-mode fission mechanism with three-Gaussian function. Comparison with experimental data, and calculations using TALYS and PACE4 codes.
doi: 10.1103/PhysRevC.94.054605
2016RO24 J.Phys.(London) G43, 105101 (2016) T.R.Routray, X.Vinas, D.N.Basu, S.P.Pattnaik, M.Centelles, L.B.Robledo, B.Behera Exact versus Taylor-expanded energy density in the study of the neutron star crust-core transition
doi: 10.1088/0954-3899/43/10/105001
2015BH07 Phys.Rev. C 91, 044611 (2015) D.Bhowmick, D.Atta, D.N.Basu, A.Chakrabarti Yields of neutron-rich nuclei by actinide photofission in the giant dipole resonance region NUCLEAR REACTIONS 238U(γ, F), (γ, X), E<29.1 MeV; analyzed photoabsorption and photofission σ(E), mass and charge cross sections for the production of A=80-161, Z=32-63 neutron-rich nuclei in photofission in GDR region; analyzed behavior of symmetric and asymmetric modes of photon-induced fission as function of the average excitation energy of the fissioning nucleus. Relevance to r-process in nucleosynthesis. 232Th, 233,234,235,236,238U, 237Np, 239Pu(γ, F), (γ, X); analyzed experimental data in the GDR region; deduced peak cross section, resonance energy, and full width at half maximum.
doi: 10.1103/PhysRevC.91.044611
2014AT02 Phys.Rev. C 90, 035802 (2014) Stability of β-equilibrated dense matter and core-crust transition in neutron stars
doi: 10.1103/PhysRevC.90.035802
2014AT04 Phys.Rev. C 90, 064622 (2014) Fusion cross sections for reactions involving medium and heavy nucleus-nucleus systems NUCLEAR REACTIONS 144,148,154Sm(16O, X), 144Sm(17O, X), 90,96Zr, 110Pd(32S, X), (36S, X), 90,96Zr, 124Sn(40Ca, X), (48Ca, X), E not given; analyzed mean barrier height, width of barrier height distribution, effective radius from measured fusion excitation functions. 244Pu, 243Am, 245,248Cm, 249Bk, 249Cf(48Ca, X), E=250 MeV; calculated mean barrier height, width of barrier height distribution, effective radius, and capture σ. 144Sm(16O, X), E(cm)=55-90 MeV; 90,96Zr(36S, X), E(cm)=70-90 MeV; 124Sn(40Ca, X), E(cm)=107-135 MeV; calculated capture σ(E) using diffused-barrier formula assuming the Gaussian shape of the barrier-height distributions and compared with experimental values. 244Pu, 243Am, 245,248Cm, 249Bk, 249Cf(48Ca, X), E=180-250 MeV; calculated capture σ(E). Relevance to production cross sections of superheavy nuclei.
doi: 10.1103/PhysRevC.90.064622
2014SE05 Phys.Rev. C 89, 028801 (2014) Higher-order symmetry energy of nuclear matter and the inner edge of neutron star crusts
doi: 10.1103/PhysRevC.89.028801
2012MI24 Rom.J.Phys. 57, 1317 (2012) Nuclear Reaction Rates and the Primordial Nucleosynthesis NUCLEAR REACTIONS 2H(p, γ), (d, n), (d, p), (α, γ), 3H(d, n), (α, γ), 3He(n, p), (d, p), (3He, 2p), (α, γ), 6Li(p, γ), (p, α), 7Li(p, α), (α, γ), 7Be(n, p), (p, γ), (α, γ), 9Be(p, γ), (p, α), (α, n), 10B(p, γ), (p, α), 11B(p, γ), (p, 2α), 12C(p, γ), (α, γ), 13C(p, γ), (α, n), 13,14N(p, γ), 15N(p, γ), (p, α), E<1 MeV; analyzed available data; calculated reaction rates, isotope abundances. Comparison with available data.
2012RO17 Eur.Phys.J. A 48, 77 (2012) T.R.Routray, A.Mishra, S.K.Tripathy, B.Behera, D.N.Basu Proton radioactivity half-lives with Skyrme interactions RADIOACTIVITY 105Sb, 109I, 112,113Cs, 135Tb, 145,147Tm, 150,151Lu, 155,156,157Ta, 159,160,161Re, 164,165,166,167Ir, 171Au, 177Tl, 185Bi(p); calculated T1/2 using energy density formalism with different Skyrme interactions. Compared to the data.
doi: 10.1140/epja/i2012-12077-6
2011MU04 Ann.Nucl.Energy 38, 1452 (2011) T.Mukhopadhyay, J.Lahiri, D.N.Basu Theoretical estimates of cross sections for neutron-nucleus collisions NUCLEAR REACTIONS 238U, 232Th, 209Bi, 208Pb, 197Au, 182,184,186W, 181Ta, 93Nb, 90Zr, 59Co, 55Mn, 40Ca, 31P, 239Pu(n, X), (n, n), E<600 MeV; calculated σ. Analytical model, comparison with experimental data.
doi: 10.1016/j.anucene.2011.04.005
2011MU11 Phys.Rev. C 83, 067603 (2011) T.Mukhopadhyay, J.Lahiri, D.N.Basu Angular distributions of neutron-nucleus collisions NUCLEAR REACTIONS 238U, 184W, 90Zr, 40Ca(n, X), E=5-600 MeV; calculated total cross sections. 238U(n, n'), E(cm)=15 MeV; 90Zr(n, n'), E(cm)=24 MeV; 40Ca(n, n'), E(cm)=65 MeV; calculated σ(θ). Optical model and nuclear reaction theory approach. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.067603
2011RO36 Eur.Phys.J. A 47, 92 (2011) T.R.Routray, S.K.Tripathy, B.B.Dash, B.Behera, D.N.Basu Proton radioactivity with a Yukawa effective interaction RADIOACTIVITY 105Sb, 109I, 112,113Cs, 145,147Tm, 150,151Lu, 155,156,157Ta, 160,161Re, 164,165,166,167Ir, 171Au, 177Tl, 185Bi(p); calculated T1/2 using finite-range effective NN interaction of single Yukawa term.
doi: 10.1140/epja/i2011-11092-5
2010CH20 Phys.Rev. C 81, 062801 (2010) P.R.Chowdhury, A.Bhattacharyya, D.N.Basu Isospin asymmetric nuclear matter and properties of axisymmetric neutron stars
doi: 10.1103/PhysRevC.81.062801
2010MU08 Phys.Rev. C 82, 044613 (2010); Erratum Phys.Rev. C 83, 039902 (2011) T.Mukhopadhyay, J.Lahiri, D.N.Basu Cross sections of neutron-induced reactions NUCLEAR REACTIONS 181Ta, 182,184,186W, 197Au, 208Pb, 209Bi, 232Th, 238U, 239Pu(n, X), E<600 MeV; calculated neutron-nucleus total and reaction σ using nuclear Ramsauer model. Comparison with experimental data and with optical model calculations of Koning-Delaroche global OMP, and Morillon-Romain global OMP.
doi: 10.1103/PhysRevC.82.044613
2010MU10 Eur.Phys.J. A 45, 121 (2010) Photonuclear reactions of actinides in the giant dipole resonance region NUCLEAR REACTIONS 232Th, 238U, 237Np(γ, F), (γ, X), E=8-20 MeV; calculated fission and absorption σ. 63Cu, 64Zn(γ, X), E=15, 20 MeV; calculated σ vs residue mass. GDR and quasi-deuteron reaction contribution discussed.
doi: 10.1140/epja/i2010-10993-y
2009BA53 Phys.Rev. C 80, 057304 (2009) D.N.Basu, P.Roy Chowdhury, C.Samanta Isobaric incompressibility of isospin asymmetric nuclear matter
doi: 10.1103/PhysRevC.80.057304
2009MU01 Phys.Rev. C 79, 017602 (2009) γ induced multiparticle emissions of medium mass nuclei at intermediate energies NUCLEAR REACTIONS 51V, 64Zn, 118Sn, 140Ce, 154Sm, 174Yb, 181Ta, 197Au, 208Pb, 209Bi(γ, X), E=30-140 MeV; calculated σ, neutron multiplicities.
doi: 10.1103/PhysRevC.79.017602
2009RO15 Phys.Rev. C 80, 011305 (2009) P.Roy Chowdhury, D.N.Basu, C.Samanta Isospin dependent properties of asymmetric nuclear matter
doi: 10.1103/PhysRevC.80.011305
2009RO16 Nucl.Phys. A826, 223 (2009) T.R.Routray, J.Nayak, D.N.Basu Cluster radioactivity in very heavy nuclei: a new perspective RADIOACTIVITY 212,213,214Po, 215At(α); 221Fr, 221,222,223,224,226Ra, 225Ac(14C); 228Th(16O); 230U(22Ne); 230Th, 231Pa, 232,233,234U(24Ne); 233U(25Ne); 234U(26Ne); 234U, 236,238Pu(28Mg); 238Pu(30Mg), (32Si); 242Cm(34Si); calculated T1/2, cluster preformation probability, related features using a folding density dependent model.
doi: 10.1016/j.nuclphysa.2009.06.018
2008BA32 Nucl.Phys. A811, 140 (2008) D.N.Basu, P.Roy Chowdhury, C.Samanta Nuclear equation of state at high baryonic density and compact star constraints RADIOACTIVITY 105Sb, 145,147Tm, 150,151Lu, 155,156,157Ta, 160,161Re, 164,165,166,167Ir, 171Au, 177Tl, 185Bi(p); calculated T1/2 using a mean-field approach with the DDM3Y folding potential. Comparison with data.
doi: 10.1016/j.nuclphysa.2008.07.009
2008RO10 Phys.Rev. C 77, 044603 (2008) P.Roy Chowdhury, C.Samanta, D.N.Basu Search for long lived heaviest nuclei beyond the valley of stability NUCLEAR STRUCTURE Z=102-120, N=120-200; calculated α-, β- and SF-decay half-lives. 266Sg, 267Bh, 266,267,269,270Hs, 268Mt, 267,268,269,270,271,273Ds, 272Rg, 277,283Cn; calculated α-decay half-lives, comparison with experimental data. Quantum tunneling model with DDM3Y interaction using three different mass formulae.
doi: 10.1103/PhysRevC.77.044603
2008RO25 At.Data Nucl.Data Tables 94, 781 (2008) P.Roy Chowdhury, C.Samanta, D.N.Basu Nuclear half-lives for α-radioactivity of elements with 100 ≤ Z ≤ 130 NUCLEAR STRUCTURE Z=100-130; calculated α-decay half-lives and Q-values within a WKB framework using microscopic nuclear potentials.
doi: 10.1016/j.adt.2008.01.003
2008SA17 J.Phys.(London) G35, 065101 (2008) C.Samanta, P.Roy Chowdhury, D.N.Basu Lambda hyperonic effect on the normal drip lines NUCLEAR STRUCTURE Li, Be, B, C, N, O, F, Ne, Na, Mg, Al, Si, P, S, Cl, Ar, K, Ca, Sc, Ti, V, Cr, Mn, Fe, Co, Ni, Cu, Zn, Ga, Ge, As, Se, Br, Kr, Rb, Sr, Y, Zr, Nd, Mo, Tc; calculated proton and neutron separation energies for normal and lambda hypernuclei using a generalized mass formula.
doi: 10.1088/0954-3899/35/6/065101
2007BA22 Acta Phys.Pol. B38, 169 (2007) High density behaviour of nuclear symmetry energy
2007CH36 Phys.Rev. C 75, 047306 (2007) P.R.Chowdhury, D.N.Basu, C.Samanta α decay chains from element 113 RADIOACTIVITY 278,283,284Nh, 274,279,280Rg, 270,275,276Mt, 266,272Bh(α); calculated T1/2. Density-dependent effective nucleon-nucleon interaction.
doi: 10.1103/PhysRevC.75.047306
2007MU12 Nucl.Phys. A789, 201 (2007) Nuclear symmetry energy from effective interaction and masses of isospin asymmetric nuclei NUCLEAR STRUCTURE A=1-300; calculated nuclear symmetry and binding energies using the DDM3Y interaction and by fitting experimental and extrapolated masses.
doi: 10.1016/j.nuclphysa.2007.04.006
2007MU13 Acta Phys.Pol. B38, 3225 (2007) Isospin asymmetry in nuclei and nuclear symmetry energy NUCLEAR STRUCTURE A >15; calculated coefficients of the liquid droplet model mass formula extracted from measured atomic mass excesses.
2007MU18 Phys.Rev. C 76, 064610 (2007) Photonuclear reactions of actinide and pre-actinide nuclei at intermediate energies NUCLEAR REACTIONS 208Pb, 209Bi, 232Th, 233,235,238U, 237Np(γ, F), E=20-140 MeV; calculated cross sections using Monte Carlo model, compared with experimental data.
doi: 10.1103/PhysRevC.76.064610
2007PA47 J.Phys.(London) G45, 055202 (2007);Addendum: J.Phys.(London) G45, 119401 (2007) S.P.Pattnaik, T.R.Routray, X.Vinas, D.N.Basu, M.Centelles, K.Madhuri, B.Behera Influence of the nuclear matter equation of state on the r-mode instability using the finite-range simple effective interaction
doi: 10.1088/1361-6471/aab7c5
2007SA49 Nucl.Phys. A789, 142 (2007) C.Samanta, P.R.Chowdhury, D.N.Basu Predictions of alpha decay half lives of heavy and superheavy elements RADIOACTIVITY 271Sg, 266,271Bh, 275Hs, 270,275,276Mt, 279Ds, 274,279,280Rg, 283,285Cn, 278,283,284Nh, 286,287,288,289Fl, 287,288Mc, 290,291,292,293Lv, 294Og(α); calculated T1/2 by calculating QM tunneling probabilities in a WKB framework. Compared results to available data.
doi: 10.1016/j.nuclphysa.2007.04.001
2007SA58 J.Phys.Soc.Jpn. 76, 124201 (2007) C.Samanta, D.N.Basu, P.Roy Chowdhury Quantum Tunneling in 277112 and Its α-Decay Chain RADIOACTIVITY 257No, 261Rf, 265Sg, 269Hs, 273Ds, 277Cn(α); calculated T1/2 in WKB framework using DDM3Y interaction, Q-values from the mass formula of Muntian-Hofmann-Patyk-Sobiczeski. Comparisons with experimental data.
doi: 10.1143/JPSJ.76.124201
2006BA68 Acta Phys.Pol. B37, 2869 (2006) D.N.Basu, P.R.Chowdhury, C.Samanta Equation of state for isospin asymmetric nuclear matter using Lane potential
2006CH04 Phys.Rev. C 73, 014612 (2006) P.R.Chowdhury, C.Samanta, D.N.Basu α decay half-lives of new superheavy elements RADIOACTIVITY 274,276,278,280,282,284,286,288,290,292Rf, 271,278,280,282,284,286,288,290,292,294Sg, 275,282,284,286,288,290,292,294,296Hs, 279,286,288,290,292,294,296,298Ds, 283,285,288,290,292,294,296,298,300Cn, 286,287,288,289,290,292,294,296,298,300,302Fl, 284,286,288,290,291,292,293,294,296,298,300,302,304Lv, 288,290,292,294,296,298,300,302,304Og, 292,294,296,298,300,302,304,306120(α); calculated Qα, T1/2. Double-folding model, comparison with data and previous calculations.
doi: 10.1103/PhysRevC.73.014612
2006CH41 Acta Phys.Pol. B37, 1833 (2006) Nuclear matter properties with the re-evaluated coefficients of Liquid drop model
2006CH63 Rom.J.Phys. 51, 853 (2006) Spin-parities and half lives of 257No and its α-decay daughter 253Fm RADIOACTIVITY 257No(α); analyzed T1/2, Qα. 257No, 253Fm levels deduced J, π.
2006SA05 J.Phys.(London) G32, 363 (2006) C.Samanta, P.R.Chowdhury, D.N.Basu Generalized mass formula for non-strange and hypernuclei with SU(6) symmetry breaking NUCLEAR STRUCTURE A=4-210; calculated hyperon binding energies. Generalized mass formula, spin-flavor SU(6) symmetry breaking.
doi: 10.1088/0954-3899/32/3/010
2005BA76 Int.J.Mod.Phys. E14, 739 (2005) Equation of state for nuclear matter based on density dependent effective interaction
doi: 10.1142/S0218301305003521
2005BA97 Phys.Rev. C 72, 051601 (2005) D.N.Basu, P.R.Chowdhury, C.Samanta Folding model analysis of proton radioactivity of spherical proton emitters RADIOACTIVITY 105Sb, 145,147Tm, 150,151Lu, 155,156,157Ta, 160,161Re, 164,165,166,167Ir, 171Au, 177Tl, 185Bi(p); calculated proton decay T1/2 for ground and isomeric states. Folding model, global proton optical potential, comparison with data.
doi: 10.1103/PhysRevC.72.051601
2005GU03 Nucl.Phys. A748, 402 (2005) Folding model analysis of proton scattering from mirror nuclei 18Ne and 18O NUCLEAR REACTIONS 18O(p, p'), E=24.5 MeV; 1H(18Ne, p), E=30 MeV/nucleon; calculated σ(E, θ). Folding model approach, comparison of effective interactions.
doi: 10.1016/j.nuclphysa.2004.11.010
2004BA46 J.Phys.(London) G30, B7 (2004) Nuclear incompressibility using the density-dependent M3Y effective interaction
doi: 10.1088/0954-3899/30/6/B01
2004BA86 J.Phys.(London) G30, B35 (2004) Lifetimes of the α decay chains of superheavy element Z = 115 RADIOACTIVITY 287,288Mc, 283,284Nh, 279,280Rg, 275,276Mt, 271,272Bh(α); calculated T1/2. microscopic approach, comparison with data.
doi: 10.1088/0954-3899/30/10/B02
2004BA87 Int.J.Mod.Phys. E13, 747 (2004) Neutron and proton drip lines using the modified Bethe-Weizsacker mass formula NUCLEAR STRUCTURE Z=1-118; calculated neutron and proton separation energies; deduced drip lines. Modified Bethe-Weizsacker formula.
doi: 10.1142/S0218301304002491
2003BA54 Phys.Lett. B 566, 90 (2003) Role of effective interaction in nuclear disintegration processes NUCLEAR STRUCTURE Z=87-106; calculated α-decay T1/2. Z=87-92; calculated cluster-decay T1/2. Superasymmetric fission model, comparison with data.
doi: 10.1016/S0370-2693(03)00801-3
2003BA64 J.Phys.(London) G29, 2079 (2003) Folding model analysis of alpha radioactivity RADIOACTIVITY 222,224,226Ra, 226,228,230,232Th, 230,232,234,236U, 236,238,240Pu, 242Cm(α); calculated α-decay T1/2. Double folding procedure, comparison with data.
doi: 10.1088/0954-3899/29/9/303
2002BA80 Phys.Rev. C66, 027601 (2002) Spontaneous heavy cluster emission rates using microscopic potentials RADIOACTIVITY 221Fr, 221,222,223,224,226Ra, 225Ac(14C); 228Th(20O); 230Th, 231Pa, 232,233,234,236U(24Ne); 233,235U(25Ne); 234,235,236U(26Ne); 232,234,235,236U, 236,238Pu(28Mg); 234,235,236U, 237Np, 238Pu(30Mg); 238Pu(32Si); 241Am, 242Cm(34Si); 231Pa(23F); calculated cluster decay T1/2. Microscopic superasymmetric fission model, comparison with data.
doi: 10.1103/PhysRevC.66.027601
2002BH05 Phys.Rev. C66, 047601 (2002) C.Bhattacharya, K.Mullick, S.Bhattacharya, K.Krishan, T.Bhattacharjee, P.Das, S.R.Banerjee, D.N.Basu, A.Ray, S.K.Basu, M.B.Chatterjee Dissipative collisions in 16O +27Al at Elab = 116 MeV NUCLEAR REACTIONS 27Al(16O, X), E=116 MeV; measured fragments isotopic yields, energy and angular distributions; deduced reaction mechanism features.
doi: 10.1103/PhysRevC.66.047601
1998BH14 Mod.Phys.Lett. A 13, 2665 (1998) D.Bhowmick, A.Chakrabarti, D.N.Basu, P.Ghosh, R.Goswami Empirical Formalism for Projectile Fragmentation and Production of New Neutron-Rich Nuclei with RIBS NUCLEAR REACTIONS 181Ta(48Ca, X), E=70 MeV/nucleon; 181Ta(50Ti, X), E=80 MeV/nucleon; 58Ni(78Kr, X), E=75 MeV/nucleon; 27Al(86Kr, X), E=70 MeV/nucleon; calculated fragments isotopic production σ. Empirical formalism, comparisons with data, previous calculations.
doi: 10.1142/S0217732398002837
1997UM02 Nucl.Phys. A615, 516 (1997) V.S.Uma Maheswari, D.N.Basu, J.N.De, S.K.Samaddar Spin Polarised Nuclear Matter and Its Application to Neutron Stars
doi: 10.1016/S0375-9474(97)00002-X
1996SA10 Phys.Rev. C53, 2287 (1996) C.Samanta, S.Mukherjee, R.Kanungo, D.N.Basu Deuteron Breakup at Extreme Forward Angles: Failure of a pure Coulomb dissociation description NUCLEAR REACTIONS 12C, 40Ca, 208Pb(d, np), E=56 MeV; analyzed σ(θp, θn, Ep); deduced reaction mechanism related features.
doi: 10.1103/PhysRevC.53.2287
1995SA39 Phys.Lett. 352B, 197 (1995) C.Samanta, R.Kanungo, S.Mukherjee, D.N.Basu Coulomb-Nuclear Interference in 56 MeV Deuteron Breakup at Extreme Forward Angle NUCLEAR REACTIONS 12C(d, np), E=56 MeV; analyzed σ(θ), σ(θp, θn, Ep); deduced Coulomb-nuclear interference role, optical potential features. Prior form DWBA.
doi: 10.1016/0370-2693(95)00515-M
1990SR02 Z.Phys. A335, 417 (1990) D.K.Srivastava, D.N.Basu, H.Rebel, H.J.Gils Orbital Dispersion and Wavefunction Mapping in Inclusive Break-Up Experiments NUCLEAR REACTIONS 12C, 208Pb(6Li, αX), E=26 MeV/nucleon; analyzed σ(θα, Eα); deduced projectile internal momentum distribution.
1988SR01 Phys.Lett. 206B, 391 (1988) D.K.Srivastava, D.N.Basu, H.Rebel Direct and Sequential Coulomb Break-Up of 7Li NUCLEAR REACTIONS 120Sn(7Li, 7Li'), E=70 MeV; calculated pure Coulomb breakup σ(θ). 208Pb(7Be, 3Heα), (7Be, tα), E=40-300 MeV; calculated breakup σ(E).
doi: 10.1016/0370-2693(88)91597-3
1988SR02 Nucl.Phys. A485, 221 (1988) D.K.Srivastava, D.N.Basu, H.Rebel The Dynamic Polarization Potential from Coulomb Dissociation of Deuterons and 3He NUCLEAR REACTIONS, ICPND 208Pb(d, np), (3He, pd), E ≈ 10-250 MeV; calculated Coulomb dissociation σ(E). Dynamic polarization. NUCLEAR STRUCTURE 3He, 2H; calculated B(E2) per unit energy following Coulomb dissociation. Dynamic polarization.
doi: 10.1016/0375-9474(88)90099-1
1988SR03 Phys.Rev. C38, 2148 (1988) D.K.Srivastava, D.N.Basu, H.Rebel Features of Direct and Sequential Coulomb Breakup of 6Li Ions NUCLEAR REACTIONS 208Pb(6Li, dα), E=30-156 MeV; calculated Coulomb dissociation σ(E); deduced breakup mechanism, relation to astrophysical S-factor. NUCLEAR STRUCTURE 6Li; calculated breakup transition B(E2).
doi: 10.1103/PhysRevC.38.2148
1985CH19 Nucl.Phys. A439, 415 (1985) A.K.Chaudhuri, D.N.Basu, B.Sinha An α-Nucleus Optical Potential using a Realistic Effective Interaction NUCLEAR REACTIONS 58Ni(α, α), E=172.5 MeV; 40Ca(α, α), E=141.7 MeV; 52Cr, 50Ti(α, α), E=104 MeV; 208Pb(α, α), E=140 MeV; calculated σ(θ), α-nucleus potential. Realistic effective interactions.
doi: 10.1016/0375-9474(85)90419-1
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