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NSR database version of April 11, 2024.

Search: Author = N.Deshmukh

Found 23 matches.

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2022BH07      Phys.Rev. C 106, 064612 (2022)

S.Bhattacharjee, P.Biswas, A.Gupta, M.K.Pradhan, N.Deshmukh, P.Basu, V.V.Parkar, S.Santra, K.Ramachandran, A.Chatterjee, S.Roy, A.Mukherjee

Systematic investigation of channel-coupling effects on elastic, inelastic, and neutron-transfer channels in 6Li+159Tb

NUCLEAR REACTIONS 159Tb(6Li, 6Li), (6Li, 7Li), E= 25, 27, 30, 35 MeV; measured reaction product, angular distributions; deduced elastic and quasielastic scattering σ(θ, E), 1n pickup reaction σ(θ, E), optical model potential parameters, spectroscopic factors for 158Tb+n and 6Li+n conigurations. Comparison to finite-range coupled-channel Born approximation (CCBA) calculations.Four Silicon surface barrier telescope detectors at 14UD BARC-TIFR Pelletron Accelerator (Mumbai, India).

doi: 10.1103/PhysRevC.106.064612
Citations: PlumX Metrics

2022GU19      Phys.Lett. B 834, 137452 (2022)

Y.K.Gupta, G.K.Prajapati, B.V.John, B.N.Joshi, L.S.Danu, S.Dubey, S.Mukhopadhyay, N.Kumar, K.Mahata, K.Ramachandran, A.Jhingan, M.Kumar, N.Deshmukh, A.S.Pradeep, B.K.Nayak, D.C.Biswas

New signature of non-equilibrium fission from pre-scission α-particle emission

NUCLEAR REACTIONS 232Th(16O, F)4H, E=96 MeV; measured reaction products, Eα, Iα, Ep, Ip, Eγ, Iγ; deduced pre-scission α-particle multiplicity spectra, fission time. Comparison with statistical model calculations. BARC-TIFR 14-MV Pelletron accelerator facility at Mumbai.

doi: 10.1016/j.physletb.2022.137452
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2021BH14      Phys.Rev. C 104, 054607 (2021)

S.Bhattacharjee, A.Mukherjee, A.Gupta, R.Santra, D.Chattopadhyay, N.Deshmukh, S.Dhuri, S.Gupta, V.V.Parkar, S.K.Pandit, K.Ramachandran, K.Mahata, A.Shrivastava, R.Pachuau, S.Rathi

Fusion of 16O + 165Ho at deep sub-barrier energies

NUCLEAR REACTIONS 165Ho(16O, 3nα)174Ta, (16O, 5n)176Re, (16O, 4n)177Re, (16O, 3n)178Re, E=62-85 MeV; measured evaporation residues (ERs) by off-line γ-ray spectroscopy, Eγ, Iγ from decays of evaporation residues, σ(E) at 14UD BARC-TIFR Pelletron-LINAC facility; deduced fusion σ(E) and compared with σ(E) results of earlier experiments, astrophysical S factor. Comparison with coupled channel (CC) calculations using Woods-Saxon potential using code PACE4, fusion hindrance and compared with prediction from adiabatic model; analyzed previous experimental results for 19F+165Ho, 7Li+165Ho, 12C+198Pt, 16O+208Pb, 28Si+64Ni, 16O+208Pb, 32S+89Y, 36S+64Ni, 40Ca+40Ca, 40Ca+48Ca, and 48Ca+48Ca systems. 178Re; measured T1/2 of the decay of the g.s.

doi: 10.1103/PhysRevC.104.054607
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6413.

2021FE06      Phys.Rev. C 103, 054604 (2021)

J.L.Ferreira, D.Carbone, M.Cavallaro, N.N.Deshmukh, C.Agodi, G.A.Brischetto, S.Calabrese, F.Cappuzzello, E.N.Cardozo, I.Ciraldo, M.Cutuli, M.Fisichella, A.Foti, L.La Fauci, O.Sgouros, V.Soukeras, A.Spatafora, D.Torresi, J.Lubian, for the NUMEN Collaboration

Analysis of two-proton transfer in the 40Ca(18O, 20Ne)38Ar reaction at 270 MeV incident energy

NUCLEAR REACTIONS 40Ca(18O, 20Ne)38Ar, E=270 MeV; measured 20Ne ejectiles, excitation energy spectrum, σ(θ) for ground and excited states of 20Ne and 38Ar using MAGNEX large acceptance spectrometer and a focal plane detector at the K800 Superconducting Cyclotron accelerator, INFN-LNS laboratory in Catania as part of the NUMEN Collaboration research program of transfer reactions; analyzed data using finite-range coupled reaction channel (CRC) and coupled-channel Born approximation (CCBA) methods with the FRESCO code; deduced spectroscopic amplitudes and differential cross sections for transitions to different states; calculated contributions from the direct and sequential transfer mechanisms.

NUCLEAR STRUCTURE 38Ar, 39K, 40Ca; calculated level energies, B(E2), B(E3) using shell-model, and compared with experimental data. 19F, 20,22Ne, 38Ar, 39K; calculated one-proton and two-proton spectroscopic amplitudes for the projectile overlaps between the initial and final states used in the CCBA and CRC calculations for the sequential two-proton transfer reaction.

doi: 10.1103/PhysRevC.103.054604
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD8035.

2020PA05      Phys.Rev. C 101, 024602 (2020)

A.Pakou, O.Sgouros, V.Soukeras, F.Cappuzzello, L.Acosta, C.Agodi, A.Boiano, S.Calabrese, D.Carbone, M.Cavallaro, N.N.Deshmukh, A.Foti, A.Hacisalihoglu, N.Keeley, M.La Commara, I.Martel, M.Mazzocco, A.Muoio, C.Parascandolo, D.Pierroutsakou, K.Rusek, A.M.Sanchez-Benitez, G.Santagati, G.Souliotis, A.Spatafora, E.Strano, D.Torresi, A.Trzcinska

9Be + p breakup at 5.67A MeV in a full kinematics approach

NUCLEAR REACTIONS 1H(9Be, X), E=51 MeV; measured ΔE-E spectra for the recoils, ααp-coin using EXPADES module at the MAGNEX facility of INFN-LNS-Catania; deduced α-α relative energy spectrum from analysis of triple coincidence events, energy spectrum of recoiling protons, rates of three breakup modes: α+α+n, 8Be+n and 5He+4He for the 9Be Borromean nucleus.

doi: 10.1103/PhysRevC.101.024602
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2019DE25      Europhys.Lett. 127, 12001 (2019)

N.Deshmukh, J.Lubian, S.Mukherjee

Total reaction cross-section and reduction methodology for various projectiles on medium-mass 58Ni target

NUCLEAR REACTIONS 58Ni(10B, 10B), E(cm)<30 MeV; measured reaction products; deduced σ using the optical model with double-folding-type potentials. Comparison with available data.

doi: 10.1209/0295-5075/127/12001
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2019GU26      Phys.Rev. C 100, 034603 (2019)

V.Guimaraes, E.N.Cardozo, V.B.Scarduelli, J.Lubian, J.J.Kolata, P.D.O'Malley, D.W.Bardayan, E.F.Aguilera, E.Martinez-Quiroz, D.Lizcano, A.Garcia-Flores, M.Febbraro, C.C.Lawrence, J.Riggins, R.O.Torres-Isea, P.N.de Faria, D.S.Monteiro, E.S.Rossi, N.N.Deshmukh

Strong coupling effect in the elastic scattering of the 10C + 58Ni system near barrier

NUCLEAR REACTIONS 58Ni(10C, 10C), (10C, 10C'), (10C, X)4He/7Li/7Be/10B/10C/12N, E=35.3 MeV, [secondary 10C beam from 3He(10B, 10C), E=54.0 MeV primary reaction at the Nuclear Science Laboratory of Notre Dame]; measured reaction products, particle identification spectrum, scattered 10C particles using three ΔE-E telescopes with silicon planar detectors, σ(θ); deduced differential σ; the results analyzed via coupled-channels, coupled-reaction-channels, and continuum-discretized coupled-channels (CDCC) calculations, with the consideration of 9B+p and 6Be+α channels as cluster configurations for the 10C projectile in CDCC approach. The 2+ inelastic transition in 10C in the projectile shown to be of crucial importance in describing the cross section data.

doi: 10.1103/PhysRevC.100.034603
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2409.

2019KE02      Phys.Rev. C 99, 014615 (2019)

N.Keeley, A.Pakou, V.Soukeras, F.Cappuzzello, L.Acosta, C.Agodi, A.Boiano, S.Calabrese, D.Carbone, M.Cavallaro, N.Deshmukh, A.Foti, A.Hacisalihoglu, M.La Commara, I.Martel, M.Mazzocco, A.Muoio, C.Parascandolo, D.Pierroutsakou, K.Rusek, A.M.Sanchez-Benitez, G.Santagati, O.Sgouros, G.Souliotis, A.Spatafora, E.Strano, D.Torresi, A.Trzcinska

Coherent coupled-reaction-channels analysis of existing and new p + 9Be data between 1.7 and 15 MeV/nucleon

NUCLEAR REACTIONS 1H(9Be, 9Be), E=15, 22, 51 MeV; measured scattered 9Be particles, σ(E, θ) using the large acceptance MAGNEX spectrometer at INFN-LNS-Catania. 9Be(p, p), (p, p'), (p, d), (polarized p, p), E=3, 68, 10, 15, MeV/nucleon; analyzed differential σ(θ, E), and vector analyzing powers Ay(θ); deduced renormalized differential σ(θ, E), and optical model parameters. Coupled-reaction-channels model using FRESCO code.

doi: 10.1103/PhysRevC.99.014615
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2402.

2018CA16      Eur.Phys.J. A 54, 72 (2018)

F.Cappuzzello, C.Agodi, M.Cavallaro, D.Carbone, S.Tudisco, D.Lo Presti, J.R.B.Oliveira, P.Finocchiaro, M.Colonna, D.Rifuggiato, L.Calabretta, D.Calvo, L.Pandola, L.Acosta, N.Auerbach, J.Bellone, R.Bijker, D.Bonanno, D.Bongiovanni, T.Borello-Lewin, I.Boztosun, O.Brunasso, S.Burrello, S.Calabrese, A.Calanna, E.R.Chavez-Lomeli, G.D'Agostino, P.N.De Faria, G.De Geronimo, F.Delaunay, N.Deshmukh, J.L.Ferreira, M.Fisichella, A.Foti, G.Gallo, H.Garcia-Tecocoatzi, V.Greco, A.Hacisalihoglu, F.Iazzi, R.Introzzi, G.Lanzalone, J.A.Lay, F.La Via, H.Lenske, R.Linares, G.Litrico, F.Longhitano, J.Lubian, N.H.Medina, D.R.Mendes, M.Moralles, A.Muoio, A.Pakou, H.Petrascu, F.Pinna, S.Reito, A.D.Russo, G.Russo, G.Santagati, E.Santopinto, R.B.B.Santos, O.Sgouros, M.A.G.da Silveira, S.O.Solakci, G.Souliotis, V.Soukeras, A.Spatafora, D.Torresi, R.Magana Vsevolodovna, A.Yildirim, V.A.B.Zagatto

The NUMEN project: NUclear Matrix Elements for Neutrinoless double beta decay

doi: 10.1140/epja/i2018-12509-3
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2018CA17      Acta Phys.Pol. B49, 275 (2018)

S.Calabrese, F.Cappuzzello, D.Carbone, M.Cavallaro, C.Agodi, L.Acosta, D.Bonanno, D.Bongiovanni, T.Borello-Lewin, I.Boztosun, D.Calvo, E.R.Chavez-Lomeli, N.Deshmukh, P.N.de Faria, P.Finocchiaro, M.Fisichella, A.Foti, G.Gallo, A.Hacisalihoglu, F.Iazzi, R.Introzzi, G.Lanzalone, R.Linares, F.Longhitano, D.Lo Presti, N.Medina, A.Muoio, J.R.B.Oliveira, A.Pakou, L.Pandola, F.Pinna, S.Reito, G.Russo, G.Santagati, O.Sgouros, S.O.Solakci, V.Soukeras, G.Souliotis, A.Spatafora, D.Torresi, S.Tudisco, A.Yildirim, V.A.B.Zagatto

First Measurement of the 116Cd(20Ne, 20O)116Sn Reaction at 15 A MeV

NUCLEAR REACTIONS 116Cd(20Ne, 20O)116Sn, E=15 MeV/nucleon; measured outgoing 20O ejectiles momentum by the MAGNEX spectrometer and detected by its Focal Plane Detector (FPD), other reaction products using K800 Superconducting cyclotron at INFN-LNS Catania coupled to carbon post-stripper; deduced identified 20O ejectiles. The 116Cd(20Ne, 20O)116Sn reaction has been measured for the first time; Double Charge-Exchange (DCE) measure with heavy ions successful, PID and ray-reconstruction procedures led to excellent signal-to-noise ratio.

doi: 10.5506/aphyspolb.49.275
Citations: PlumX Metrics

2018DE26      Eur.Phys.J. A 54, 101 (2018)

N.Deshmukh, J.Lubian

Total reaction cross section for the 11B + 58Ni system and application of a recent new reduction methodology

NUCLEAR REACTIONS 58Ni(11B, x), (11B, 11B), E(cm)=15.97-29.41 MeV; calculated σ(θ) using data from previous work of the authors using optical model with Sao Paulo potential; deduced potential parameters, possible transfer contribution; calculated 18 other reactions with available data with halo, unstable, stable, radioactive and tightly bound projectiles; deduced total reaction σ systematic trend vs E(cm)/V(Coulomb).

doi: 10.1140/epja/i2018-12538-x
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2018LE19      Phys.Rev. C 98, 064601 (2018)

E.Leistenschneider, A.Lepine-Szily, M.A.G.Alvarez, D.R.Mendes, R.Lichtenthaler, V.A.P.Aguiar, M.Assuncao, R.P.Condori, U.U.da Silva, P.N.de Faria, N.Deshmukh, J.G.Duarte, L.R.Gasques, V.Guimaraes, E.L.A.Macchione, M.C.Morais, V.Morcelle, K.C.C.Pires, V.B.Scarduelli, G.Scotton, J.M.B.Shorto, V.A.B.Zagatto

Spectroscopy of high-lying resonances in 9Be by the measurement of (p, p), (p, d), and (p, α) reactions with a radioactive 8Li beam

NUCLEAR REACTIONS 1H(8Li, p)8Li, (8Li, d)7Li, (8Li, α)5He, C, 197Au(8Li, 8Li), E=22.5, 16 MeV, [secondary 8Li beam produced in 9Be(7Li, 8Li), E=24.4 MeV]; measured reaction products, yields, Ep, Ip, Ed, Id, Eα, Iα, differential σ(θ) using ΔE-E silicon telescope at the RIBRAS facility of the University of Sao Paulo 8-UD tandem accelerator. 9Be; deduced levels, resonances, J, π, l-values, Γp, Γd, Γα, and reduced widths γ2 and the dimensionless reduced widths θ2α for the α and deuteron channels using R-matrix analysis. Comparison with previous experimental data.

doi: 10.1103/PhysRevC.98.064601
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0933. Data from this article have been entered in the XUNDL database. For more information, click here.

2017PA46      Chin.Phys.C 41, 104001 (2017)

D.Patel, S.Mukherjee, N.Deshmukh, J.Lubian, J.-S.Wang, T.Correa, B.K.Nayak, Y.-Y.Yang, W.i-H.Ma, D.C.Biswas, Y.K.Gupta, S.Santra, E.T.Mirgule, L.S.Danu, N.L.Singh, A.Saxena

Influence of breakup on elastic and α-production channels in the 6Li+ 116Sn reaction

NUCLEAR REACTIONS 116Sn(6Li, X)4H, E=22-40 MeV; measured reaction products, Eα, Iα; deduced σ(θ). Comparison with the predictions of continuum-discretized coupled channels (CDCC) calculations.

doi: 10.1088/1674-1137/41/10/104001
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2017SC24      Phys.Rev. C 96, 054610 (2017)

V.Scarduelli, E.Crema, V.Guimaraes, D.Abriola, A.Arazi, E.de Barbara, O.A.Capurro, M.A.Cardona, J.Gallardo, D.Hojman, G.V.Marti, A.J.Pacheco, D.Rodrigues, Y.Y.Yang, N.N.Deshmukh, B.Paes, J.Lubian, D.R.Mendes, Jr, V.Morcelle, D.S.Monteiro

Elastic and inelastic scattering for the 10B + 58Ni system at near-barrier energies

NUCLEAR REACTIONS 58Ni(10B, 10B), (10B, 10B'), E=19.0, 21.0, 23.0, 24.0, 25.0, 35.0 MeV; measured particle spectra, σ(θ, E) at the 20 UD tandem accelerator facility of TANDAR laboratory in Buenos Aires; analyzed data by large-scale coupled reaction channel calculation, considering several inelastic transitions of the projectile and the target together with one- and two-step transfer reactions.

doi: 10.1103/PhysRevC.96.054610
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0882.

2016LI17      Few-Body Systems 57, 157 (2016)

R.Lichtenthaler, M.A.G.Alvarez, A.Lepine-Szily, S.Appannababu, K.C.C.Pires, U.U.da Silva, V.Scarduelli, R.P.Condori, N.Deshmukh

RIBRAS: The Facility for Exotic Nuclei in Brazil

doi: 10.1007/s00601-015-1039-z
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2015DE36      Phys.Rev. C 92, 054615 (2015)

N.N.Deshmukh, V.Guimaraes, E.Crema, D.Abriola, A.Arazi, E.de Barbara, O.A.Capurro, M.A.Cardona, J.Gallardo, D.Hojman, G.V.Marti, A.J.Pacheco, D.Rodrigues, Y.Y.Yang, A.N.Deshmukh, D.R.Mendes, V.Morcelle, V.Scarduelli, D.S.Monteiro

Elastic and inelastic scattering for the 11B + 58Ni system: Target and projectile reorientation effects

NUCLEAR REACTIONS 58Ni(11B, 11B), (11B, 11B'), E=19.0, 20.0, 21.0, 23.0, 24.0, 25.0, 35.0 MeV; measured scattered particle spectra, σ(θ, E) at Tandar laboratory in Buenos Aires. 58Ni; measured σ(θ) for the first three excited states. Enriched target. Comparison with coupled-channel calculations. Discussed influence of 11B ground-state-spin reorientation and 58Ni first excited 2+ state on the reaction mechanism.

doi: 10.1103/PhysRevC.92.054615
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0788.

2014DU02      Phys.Rev. C 89, 014610 (2014)

S.Dubey, S.Mukherjee, D.C.Biswas, B.K.Nayak, D.Patel, G.K.Prajapati, Y.K.Gupta, B.N.Joshi, L.S.Danu, S.Mukhopadhyay, B.V.John, V.V.Desai, S.V.Suryanarayana, R.P.Vind, N.N.Deshmukh, S.Appnnababu, P.M.Prajapati

Effect of breakup processes on the near-barrier elastic scattering of the 6, 7Li + 232Th systems

NUCLEAR REACTIONS 232Th(6Li, 6Li), (7Li, 7Li), E=24, 26, 30, 32, 35, 40, 44 MeV; measured scattered 6,7Li particle spectra, σ(E, θ), total fusion and reaction σ(E) using ΔE-E telescopes at BARC-TIFR pelletron accelerator facility; analyzed data by optical potential model ECIS code with Woods-Saxon and Sao Paulo potentials. Indication of breakup threshold anomaly for 6Li scattering. Discussed role of projectile breakup on reaction mechanism.

doi: 10.1103/PhysRevC.89.014610
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6234.

2012BI15      J.Phys.:Conf.Ser. 381, 012091 (2012)

D.C.Biswas, P.Roy, Y.K.Gupta, B.N.Joshi, B.K.Nayak, L.S .Danu, B.V.John, R.P.Vind, N.Deshmukh, S.Mukherjee, A.K.Jain, R.K.Choudhury

Projectile structure effects in multi-nucleon and cluster transfers in 16, 18O+164Dy, 208Pb reactions

NUCLEAR REACTIONS 164Dy, 208Pb(16O, X), (18O, X), E=90, 96 MeV; measured reaction fragments using ΔE-E Si telescopes inside scattering chamber; deduced projectile-like fragments σ(θ).

doi: 10.1088/1742-6596/381/1/012091
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2012RA01      Nucl.Phys. A874, 14 (2012)

P.K.Rath, S.Santra, N.L.Singh, K.Mahata, R.Palit, B.K.Nayak, K.Ramachandran, V.V.Parkar, R.Tripathi, S.K.Pandit, S.Appannababu, N.N.Deshmukh, R.K.Choudhury, S.Kailas

Fusion of 6Li with 152Sm: Role of projectile breakup versus target deformation

NUCLEAR REACTIONS 152Sm(6Li, xn), E=20-40 MeV; measured Eγ, Iγ; deduced complete, incomplete fusion σ also for isomeric states 154Tbm1,154Tbm2, reaction mechanism; calculated σ using CC and statistical code PACE, fusion σ using proximity potentials; deduced level density parameters. Comparison of scaled σ with other reactions.

doi: 10.1016/j.nuclphysa.2011.10.004
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6180.

2011AP01      Phys.Rev. C 83, 034605 (2011)

S.Appannababu, S.Mukherjee, B.K.Nayak, R.G.Thomas, P.Sugathan, A.Jhingan, E.Prasad, D.Negi, N.N.Deshmukh, P.K.Rath, N.L.Singh, R.K.Choudhury

Fission fragment mass distributions in reactions forming the 213Fr compound nucleus

NUCLEAR REACTIONS 186W(27Al, X), E=123-140 MeV; 197Au(16O, X), E=79-100 MeV; measured fission fragment spectra; deduced density plots for mass ratio vs center of mass angle, mass ratio distributions 213Fr; deduced mass variance. Comparison with theoretical calculations.

doi: 10.1103/PhysRevC.83.034605
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2011DE05      Phys.Rev. C 83, 024607 (2011)

N.N.Deshmukh, S.Mukherjee, D.Patel, N.L.Singh, P.K.Rath, B.K.Nayak, D.C.Biswas, S.Santra, E.T.Mirgule, L.S.Danu, Y.K.Gupta, A.Saxena, R.K.Choudhury, R.Kumar, J.Lubian, C.C.Lopes, E.N.Cardozo, P.R.S.Gomes

Breakup threshold anomaly in the near-barrier elastic scattering of 6Li + 116, 112Sn

NUCLEAR REACTIONS 112Sn(6Li, 6Li), (6Li, X), E=21, 23, 25, 35 MeV; 116Sn(6Li, 6Li), (6Li, X), E=20, 21, 22, 23, 26, 30, 35 MeV; measured 6Li spectra by E-ΔE method; deduced elastic scattering σ and total reaction σ. Optical model analysis with phenomenological Woods-Saxon potential. Comparison of reduced cross sections with reaction cross sections for several other systems. Presence of the breakup threshold anomaly.

doi: 10.1103/PhysRevC.83.024607
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6098.

2011DE29      Eur.Phys.J. A 47, 118 (2011)

N.N.Deshmukh, S.Mukherjee, B.K.Nayak, D.C.Biswas, S.Santra, E.T.Mirgule, S.Appannababu, D.Patel, A.Saxena, R.K.Choudhury, J.Lubian, P.R.S.Gomes

Investigation of the threshold anomaly in the near-barrier elastic scattering of 7Li on 116Sn

NUCLEAR REACTIONS 116Sn(7Li, 7Li), E=18, 19, 20, 21, 22, 23, 24, 26, 30, 35 MeV; measured E(particle), I(particle, θ); calculated σ, σ(θ); deduced σ, σ(θ), optical potential parameters.

doi: 10.1140/epja/i2011-11118-0
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6172.

2010MU09      Eur.Phys.J. A 45, 23 (2010)

S.Mukherjee, N.N.Deshmukh, V.Guimaraes, J.Lubian, P.R.S.Gomes, A.Barioni, S.Appannababu, C.C.Lopes, E.N.Cardozo, K.C.C.Pires, R.Lichtenthaler, A.Lepine-Szily, D.S.Monteiro, J.M.B.Shorto, P.N.de Faria, E.Crema, V.Morcelle, M.C.Morais, R.P.Condori

Total reaction cross-sections for light weakly bound systems

NUCLEAR REACTIONS 9Be, 51V(8Li, 8Li), (8Li, X), E=18.5, 19.6 MeV; measured σ, σ(θ); calculated σ(θ) using Sao Paulo potential and WS form factors; deduced optical model parameters. Comparison with other reactions. Secondary radioactive beam.

doi: 10.1140/epja/i2010-10987-9
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0625.

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