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NSR database version of April 11, 2024.

Search: Author = A.K.Basak

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2023JO03      Nucl.Phys. A1031, 122610 (2023)

F.Johora, D.Almalawi, M.Nure A.Abdullah, S.Hossain, Z.F.Shehadeh, A.K.Basak

Non-monotonic potential description of α+209Bi elastic scattering

NUCLEAR REACTIONS 209Bi(α, α), E=19-104 MeV; analyzed available data; deduced σ(θ), σ, potential parameters using the non-monotonic (NM) potential in the framework of optical model (OM).

doi: 10.1016/j.nuclphysa.2023.122610
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2022BA24      Europhys.Lett. 138, 44002 (2022)

A.K.Basak, A.C.Merchant, M.Freer, M.S.Islam, R.A.Ramon, M.Mizanur Rahman, A.S.B.Tariq, M.A.Uddin, A.Soylu

16O + 16O cluster states and their fusion to 32S: A non-monotonic potential description

NUCLEAR REACTIONS 16O(16O, X)32S, E=25-1120 MeV; analyzed available data; calculated σ, rotational constants, potential families, quasi-molecular states, bands, optical and nuclear models potentials.

doi: 10.1209/0295-5075/ac6c48
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2021IS08      J.Phys.(London) G48, 075109 (2021)

M.S.Islam, R.A.Ramon, M.Mizanur Rahman, R.Majumder, M.A.Sayed, A.Nilima, M.M.B.Azad, A.S.B.Tariq, M.A.Uddin, A.K.Basak

Nature of potential families from elastic 16O +16O rainbow scattering

NUCLEAR REACTIONS 16O(16O, 16O), E=75-1120 MeV; analyzed available data; deduced optical potential parameters, σ.

doi: 10.1088/1361-6471/abd88e
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2021IS12      J.Phys.(London) G48, 125108 (2021)

M.S.Islam, R.A.Ramon, M.M.Rahman, M.S.Islam, M.M.B.Azad, A.S.B.Tariq, M.A.Uddin, S.Ali, A.K.Basak

Primary rainbow and Airy minima in 12C + 12C elastic scattering with families of non-monotonic potentials

NUCLEAR REACTIONS 12C(12C, 12C), E=25-360 MeV; analyzed available data; deduced σ, optical model parameters within the framework of the optical model (OM) using non-monotonic (NM) nucleus-nucleus potential.

doi: 10.1088/1361-6471/ac2fb0
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2015HO06      Phys.Rev. C 91, 064613 (2015)

S.Hossain, A.S.B.Tariq, A.Nilima, M.S.Islam, R.Majumder, M.A.Sayed, M.M.Billah, M.M.B.Azad, M.A.Uddin, I.Reichstein, F.B.Malik, A.K.Basak

Dependence of the 16O+16O nuclear potential on nuclear incompressibility

NUCLEAR REACTIONS 16O(16O, 16O), E=31.0, 41.0, 49.0, 59.0, 75.0, 80.6, 87.2, 92.4, 94.8, 98.6, 103.1, 115.9, 124.0, 145.0, 250.0, 350.0 MeV; analyzed σ(E, θ) data in the optical model using Nonmonotonic (NM) nucleus-nucleus potentials from energy-density functional (EDF) theory, and for nuclear incompressibility in K=188-266 MeV range.

doi: 10.1103/PhysRevC.91.064613
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2013HO02      Phys.Scr. 87, 015201 (2013)

S.Hossain, M.N.A.Abdullah, Md.Zulfiker Rahman, A.K.Basak, F.B.Malik

Non-monotonic potentials for 6Li elastic scattering at 88 MeV

NUCLEAR REACTIONS 24,25,26Mg, 27Al, 40,44Ca, 59Co, 60Ni, 197Au, 206,208Pb(6Li, 6Li), E=88 MeV; analyzed available data, performance of the traditional phenomenological Woods-Saxon (WS) and squared WS potentials with that of a non-monotonic potential; deduced energy density functional, σ(θ). Comparison with available data.

doi: 10.1088/0031-8949/87/01/015201
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2013HO16      J.Phys.(London) G40, 105109 (2013)

S.Hossain, M.Billah, M.M.B.Azad, F.Parvin, M.N.A.Abdullah, K.M.Hasan, M.A.Uddin, A.S.B.Tariq, A.K.Basak, I.Reichstein, F.B.Malik

Non-monotonic potential description of alpha-Zr refractive elastic scattering

NUCLEAR REACTIONS 90Zr(α, α), E=15-141.7 MeV; analyzed available data; deduced scattering parameters, σ. Optical model framework using non-monotonic potentials.

doi: 10.1088/0954-3899/40/10/105109
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2013UD01      Eur.Phys.J. D 67, 214 (2013)

M.A.Uddin, A.K.F.Haque, T.I.Talukder, A.K.Basak, B.C.Saha, F.B.Malik

Semi-empirical model for stopping cross sections of p, α and Li ions

NUCLEAR REACTIONS Mo, Au(α, X), (p, X), (Li, X), E<100 MeV; calculated stopping σ for Z=2-100; Comparison with available data.

doi: 10.1140/epjd/e2013-40164-8
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2011BA23      Europhys.Lett. 94, 62002 (2011)

A.K.Basak, M.M.Billah, M.J.Kobra, M.K.Sarkar, M.Mizanur Rahman, Pretam K.Das, S.Hossain, M.N.A.Abdullah, A.S.B.Tariq, M.A.Uddin, S.Bhattacharjee, I.Reichstein, F.B.Malik

Non-monotonic potentials and vector analyzing powers of 6, 7Li scattering by 12C, 26Mg, 58Ni, and 120Sn

NUCLEAR REACTIONS 12C, 26Mg, 58Ni(6Li, 6Li), (7Li, 7Li), E=20 MeV; 120Sn(6Li, 6Li), (7Li, 7Li), E=44 MeV; calculated σ, vector analyzing power. Optical model potential, comparison with experimental data.

doi: 10.1209/0295-5075/94/62002
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2009HO11      Eur.Phys.J. A 41, 215 (2009)

S.Hossain, M.N.A.Abdullah, A.K.Basak, S.K.Das, M.A.Uddin, A.S.B.Tariq, I.Reichstein, K.M.Rusek, F.B.Malik

Potential description of 6Li elastic scattering by 28Si

NUCLEAR REACTIONS 28Si(6Li, 6Li), E=7.5, 9.0, 11.0, 13.0, 22.8, 25.0, 27.0, 30.0, 34.0, 46.0, 75.6, 99.0, 135.0, 154.0, 210.0, 318.0 MeV; calculated σ(θ) using the energy-density functional formalism with different potentials; deduced parameters for the various potentials.

doi: 10.1140/epja/i2009-10813-7
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2008HO15      Europhys.Lett. 84, 52001 (2008)

S.Hossain, M.N.A.Abdullah, A.S.B.Tariq, M.A.Uddin, A.K.Basak, K.M.Rusek, I.Reichstein, F.B.Malik

Microscopic 6Li-28Si potential from the energy-density functional theory

NUCLEAR REACTIONS 28Si(7Li, 7Li), E=7.5-99.0 MeV; analyzed σ(θ).

doi: 10.1209/0295-5075/84/52001
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2008TA01      Eur.Phys.J. D 46, 281 (2008)

M.R.Talukder, S.Bose, M.A.R.Patoary, A.K.F.Haque, M.A.Uddin, A.K.Basak, M.Kando

Empirical model for electron impact ionization cross sections of neutral atoms

ATOMIC PHYSICS H, He, Li, C, N, O, F, Ne, Na, Mg, Al, Si, P, S, Cl, Ar, Fe, Cu, Ga, Ge, As, Se, Br, Kr, Ag, In, Sn, Sb, Te, I, Xe, Ba, Hg, Pb, Bi, U(e, X), E < 10 MeV; calculated electron impact total ionization cross sections for both open and closed shell neutral atoms using an empirical expression.

doi: 10.1140/epjd/e2007-00318-y
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2006AB32      Nucl.Phys. A775, 1 (2006)

M.N.A.Abdullah, M.S.Sabra, M.M.Rashid, Z.Shehadeh, M.M.Billah, S.K.Das, M.A.Uddin, A.K.Basak, I.Reichstein, H.M.Sen Gupta, F.B.Malik

Alpha-alpha potential up to 47.3 MeV bombarding energy

NUCLEAR REACTIONS 4He(α, α), E=2.0-47.3 MeV; analysed σ, σ(θ); deduced parameters. 8Be deduced decay width. Various non-monotonic and Woods-Saxon α-nucleus potentials compared, phase shift effects discussed.

doi: 10.1016/j.nuclphysa.2006.06.007
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2006HO04      Phys.Lett. B 636, 248 (2006)

S.Hossain, M.N.A.Abdullah, K.M.Hasan, M.Asaduzzaman, M.A.R.Akanda, S.K.Das, A.S.B.Tariq, M.A.Uddin, A.K.Basak, S.Ali, F.B.Malik

Shallow folding potential for 16O + 12C elastic scattering

NUCLEAR REACTIONS 16O(α, α), E=23.2-172.5 MeV; 12C(16O, 16O), E=132.0-260.0 MeV; calculated σ(θ). 12C deduced radius, α-cluster structure. Folding model, comparisons with data.

doi: 10.1016/j.physletb.2006.03.071
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2005AB24      Nucl.Phys. A760, 40 (2005)

M.N.A.Abdullah, A.B.Idris, A.S.B.Tariq, M.S.Islam, S.K.Das, M.A.Uddin, A.S.Mondal, A.K.Basak, I.Reichstein, H.M.Sen Gupta, F.B.Malik

Potentials for the α- 40, 44, 48Ca elastic scattering

NUCLEAR REACTIONS 40,44,48Ca(α, α), E=10-180 MeV; analyzed σ(θ); deduced parameters. Non-monotonic and Squared Woods-Saxon α-nucleus potentials compared, dispersion effects discussed.

doi: 10.1016/j.nuclphysa.2005.05.149
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2005BI23      Nucl.Phys. A762, 50 (2005)

M.M.Billah, M.N.A.Abdullah, S.K.Das, M.A.Uddin, A.K.Basak, I.Reichstein, H.M.Sen Gupta, F.B.Malik

Alpha-Ni optical model potentials

NUCLEAR REACTIONS 58,60,62,64Ni(α, α), E ≈ 15-166 MeV; calculated σ(θ). Four optical potentials compared with data.

doi: 10.1016/j.nuclphysa.2005.07.020
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2005HO12      J.Phys.(London) G31, 309 (2005)

S.Hossain, M.N.A.Abdullah, S.K.Das, M.A.Uddin, A.K.Basak, H.M.Sen Gupta, I.J.Thompson, F.B.Malik

Band mixing in 29Si and 29P

NUCLEAR REACTIONS 28Si(α, t), (α, 3He), E=45 MeV; analyzed σ(E, θ). 29P, 29Si deduced configurations, band-mixing effects. Coupled channels approach, finite-range transfer theory, Nilsson model.

doi: 10.1088/0954-3899/31/5/003
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2003AB11      J.Phys.(London) G29, 1259 (2003)

M.N.A.Abdullah, S.K.Das, A.S.B.Tariq, M.S.Mahbub, A.S.Mondal, M.A.Uddin, A.K.Basak, H.M.Sen Gupta, F.B.Malik

Molecular versus squared Woods-Saxon α-nucleus potentials in the 27Al(α, t)28Si reaction

NUCLEAR REACTIONS 27Al(α, t), (α, α), E=64.5 MeV; calculated σ(θ), σ(E, θ). Comparison of Woods-Saxon and molecular potentials, comparison with data.

doi: 10.1088/0954-3899/29/6/323
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2003AB22      Phys.Lett. B 571, 45 (2003)

M.N.A.Abdullah, M.S.I.Sarker, S.Hossain, S.K.Das, A.S.B.Tariq, M.A.Uddin, A.S.Mondal, A.K.Basak, S.Ali, H.M.Sen Gupta, F.B.Malik

Cluster structure of 40, 44, 48Ca

NUCLEAR REACTIONS 40,44,48Ca(α, α), E=22-166 MeV; analyzed σ(θ); deduced parameters. 40,44,48Ca deduced α-cluster structure. Folded potential.

doi: 10.1016/j.physletb.2003.08.014
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2003AB24      Eur.Phys.J. A 18, 65 (2003)

M.N.A.Abdullah, S.Hossain, M.S.I.Sarker, S.K.Das, A.S.B.Tariq, M.A.Uddin, A.K.Basak, S.Ali, H.M.Sen Gupta, F.B.Malik

Cluster structure of 16O

NUCLEAR REACTIONS 16O(α, α), E=25.4-146.0 MeV; calculated σ(θ). 16O deduced radius. Folding model, α-cluster configurations, comparisons with data.

doi: 10.1140/epja/i2003-10068-7
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2002AB22      Eur.Phys.J. A 15, 477 (2002)

M.N.A.Abdullah, M.S.Mahbub, S.K.Das, A.S.B.Tariq, M.A.Uddin, A.K.Basak, H.M.Sen Gupta, F.B.Malik

Investigation of α-nucleus interaction in the 27Al(α, α)27Al scattering and 27Al(α, d)29Si reaction

NUCLEAR REACTIONS 27Al(α, α), E=22.3-64.5 MeV; analyzed σ(θ); deduced potential parameters. 27Al(α, d), E=26.5, 27.2 MeV; calculated spectroscopic factors, σ(θ). Molecular and Michel potentials, DWBA.

doi: 10.1140/epja/i2002-10066-0
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2001BB08      Eur.Phys.J. A 12, 387 (2001)

A.K.Basak, M.N.A.Abdullah, A.S.B.Tariq, S.K.Das, A.F.M.M.Rahman, A.S.Mondal, H.M.Sen Gupta, F.B.Malik

Investigation of Inelastic α-Scattering on 24Mg and 28Si

NUCLEAR REACTIONS 24Mg(α, α'), E=54 MeV; 28Si(α, α'), E=26 MeV; measured σ(E, θ); deduced potential parameters. Coupled channels analysis.

doi: 10.1007/s10050-001-8662-4
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2001DA19      Phys.Rev. C64, 034605 (2001)

S.K.Das, A.S.B.Tariq, A.F.M.M.Rahman, S.Hossain, A.S.Mondal, A.K.Basak, H.M.Sen Gupta, F.B.Malik

Effect of the α-Nucleus Interaction on the 29, 30Si(α, d)31, 32P Reaction

NUCLEAR REACTIONS 29,30Si(α, d), E=25 MeV; calculated σ(E, θ), spectroscopic factors. Microscopic and macroscopic DWBA calculations, comparison of molecular, standard and squared Woods-Saxon α-nucleus potentials.

doi: 10.1103/PhysRevC.64.034605
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2000DA28      Phys.Rev. C62, 054605 (2000)

S.K.Das, A.S.B.Tariq, M.A.Uddin, A.S.Mondal, A.K.Basak, K.M.Rashid, H.M.Sen Gupta, F.B.Malik

Effect of α-Nucleus Potential on the 28Si(α, d)30P Reaction

NUCLEAR REACTIONS 28Si(α, d), E=26 MeV; analyzed σ(E, θ). 30P level deduced J, π. DWBA calculations, several potentials compared.

doi: 10.1103/PhysRevC.62.054605
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2000DA29      Phys.Rev. C62, 054606 (2000)

S.K.Das, A.K.Basak, K.Banu, A.S.Mondal, A.S.B.Tariq, A.F.M.M.Rahman, H.M.Sen Gupta, F.B.Malik

Effect of the α-Nucleus Potential on the 28Si(α, p)31P Reaction

NUCLEAR REACTIONS 28Si(α, α), (α, p), E=26 MeV; analyzed σ(E, θ). DWBA calculations, several potentials compared.

doi: 10.1103/PhysRevC.62.054606
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1999DA20      Phys.Rev. C60, 044617 (1999); Comment Phys.Rev. C62, 049801 (2000)

S.K.Das, A.S.B.Tariq, A.F.M.Rahman, R.K.Roy, M.N.Huda, A.S.Mondal, A.K.Basak, H.M.Sen Gupta, F.B.Malik

Effect of α-Nucleus Potential on the 27Al(α, t)28Si Reaction

NUCLEAR REACTIONS 27Al(α, α), E=64.5 MeV; analyzed σ(θ); deduced parameters. 27Al(α, t), E=64.5 MeV; calculated σ(E, θ). 28Si deduced spectroscopic factors. Finite-range DWBA, molecular and Michel optical potentials. Comparisons with data.

doi: 10.1103/PhysRevC.60.044617
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1999DA24      Nuovo Cim. 112A, 661 (1999)

S.K.Das, A.K.Basak, A.S.Mondal, A.S.B.Tariq, A.F.M.Rahman, D.R.Sarker, H.M.Sen Gupta

Normalization Constant of the (α, t) Reaction

NUCLEAR REACTIONS 16O, 19F, 25Mg, 27Al, 30Si, 40Ca, 51V, 55Mn, 54Fe, 59Co, 64Ni, 116Sn, 144Sm, 208Pb(α, t), E=25-104 MeV; analyzed σ(θ); deduced normalization constant. DWBA analysis.

doi: 10.1007/BF03035876
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1999TA13      Phys.Rev. C59, 2558 (1999)

A.S.B.Tariq, A.F.M.M.Rahman, S.K.Das, A.S.Mondal, M.A.Uddin, A.K.Basak, H.M.Sen Gupta, F.B.Malik

Potential Description of Anomalous Large Angle Scattering of α Particles

NUCLEAR REACTIONS 28Si(α, α), E=14.47-45 MeV; 30Si(α, α), E=26.6 MeV; 24Mg(α, α), E=22-120 MeV; analyzed σ(θ); deduced potential parameters. Michel, molecular potentials, anomalous large angle scattering.

doi: 10.1103/PhysRevC.59.2558
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1998HA68      Nuovo Cim. 111, 1131 (1998)

M.Haque, S.K.Das, A.K.Basak, H.M.Sen Gupta

Anomaly in the Normalization Constant of the (3He, p) Reaction

NUCLEAR REACTIONS 62Ni(3He, p), E not given; calculated DWBA normalization constants; deduced dependence on final level, possible multi-step mechanisms.


1997BA60      Phys.Rev. C56, 1983 (1997)

A.K.Basak, M.A.Basher, A.S.Mondal, M.A.Uddin, S.Bhattacherjee, A.Husain, S.K.Das, M.Haque, H.M.Sen Gupta

64Cu Levels from the 62Ni(3He, p) Reaction at 18 MeV

NUCLEAR REACTIONS 62Ni(3He, p), E=18 MeV; measured proton spectra, σ(Ep, θ); deduced optical model parameters. 64Cu levels deduced J, π. Shell model analysis.

doi: 10.1103/PhysRevC.56.1983
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1992BA16      Phys.Rev. C45, 1575 (1992)

M.A.Basher, H.R.Siddique, A.Husain, A.K.Basak, H.M.Sen Gupta

Level Structure of 52Cr from the 51V(3He, d) Reaction

NUCLEAR REACTIONS 51V(3He, d), E=15 MeV; measured σ(θ). 52Cr deduced levels, L, J, π, spectroscopic factors. DWBA analysis.

doi: 10.1103/PhysRevC.45.1575
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1989BA24      Nucl.Phys. A499, 353 (1989)

A.K.Basak

Parity-Violating Effects in the 6Li(α, γ)10B Capture Reaction via the 5.1 MeV Doublet Resonance

NUCLEAR REACTIONS 6Li(α, γ), E=1.085, 1.175 MeV; measured σ(θ). 10B levels deduced γ-transition strengths, mixing ratio. Enriched target.

doi: 10.1016/0375-9474(89)90051-1
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0058.


1986DR03      Nucl.Phys. A448, 93 (1986)

P.V.Drumm, O.Karban, A.K.Basak, P.M.Lewis, S.Roman, G.C.Morrison

Study of 14N by One-Nucleon Transfer Reactions Induced with Polarised 3He

NUCLEAR REACTIONS 13C, 15N(polarized 3He, 3He), 13C(polarized 3He, d), 15N(polarized 3He, α), E=33 MeV; measured σ(θ), A(θ); deduced optical-model parameters. 14N levels deduced j-transfer values, S(lj).

doi: 10.1016/0375-9474(86)90182-X
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0086.


1984TO12      Phys.Lett. 149B, 9 (1984)

J.A.Tostevin, J.M.Nelson, O.Karban, A.K.Basak, S.Roman

Direct Observation of the Alpha Particle D-State in the (d, α) Reaction

NUCLEAR REACTIONS 40Ca(polarized d, α), E=12.3 MeV; calculated σ(θ), vector analyzing power vs θ; deduced α-particle D-state role. DWBA, cluster transfer.

doi: 10.1016/0370-2693(84)91540-5
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1983LE03      Nucl.Phys. A395, 204 (1983)

P.M.Lewis, A.K.Basak, J.D.Brown, P.V.Drumm, O.Karban, E.C.Pollacco, S.Roman

The Elastic and Inelastic Scattering of 33 MeV Polarized 3He from Oxygen and Iron Isotopes

NUCLEAR REACTIONS 17,18O, 54,56Fe(polarized 3He, 3He), (polarized 3He, 3He'), E=33 MeV; measured σ(θ), A(θ); deduced optical model parameters, deformation parameters. Enriched targets.

doi: 10.1016/0375-9474(83)90096-9
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1982KA12      Phys.Lett. 112B, 433 (1982)

O.Karban, A.K.Basak, P.M.Lewis, S.Roman

Configurations of Particle-Hole States in 16O

NUCLEAR REACTIONS 17O(polarized 3He, α), E=33 MeV; measured σ(θ), analyzing power vs θ. 16O levels deduced L, j-transfer, C2S, configurations. DWBA analysis.

doi: 10.1016/0370-2693(82)90842-5
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1981BA37      Nucl.Phys. A368, 74 (1981)

A.K.Basak, O.Karban, S.Roman, G.C.Morrison, C.O.Blyth, J.M.Nelson

Scattering and Charge-Exchange Reactions with Polarized 3He on Lithium Isotopes

NUCLEAR REACTIONS 6,7Li(polarized 3He, 3He), (polarized 3He, 3He'), (polarized 3He, t), E=33.3 MeV; measured σ(θ), A(θ); deduced optical-model parameters, reaction mechanism. Enriched 6Li target.

doi: 10.1016/0375-9474(81)90731-4
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1981BA38      Nucl.Phys. A368, 93 (1981)

A.K.Basak, O.Karban, S.Roman, G.C.Morrison, C.O.Blyth, J.M.Nelson

Polarization Effects in 3He Induced Transfer Reactions on Lithium Isotopes

NUCLEAR REACTIONS 6,7Li(polarized 3He, d), (polarized 3He, α), E=33.3 MeV; measured σ(θ), A(θ). 7,8Be, 5,6Li levels deduced S. Enriched 6Li target. DWBA, coupled-channels analyses.

doi: 10.1016/0375-9474(81)90732-6
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1981EN04      Nucl.Phys. A366, 1 (1981)

F.Entezami, A.K.Basak, O.Karban, P.M.Lewis, S.Roman

Interactions of Polarized 3He Particles with 24Mg

NUCLEAR REACTIONS 24Mg(polarized 3He, 3He), (polarized 3He, 3He'), (polarized 3He, d), (polarized 3He, α), E=33.3 MeV; measured σ(θ), A(θ); deduced contribution of two-step processes. Enriched target. DWBA, coupled-channels analysis.

doi: 10.1016/0375-9474(81)90483-8
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1818.


1981KA24      Nucl.Phys. A366, 68 (1981)

O.Karban, A.K.Basak, F.Entezami, S.Roman

Spectroscopy of 62Ni with the 61Ni(d(pol), p) Reaction

NUCLEAR REACTIONS 61Ni(polarized d, p), E=12.3 MeV; measured σ(θ), iT11, T20, T22 vs (θ). 62Ni deduced levels, L, j-transfer, π, (2J+1)S. Enriched target.

doi: 10.1016/0375-9474(81)90488-7
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1817.


1981KA38      Nucl.Phys. A369, 38 (1981)

O.Karban, A.K.Basak, F.Entezami, P.M.Lewis, S.Roman

Analysing Powers of the 54Fe(3He(pol), d)55Co and 54Fe(3He(pol), α)53Fe Reactions

NUCLEAR REACTIONS 54Fe(polarized 3He, d), (polarized 3He, α), E=33 MeV; measured σ(θ), A(θ). 55Co, 53Fe levels deduced J, π, C2S, j-dependence. Enriched target.

doi: 10.1016/0375-9474(81)90005-1
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1815.


1980OK04      Nucl.Phys. A349, 339 (1980)

N.T.Okumusoglu, A.K.Basak, C.O.Blyth

Analyzing Powers in the Three-Body Break-Up Reactions from 3He(pol) + 2H

NUCLEAR REACTIONS 2H(polarized 3He, 2p), (polarized 3He, pt), (polarized 3He, p3He), E=33 MeV; measured σ(Ep, θ1, θ2), analyzing power vs Ep.

doi: 10.1016/0375-9474(80)90291-2
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0339.


1978BA13      Nucl.Phys. A295, 111 (1978)

A.K.Basak, J.A.R.Griffith, O.Karban, J.M.Nelson, S.Roman

Tensor Analysing Powers of (d, p) Reactions on 28Si, 67Zn, 90Zr and 208Pb at 12.3 MeV

NUCLEAR REACTIONS 28Si, 67Zn, 90Zr, 208Pb(polarized d, p), E=12.3 MeV; measured analyzing powers iT11(θ), T20(θ); deduced J-transfers. 68Zn level deduced J, π. Natural 28Si; enriched 67Zn, 90Zr, 208Pb targets.

doi: 10.1016/0375-9474(78)90023-4
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1978LU05      Nucl.Phys. A297, 189 (1978)

Y.-W.Lui, O.Karban, A.K.Basak, C.O.Blyth, J.M.Nelson, S.Roman

Scattering of Polarized 3He by 4He between 18 and 32 MeV

NUCLEAR REACTIONS 4He(polarized 3He, 3He), E=18-32 MeV; measured A(θ); deduced phase shifts. 7Be deduced level, J, π.

doi: 10.1016/0375-9474(78)90271-3
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1978TU07      Fizika, Suppl. 10, 51 (1978)

G.Tungate, J.A.R.Griffith, O.Karban, A.K.Basak

Elastic Scattering of 12.4 MeV Tensor Polarized Deuterons

NUCLEAR REACTIONS 64Ni, 65Cu, 90Zr(polarized d, d), E=12.4 MeV; measured σ(θ), iT11(θ), T20(θ), T22(θ). Optical model analysis with tensor terms.


1977BA04      Nucl.Phys. A275, 381 (1977)

A.K.Basak, J.A.R.Griffith, O.Karban, J.M.Nelson, S.Roman, G.Tungate

Polarization Transfer in the 28Si(d, p)29Si(g.s.) Reaction and Deuteron D-State Effects

NUCLEAR REACTIONS 28Si(polarized d, p), E=12.1 MeV; measured polarization transfer coefficient at θ(lab)=10°, 20°; deduced evidence of deuteron d-state contribution.

doi: 10.1016/0375-9474(77)90459-6
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1977BA14      Nucl.Phys. A278, 217 (1977)

A.K.Basak, J.A.R.Griffith, M.Irshad, O.Karban, E.J.Ludwig, J.M.Nelson, S.Roman, G.Tungate

Spectroscopy of the 50Cr(d, p)51Cr Reaction and the Deuteron d-State Effects

NUCLEAR REACTIONS 50Cr(polarized d, p), E=12.3 MeV; measured analyzing powers iT11(θ), T20(θ), T22(θ). 51Cr levels deduced J. Enriched target.

doi: 10.1016/0375-9474(77)90236-6
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1977BA39      Nucl.Phys. A286, 420 (1977)

A.K.Basak, J.A.R.Griffith, O.Karban, S.Roman, G.Tungate

Analysing Powers of the (d, p) and (d, t) Reactions Induced by 12 MeV Polarized Deuterons in the 1p Shell

NUCLEAR REACTIONS 9Be(polarized d, p), 9Be(polarized d, t), E=12 MeV; measured iT11, T20, T22(θ); 12C(polarized d, p), E=12.3 MeV; measured T20, T22; deduced J-mixing ratio. Natural targets.

doi: 10.1016/0375-9474(77)90593-0
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1977KA10      J.Phys.(London) G3, 571 (1977)

O.Karban, A.K.Basak, C.O.Blyth, W.Dahme, J.B.A.England, J.M.Nelson, N.T.Okumusoglu, S.Roman, G.G.Shute, R.Vlastou

Scattering of 33 MeV Polarized 3He Particles by Hydrogen and Helium Isotopes

NUCLEAR REACTIONS 1,2,3H, 3,4He(polarized 3He, 3He), E=33.3 MeV; measured A(θ); deduced optical-model parameters.

doi: 10.1088/0305-4616/3/4/017
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1093.


1977RO12      Nucl.Phys. A284, 365 (1977)

S.Roman, A.K.Basak, J.B.A.England, O.Karban, G.C.Morrison, J.M.Nelson

Polarization Effects in the Elastic Scattering of 3He and (3He, d) Reaction on 58Ni

NUCLEAR REACTIONS 58Ni(polarized 3He, 3He), 58Ni(polarized 3He, d), E=33.3 MeV; measured A(θ). Enriched target.

doi: 10.1016/0375-9474(77)90390-6
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1977RO17      Nucl.Phys. A289, 269 (1977)

S.Roman, A.K.Basak, J.B.A.England, J.M.Nelson, N.E.Sanderson, F.D.Santos, A.M.Eiro

3He D-State Effects in (d, 3He) Reactions

NUCLEAR REACTIONS 27Al(polarized d, 3He), E=12.4 MeV; measured iT11, T20, T22(θ); deduced 3He d-state contribution. Natural target.

doi: 10.1016/0375-9474(77)90032-X
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1976KA20      Nucl.Phys. A266, 413 (1976)

O.Karban, A.K.Basak, J.A.R.Griffith, S.Roman, G.Tungate

Tensor Analysing Powers in Deuteron Elastic Scattering by 50Cr, 66Zn and 67Zn

NUCLEAR REACTIONS 50Cr, 66,67Zn(d, d), E=12.4 MeV; measured σ(θ), iT11, T20, T22(θ); deduced tensor optical model parameters. Enriched targets.

doi: 10.1016/0375-9474(76)90367-5
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1976KA23      Nucl.Phys. A269, 312 (1976)

O.Karban, A.K.Basak, J.B.A.England, G.C.Morrison, J.M.Nelson, S.Roman, G.G.Shute

The j-Dependence of (3He, d) and (3He, α) Reaction Analysing Powers in the 1p Shell

NUCLEAR REACTIONS 9Be, 12C(polarized 3He, d), (polarized 3He, α), E=33.3 MeV; measured σ(θ), A(θ); deduced J-dependence. 10B, 8Be, 13N, 11C levels deduced S.

doi: 10.1016/0375-9474(76)90683-7
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetR0022.


1976SA26      Phys.Rev.Lett. 37, 1672 (1976)

N.E.Sanderson, A.K.Basak, J.B.A.England, J.M.Nelson, S.Roman

Investigation of d5/2-d3/2 Admixing in the Pickup Strength to the First Excited States of 22Ne and 26Mg

NUCLEAR REACTIONS 23Na, 27Al(polarized d, 3He), E=12.4 MeV; measured vector analyzing power iT11; deduced admixing in pickup strength to levels in 22Ne, 26Mg.

doi: 10.1103/PhysRevLett.37.1672
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1974BA49      Nucl.Phys. A229, 219 (1974)

A.K.Basak, J.A.R.Griffith, M.Irshad, O.Karban, E.J.Ludwig, J.M.Nelson, S.Roman

Vector Analyzing Power of (d, p) and (d, t) Reactions on 142Nd at 12.3 MeV

NUCLEAR REACTIONS 142Nd(polarized d, d), (polarized d, p), (polarized d, t), E=12.3 MeV; measured iT11(θ); deduced optical-model parameters, reaction characteristics. 143Nd levels deduced L(n), J, S; 141Nd levels deduced L(n), J. Enriched target.

doi: 10.1016/0375-9474(74)90784-2
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1971HU18      Nucleus (Lahore) 8, 55 (1971)

A.Husain, M.M.Kasim, A.K.Basak, A.S.Mandal, P.Ali, B.C.Saha

The Lifetime of Heavy Spallation Hyperfragments


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