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NSR database version of April 11, 2024.

Search: Author = A.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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2015VI03      Pramana 85, 539 (2015)

P.K.Vijayan, A.Basak, I.V.Dulera, K.K.Vaze, S.Basu, R.K.Sinha

Conceptual design of Indian molten salt breeder reactor

doi: 10.1007/s12043-015-1070-0
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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, 7}Li 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, 48}Ca 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, 48}Ca

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, 30}Si(α, d)^{31, 32}P 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.

1987WA21      Nucl.Phys. A470, 339 (1987)

R.E.Warner, B.A.Vaughan, J.A.Ditusa, J.W.Rovine, R.S.Wakeland, C.P.Browne, S.E.Darden, S.Sen, A.Nadasen, A.Basak, T.R.Donoghue, T.Rinckel, K.Sale, G.C.Ball, W.G.Davies, A.J.Ferguson, J.S.Forster

The Mechanism of the ⁷Li(d, 2α)n Reaction from E(d) = 3 to 15 MeV

NUCLEAR REACTIONS, MECPD ⁷Li(d, 2α), E=3-15 MeV; measured σ(θ₁, θ₂) vs energy difference; deduced reaction mechanism. ⁸Be deduced levels. Enriched ⁷LiF targets.

doi: 10.1016/0375-9474(87)90006-6
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0316.

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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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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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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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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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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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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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

Note: The following list of authors and aliases matches the search parameter A.Basak: , A.K.BASAK