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NSR database version of April 11, 2024.

Search: Author = M.A.Eswaran

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1997MI17      Phys.Rev. C56, 1943 (1997)

E.T.Mirgule, M.A.Eswaran, S.Kumar, D.R.Chakrabarty, V.M.Datar, U.K.Pal, H.H.Oza, N.L.Ragoowansi

6α-Cluster Resonance Structures in 12C + 12C System and Their Decay in α and 8Be Channels

NUCLEAR REACTIONS 12C(12C, α), (12C, 8Be), E=48-72 MeV; measured σ(E, θ). 24Mg deduced non-statistical resonance structures. Hauser-Feshbach model.

doi: 10.1103/PhysRevC.56.1943
Citations: PlumX Metrics


1995MI02      Nucl.Phys. A583, 287c (1995)

E.T.Mirgule, S.Kumar, M.A.Eswaran, D.R.Chakrabarty, V.M.Datar, N.L.Ragoowansi, H.H.Oza, U.K.Pal

Investigation on the α-Particle Linear Chain Configuration in 24Mg at 46.4 MeV Excitation

NUCLEAR REACTIONS 12C(12C, α), (12C, 8Be), E=50-70 MeV; measured α-, 8Be spectra, σ(θ) vs E. 24Mg deduced resonance, decay features, α-chain character.

doi: 10.1016/0375-9474(94)00674-C
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1387.


1994KU18      Phys.Rev. C50, 1535 (1994)

S.Kumar, M.A.Eswaran, E.T.Mirgule, D.R.Chakrabarty, V.M.Datar, N.L.Ragoowansi, U.K.Pal, H.H.Oza

Structural Connection of Highly Deformed Shape Isomeric States in 28Si, 24Mg, and 20Ne by Alpha-Alpha Coincidence Studies in 12C(16O, α)24Mg(*) → α + 20Ne(*)

NUCLEAR REACTIONS 12C(16O, α), E=63 MeV; measured σ(θ(α1), θ(α2), E(α1)), αα-coin, following 24Mg breakup. 28Si, 24Mg, 20Ne deduced highly deformed shape isomers structural connection.

doi: 10.1103/PhysRevC.50.1535
Citations: PlumX Metrics


1993ES01      Phys.Rev. C47, 1418 (1993)

M.A.Eswaran, S.Kumar, E.T.Mirgule, D.R.Chakrabarty, V.M.Datar, N.L.Ragoowansi, U.K.Pal

Evidence for Superdeformed Shape Isomeric States in 28Si at Excitations Above 40 MeV Through Observations of Selective Particle Decays of 16O + 12C Resonances in 8Be and Alpha Channels

NUCLEAR REACTIONS 12C(16O, 8Be), (16O, α), E(cm)=25.7-38.6 MeV; measured spectra, σ(θ) vs E. 28Si deduced resonances, J, π, configuration, superdeformed isomeric states.

doi: 10.1103/PhysRevC.47.1418
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6144.


1993ES03      Phys.Rev. C48, 2120 (1993)

M.A.Eswaran, S.Kumar

Reply to ' Comment on ' Evidence for Superdeformed Shape Isomeric States in 28Si at Excitations Above 40 MeV Through Observations of Selective Particle Decays of 16O + 12C Resonances in 8Be and Alpha Channels ' '

NUCLEAR REACTIONS 12C(16O, 8Be), (16O, α), E(cm)=25.7-38.6 MeV; analyzed previous data analyses. 28Si deduced superdeformed shape isomeric states structure.

doi: 10.1103/PhysRevC.48.2120
Citations: PlumX Metrics


1990ES01      Phys.Rev. C42, 1036 (1990)

M.A.Eswaran, S.Kumar, E.T.Mirgule

Direct Cluster Transfer in 3He Bombardment of 13C at Sub-Barrier Energies

NUCLEAR REACTIONS 13C(3He, α), E(cm)=1.20, 1.05 MeV; measured σ(θ); deduced reaction mechanism. Exact finite-range DWBA analysis.

doi: 10.1103/PhysRevC.42.1036
Citations: PlumX Metrics


1989ES06      Phys.Rev. C39, 1856 (1989)

M.A.Eswaran, S.Kumar, E.T.Mirgule, N.L.Ragoowansi

Intermediate Structure in 12C + 16O System through Alpha-Induced Reactions on 24Mg in the Energy Range Eα = 26-37 MeV

NUCLEAR REACTIONS 24Mg(α, 12C), E=26-37 MeV; measured σ(Eα). 24Mg(α, α'), E=26-37 MeV; measured σ(θ); deduced final state intermediate structure. Statistical model, fluctuation analysis.

doi: 10.1103/PhysRevC.39.1856
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6288.


1983CH29      Phys.Rev. C28, 1012 (1983)

D.R.Chakrabarty, M.A.Eswaran, N.L.Ragoowansi

Spin and Isospin Characteristics of the Excited States of 36Ar through the Reaction 32S(α, γ)36Ar in the Bombarding Energy Range E(α) = 4 to 5 MeV

NUCLEAR REACTIONS, ICPND 32S(α, γ), E=4.13-5 MeV; measured γ yields, Eγ, Iγ, γ(θ). 36Ar deduced resonances, J, π, T, Γp, Γα, α-reduced width, γ-multipolarity, transition strength. Enriched target.

doi: 10.1103/PhysRevC.28.1012
Citations: PlumX Metrics


1982CH10      Phys.Rev. C25, 1933 (1982)

D.R.Chakrabarty, M.A.Eswaran

Cluster Representation of 6Li and the Finite-Range Distorted-Wave Born Approximation Analysis of 6Li-Induced Alpha Transfer Reactions

NUCLEAR REACTIONS 26Mg, 27Al, 29Si, 31P(6Li, d), E=36 MeV; calculated σ(θ). Finite-range DWBA, α-cluster representation of 6Li.

doi: 10.1103/PhysRevC.25.1933
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1979ES01      Nucl.Phys. A313, 467 (1979)

M.A.Eswaran, R.N.Boyd, E.Sugarbaker, R.Cook, H.E.Gove

The 16O(6Li, dγ)20Ne Reaction

NUCLEAR REACTIONS 16O(6Li, dγ), E=32 MeV; measured dγ(θ), σ(θd). Compared with DWBA, CCBA reactions.

doi: 10.1016/0375-9474(79)90513-X
Citations: PlumX Metrics


1979ES05      Nucl.Phys. A325, 269 (1979)

M.A.Eswaran, H.E.Gove, R.Cook, B.Sikora

The α-Transfer Reactions 27Al(6Li, d)31P, 29Si(6Li, d)33S and 31P(6Li, d)35Cl at 36 MeV

NUCLEAR REACTIONS 27Al, 29Si, 31P(6Li, d), E=36 MeV; measured σ(Ed, θ). 31P, 33S, 35Cl deduced Sα. Exact finite-range DWBA analysis.

doi: 10.1016/0375-9474(79)90163-5
Citations: PlumX Metrics


1979ES07      Nucl.Phys. A332, 525 (1979)

M.A.Eswaran, H.E.Gove, R.Cook, J.P.Draayer

A Study of the 19F(6Li, d)23Na Reaction at 36 MeV

NUCLEAR REACTIONS 19F(6Li, d), E=36.0 MeV; measured σ(Ed, θ). 23Na levels deduced Sα. DWBA, SU(3) models.

doi: 10.1016/0375-9474(79)90017-4
Citations: PlumX Metrics


1978ES01      Phys.Rev. C18, 1528 (1978)

M.A.Eswaran, H.E.Gove

Systematics of Ground State α-Cluster Spectroscopic Strengths for Odd-A sd-Shell Nuclei

NUCLEAR REACTIONS 17O, 19F, 21Ne, 23Na, 25Mg, 27Al, 29Si, 31P, 35Cl(6Li, d); analyzed data. 21Ne, 23Na, 25Mg, 27Al, 29Si, 31P, 33S, 35Cl, 39K deduced ground state Sα systematics.

doi: 10.1103/PhysRevC.18.1528
Citations: PlumX Metrics


1972ES02      Phys.Rev. C5, 1270 (1972)

M.A.Eswaran, M.Ismail, N.L.Ragoowansi

Studies on Analog States in 33Cl by Isospin-Forbidden Resonances in the Reaction 32S(p, γ)33Cl

RADIOACTIVITY 33Cl; measured T1/2, Iβ(t).

NUCLEAR REACTIONS 32S(p, γ), E=3.36-5.41 MeV; measured σ(E;Eγ). 33Cl deduced resonances, J, π, γ-branching, isobaric analogs.

doi: 10.1103/PhysRevC.5.1270
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1969ES02      Phys.Rev. 185, 1458 (1969)

M.A.Eswaran, M.Ismail, N.L.Ragoowansi

Study of the Low-Lying Levels of 27Mg by Angular-Correlation Measurements in the Reaction 26Mg(d, pγ)27Mg

NUCLEAR REACTIONS 26Mg(d, pγ), E = 2.9-3.5 MeV; measured σ(E;Ep, Eγ, θ(pγ)). 27Mg deduced levels, J, γ-branching, γ-mixing.

doi: 10.1103/PhysRev.185.1458
Citations: PlumX Metrics


1968ES01      Proc.Indian Acad.Sci. 67A, 19 (1968)

M.A.Eswaran, N.L.Ragoowansi

Spins of the First Two Excited States in 27Mg by an Angular Correlation Technique in the Reaction 26Mg(d, pγ)27Mg

NUCLEAR STRUCTURE 27Mg; measured not abstracted; deduced nuclear properties.


1965ES01      Nucl.Phys. 66, 401 (1965)

M.A.Eswaran, H.E.Gove, A.E.Litherland, C.Broude

Lifetimes of Excited States in Cu63, Cu65, Ni62 and Fe56 by Doppler Shift Attenuation Measurements

NUCLEAR REACTIONS 56Fe(16O, 16O'γ), E = 34 MeV; 62Ni, 63,65Cu(16O, 16O'γ), E = 36 MeV; measured (16O')(γ)-coin , Doppler shift. 56Fe, 62Ni, 63,65Cu levels deduced T1/2.

doi: 10.1016/0029-5582(65)90188-4
Citations: PlumX Metrics


1965EV03      Can.J.Phys. 43, 82 (1965)

H.C.Evans, M.A.Eswaran, H.E.Gove, A.E.Litherland, C.Broude

Lifetimes of the Low-Lying Levels of 20Ne

NUCLEAR STRUCTURE 20Ne, 12C; measured not abstracted; deduced nuclear properties.

doi: 10.1139/p65-007
Citations: PlumX Metrics


1964BR07      Bull. Am. Phys. Soc. 9, No. 4, 439, FA3 (1964)

C.Broude, M.A.Eswaran

Properties of Some Low-Lying States in 22Ne

NUCLEAR STRUCTURE 22Ne; measured not abstracted; deduced nuclear properties.


1964BR11      Can. J. Phys. 42, 1300 (1964)

C.Broude, M.A.Eswaran

Gamma-Ray Angular Correlation Measurements in Ne22

NUCLEAR STRUCTURE 22Ne; measured not abstracted; deduced nuclear properties.

doi: 10.1139/p64-117
Citations: PlumX Metrics


1964ES01      Phys.Letters 8, 52 (1964)

M.A.Eswaran, H.E.Gove, A.E.Litherland, C.Broude

Measurement of Lifetimes of Nuclear Excited States by Doppler Shift Attenuation Method

NUCLEAR STRUCTURE 65Cu, 63Cu, 62Ni, 56Fe; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(64)90796-6
Citations: PlumX Metrics


1964ES02      Can.J.Phys. 42, 1311 (1964)

M.A.Eswaran, C.Broude

Lifetime Measurements of States in O18 and Ne22

NUCLEAR STRUCTURE 7Li, 22Ne; measured not abstracted; deduced nuclear properties.

doi: 10.1139/p64-118
Citations: PlumX Metrics


1963ES01      Bull.Am.Phys.Soc. 8, No.4, 375, U3 (1963)

M.A.Eswaran, H.E.Gove, A.E.Litherland, C.Broude

Doppler-Shift Attenuation Measurements Following Coulomb Excitation in Cu63 and Cu65

NUCLEAR STRUCTURE 63Cu, 65Cu; measured not abstracted; deduced nuclear properties.


1963GO11      Phys.Canada 19, No.3, 36, Abstr.8.2 (1963)

H.E.Gove, A.E.Litherland, C.Broude, M.A.Eswaran

The Coulomb Excitation of Levels in Cu63 and Ni62

NUCLEAR STRUCTURE 63Cu, 62Ni; measured not abstracted; deduced nuclear properties.


1962VA02      Phys.Rev. 125, 656 (1962)

J.Varma, M.A.Eswaran

Decay of Se75 and the Lifetime of the 280-keV State of As75

NUCLEAR STRUCTURE 75Se; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.125.656
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