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NSR database version of April 27, 2024.

Search: Author = B.S.Bhandari

Found 14 matches.

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1996AR14      Phys.Rev. C54, 3294 (1996)

J.D.T.Arruda-Neto, T.Saito, M.Sugawara, T.Tamae, H.Miyase, K.Abe, O.Konno, M.Oikawa, S.Simionatto, M.L.Yoneama, J.F.Dias, A.Deppman, B.S.Bhandari, V.P.Likhachev, A.C.S.Lima

Photoexcitation Mechanisms Investigated Through the Fission Channel

NUCLEAR REACTIONS 182W, 197Au, Ta(e, F), E not given; analyzed fission data; deduced σ(γ, F), compound nucleus excitation energy delineation related features.

doi: 10.1103/PhysRevC.54.3294
Citations: PlumX Metrics


1996YO04      Nucl.Phys. A604, 263 (1996)

M.-L.Yoneama, E.Jacobs, J.D.T.Arruda-Neto, B.S.Bhandari, D.De Frenne, S.Pomme, K.Persyn, K.Govaert

Study of the 232Th Fission Barrier by Electron-Induced Fission

NUCLEAR REACTIONS 232Th(e, F), E=4.5-7.9 MeV; measured electron induced σ, α(θ); deduced photofission σ for (1-, 0), (1-, 1), (2+0) channels, isomer fission, fission barrier.

doi: 10.1016/0375-9474(96)00159-5
Citations: PlumX Metrics


1995AR03      Phys.Rev. C51, R452 (1995)

J.D.T.Arruda-Neto, T.Saito, M.Sugawara, T.Tamae, H.Miyase, K.Abe, O.Konno, M.Oikawa, A.Deppman, S.Simionatto, E.M.L.Macedo, B.S.Bhandari

Photofission of 182W following Reabsorption of Photopions

NUCLEAR REACTIONS 182W(e, F), E=80-180 MeV; measured fission σ(E); deduced σ(γ, F), pion reabsorption σ. Enriched targets.

doi: 10.1103/PhysRevC.51.R452
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0773.


1992BH03      Phys.Rev. C45, 2803 (1992)

B.S.Bhandari, Y.B.Bendardaf

Systematics of the Deduced Fission Barriers for the Doubly Even Transactinium Nuclei

NUCLEAR STRUCTURE 236,238,240,242,244Pu, 240,242,244,246,248,250Cm; calculated isomer energies, T1/2, SF-decay T1/2, outer barrier heights. 230,232Th, 230,232,234,236,238U, 246,248,250,252,254,256Cf, 242,244,246,248,250,252,254,256,258Fm, 250,252,254,256,258,260,262No, 250Rf, 252Rf, 254Rf, 256Rf, 258Rf, 260Rf; calculated SF-decay T1/2, outer barrier height. Double humped fission barrier model. Other nuclei, other aspects discussed.

doi: 10.1103/PhysRevC.45.2803
Citations: PlumX Metrics


1991BH03      Phys.Rev.Lett. 66, 1034 (1991)

B.S.Bhandari

Resonant Tunneling and the Bimodal Symmetric Fission of 258Fm

RADIOACTIVITY 258Fm(SF); analyzed T1/2 data; deduced resonance tunneling evidence. Other nuclei considered.

doi: 10.1103/PhysRevLett.66.1034
Citations: PlumX Metrics


1991BH04      Phys.Rev. C44, 292 (1991)

B.S.Bhandari, M.Khaliquzzaman

Comparison of Various Parametrizations of the Double-Humped Fission Barrier

NUCLEAR STRUCTURE A=236-245; calculated SF-decay T1/2. Double humped fission barrier parametrization, different approaches.

doi: 10.1103/PhysRevC.44.292
Citations: PlumX Metrics


1990BH02      Phys.Rev. C42, 1443 (1990)

B.S.Bhandari

Test of the Adequacy of Using Smoothly Joined Parabolic Segments to Parametrize the Multihumped Fission Barriers in Actinides

NUCLEAR STRUCTURE 236,238U, 237Np, 235,237,238,239,240,241,242,243,244,245Pu, 239,240,241,242,243,244,245Am, 241,242,243,244,245Cm; calculated fission T1/2; deduced fission barrier parametrization.

doi: 10.1103/PhysRevC.42.1443
Citations: PlumX Metrics


1989BH01      Phys.Rev. C39, 917 (1989)

B.S.Bhandari, A.S.Al-Kharam

Tunneling through Equivalent Multihumped Fission Barriers: Some implications for the actinide nuclei

NUCLEAR STRUCTURE 232Th, 233,234,236,238U, 237Np, 238,239,240,242Pu, 241Am; analyzed fission data; deduced tunneling role. Photofission data.

doi: 10.1103/PhysRevC.39.917
Citations: PlumX Metrics


1980BH02      Phys.Rev. C22, 606 (1980)

B.S.Bhandari

Subbarrier Photofission of 238U

RADIOACTIVITY, Fission 238U(SF), 238mU; calculated T1/2. Double-hump barrier model.

NUCLEAR REACTIONS 238U(γ, F), E=5-8 MeV; calculated σ(E). Double-hump barrier model.

doi: 10.1103/PhysRevC.22.606
Citations: PlumX Metrics


1979BH03      Phys.Rev. C19, 1820 (1979)

B.S.Bhandari

Three-Hump Fission Barrier in 232Th

NUCLEAR REACTIONS 232Th(γ, F), E=3-7 MeV; calculated σ, T1/2. Three-hump fission barrier model.

doi: 10.1103/PhysRevC.19.1820
Citations: PlumX Metrics


1978AR09      Phys.Rev. C18, 863 (1978)

J.D.T.Arruda Neto, S.B.Herdade, B.S.Bhandari, I.C.Nascimento

Electric Quadrupole Giant Resonance in the Photofission of 238U

NUCLEAR REACTIONS 238U(e, F), E=5.5-28.3 MeV; measured yield, σ(fragment, θ); deduced E2 σ. 238U deduced E2 isoscalar giant resonance parameters.

doi: 10.1103/PhysRevC.18.863
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1978PR05      Phys.Rev. C18, 1531 (1978)

M.Prakash, B.S.Bhandari

Quantitative Resolution of 234Th Anomaly

NUCLEAR STRUCTURE 234Th; calculated fission penetrability through triple-humped potential barrier.

doi: 10.1103/PhysRevC.18.1531
Citations: PlumX Metrics


1976AR08      Phys.Rev. C14, 1499 (1976)

J.D.T.Arruda Neto, S.B.Herdade, B.S.Bhandari, I.C.Nascimento

Electrofission and Photofission of 238U in the Energy Range 6-60 MeV

NUCLEAR REACTIONS 238U(e, F), E=6-60 MeV; measured measured σ(E); deduced E1 contribution to fission process.

doi: 10.1103/PhysRevC.14.1499
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0533.


1976BH01      Nucl.Sci.Eng. 60, 19 (1976)

B.S.Bhandari, I.C.Nascimento

Present Status of Photofission of Actinides Near Threshold

doi: 10.13182/NSE76-A26853
Citations: PlumX Metrics


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