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NSR database version of April 26, 2024.

Search: Author = J.Joseph

Found 19 matches.

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2020HO02      Phys.Rev. C 101, 014616 (2020)

M.M.Hosamani, N.M.Badiger, N.Madhavan, I.Mazumdar, S.Nath, J.Gehlot, A.K.Sinha, S.M.Patel, P.B.Chavan, T.Varughese, Vi.Srivastava, M.M.Shaikh, P.S.Devi, P.V.Laveen, A.Shamlath, M.Shareef, S.K.Duggi, P.V.Madhusudhana Rao, G.N.Jyothi, A.Tejaswi, P.N.Patil, A.Vinayak, K.K.Rajesh, A.Yadav, A.Parihari, R.Biswas, M.Dhibar, D.P.Kaur, M.Ratna Raju, J.Joseph

Evaporation-residue-gated spin distribution measurements of the highly fissile compound nucleus ²²⁴Th^* through ¹⁶O + ²⁰⁸Pb and ¹⁸O + ²⁰⁶Pb reactions

NUCLEAR REACTIONS ²⁰⁸Pb(¹⁶O, X)²²⁴Th^*, E=87, 93.2, 99.3, 105.5, 113.5, 122.6 MeV pulsed beam; ²⁰⁶Pb(¹⁸O, X)²²⁴Th^*, E=85.7, 91.9, 100, 104.1, 108.2, 112.2, 117.4, 121.4 MeV pulsed beam; measured evaporation residues (ER), σ(E) and spin distributions of ERs from deexciting ²²⁴Th compound nucleus using the HYbrid Recoil mass Analyzer (HYRA) coupled with the TIFR 4π spin spectrometer of of 32 NaI(Tl) scintillation detectors at the IUAC-New Delhi accelerator facility; deduced experimental and simulated fold distributions, reduced ER σ(E), experimental absolute ER σ(E), including results of previous experiments.

doi: 10.1103/PhysRevC.101.014616
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6377.

2020SA25      Eur.Phys.J.Plus 135, 512 (2020)

K.P.Santhosh, J.G.Joseph

¹⁰Be-accompanied ternary fission of Cf isotopes: a level density formulation

RADIOACTIVITY ²⁵²Cf(SF); calculated fission yields. ¹⁰Be; Comparison with experimental data.

doi: 10.1140/epjp/s13360-020-00522-5
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2018SA24      Pramana 91, 5 (2018)

K.P.Santhosh, S.Krishnan, J.G.Joseph

All possible tripartitions of ²³⁶U isotope in collinear configuration

RADIOACTIVITY ²³⁶U(SF); calculated ternary fission yields using unified ternary fission model.

doi: 10.1007/s12043-018-1578-1
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2012SA05      Nucl.Phys. A877, 1 (2012)

K.P.Santhosh, J.G.Joseph, B.Priyanka

Fine structure in the α-decay of odd-even nuclei

RADIOACTIVITY ^211,213Bi, ^211,215,217At, ²²¹Fr, ^{215,221,223,225,227}Ac, ^{217,225,227,229,231}Pa, ^235,237Np, ^241,243Am, ^247,249Bk, ^{247,251,253,255}Es, ^255,257Md(α); calculated T_1/2, α-branching ratio to individual residual states using CPPMDN (Coulomb and proximity potential model for deformed nuclei). Compared with data.

doi: 10.1016/j.nuclphysa.2012.01.009
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2012SA34      Phys.Rev. C 86, 024613 (2012)

K.P.Santhosh, J.G.Joseph

Systematic studies on α-decay fine structure of odd-odd nuclei in the region 83 ≤ Z ≤ 101

RADIOACTIVITY ^210,212Bi, ^{208,210,212,214,216,218}At, ^{212,214,216,218,220}Fr, ^{214,216,222,224}Ac, ^{216,218,224,226,228}Pa, ²⁵⁴Es, ^248,256,258Md(α); calculated half-lives, branching ratios, penetrability using the Coulomb and proximity potential model for deformed nuclei (CPPMDN). Comparison with experimental data.

doi: 10.1103/PhysRevC.86.024613
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2011SA10      Nucl.Phys. A850, 34 (2011)

K.P.Santhosh, S.Sahadevan, J.G.Joseph

Alpha decay of even-even nuclei in the region 78 ≤ Z ≤ 102 to the ground state and excited states of daughter nuclei

NUCLEAR STRUCTURE Z=78-102; calculated α-decay T_1/2, branching ratios. Coulomb and proximity potential model for deformed nuclei, comparison with experimental data.

doi: 10.1016/j.nuclphysa.2010.12.002
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2011SA24      J.Phys.(London) G38, 075101 (2011)

K.P.Santhosh, J.G.Joseph, B.Priyanka, S.Sahadevan

Systematic study on the α-decay fine structure of even-odd nuclei in the range 84 ≤ Z ≤ 102

NUCLEAR STRUCTURE Z=84-102; calculated α-decay T_1/2. Coulomb and proximity potential model for deformed nuclei, comparison with experimental data.

doi: 10.1088/0954-3899/38/7/075101
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2011SA40      Phys.Rev. C 84, 024609 (2011)

K.P.Santhosh, B.Priyanka, J.G.Joseph, S.Sahadevan

α decay chains in ^271-294115 superheavy nuclei

RADIOACTIVITY ^{271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290,291,292,293,294}Mc, ^{267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290}Nh, ^{263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286}Rg, ^{259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282}Mt, ^{255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278}Bh, ^{251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274}Db, ^{247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270}Lr, ^{243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266}Md, ^{239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262}Es, ^{235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258}Bk, ^{231,232,233,234,235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254}Am, ^{227,228,229,230,231,232,233,234,235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250}Np(α), (SF); calculated half-lives, Q_α in the framework of Coulomb and proximity potential model for deformed nuclei (CPPMDN). Comparison with experimental data.

doi: 10.1103/PhysRevC.84.024609
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2010SA36      Phys.Rev. C 82, 064605 (2010)

K.P.Santhosh, J.G.Joseph, S.Sahadevan

α decay of nuclei in the range 67≤Z≤91 from the ground state and isomeric state

RADIOACTIVITY ^{151,152,153,154}Ho, ^153,154,155Tm, ^155,156,157Lu, ¹⁵⁶Hf, ^{157,158,159,160,161}Ta, ¹⁵⁸W, ^{161,162,163,164,165}Re, ^{165,166,167,169,171,174}Ir, ¹⁷²Pt, ^{170,171,173,175,176,177}Au, ^176,177,187Hg, ^{177,179,181,183,185}Tl, ^{179,180,181,183,185,187}Pb, ^{186,187,188,189,190,191,192,193,194,195,196}Bi, ^{187,188,192,193,195,197,199,201}Po, ^{191,192,193,194,195,197,198,200,202,212,214}At, ^{195,197,199,201,203}Rn, ^{201,202,203,204,206}Fr, ^{201,203,205,207}Ra, ^206,208,216Ac, ²¹⁶Th, ²¹⁷Pa(α), ²⁴⁵Md, ²⁵⁷Db, ²⁶³Sg; calculated half-lives for favored and unfavored transitions for ground states and isomers using Coulomb and proximity potential model for deformed nuclei (CPPMDN). Comparison with experimental data.

doi: 10.1103/PhysRevC.82.064605
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1978BA54      Phys.Lett. 79B, 52 (1978)

G.Bardin, J.Duclos, J.Joseph, A.Magnon, J.Martino, E.Zavattini

Total Muon Capture Rate in ⁶Li and ⁷Li

NUCLEAR REACTIONS ^6,7Li(μ^-, X), ^6,7Li(μ⁺, X); measured μ+, μ- T_1/2. ^6,7Li deduced total muon capture rates. Enriched targets.

doi: 10.1016/0370-2693(78)90433-1
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1978DE15      Nuovo Cim. 43A, 475 (1978)

P.Desgrolard, P.A.M.Guichon, J.Joseph

Muon Capture Rates for A = 6-14 Nuclei

ATOMIC PHYSICS ^6,7Li, ⁹Be, ^10,11B, ^12,13C, ¹⁴N(μ^-, X); calculated muon capture rates.

doi: 10.1007/BF02730442
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1978GU05      Z.Phys. A285, 183 (1978)

P.Guichon, M.Giffon, J.Joseph, R.Laverriere, C.Samour

Exchange Current Corrections for Partial Capture Rates of Muons in Nuclei

NUCLEAR REACTIONS ¹²C, ¹⁶O, ³²S, ⁴⁰Ca(μ^-, γ); calculated exchange current corrections for partial capture rates.

doi: 10.1007/BF01408745
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1975DU07      Phys.Rev. C12, 28 (1975)

D.Duplain, B.Goulard, J.Joseph

Multipole Excitations in Nuclear Muon Capture and Mean Nuclear Excitation Energies

NUCLEAR REACTIONS ⁴⁰Ca, ⁶⁰Ni, ⁸⁸Sr, ¹¹⁴Sn, ¹⁴⁰Ce, ²⁰⁸Pb(μ^-, X); calculated muon capture rates.

doi: 10.1103/PhysRevC.12.28
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1973GO25      Phys.Lett. 45B, 27 (1973)

B.Goulard, J.Joseph

Muonuclear Absorption

NUCLEAR STRUCTURE ⁴⁰Ca; calculated muon absorption.

doi: 10.1016/0370-2693(73)90244-X
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1973GO36      Can.J.Phys. 51, 2376 (1973)

B.Goulard, J.Joseph

The Factorization Method and the Electromagnetic Giant Dipole Resonance

NUCLEAR REACTIONS ¹⁶O, ⁴⁰Ca(γ, n), E=15-28 MeV; calculated σ(Eγ). ¹⁶O, ⁴⁰Ca calculated resonances.

doi: 10.1139/p73-310
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1973JO17      Can.J.Phys. 51, 2382 (1973)

J.Joseph, B.Goulard

Muonuclear Absorption and the Factorization Method

NUCLEAR REACTIONS ¹⁶O, ⁴⁰Ca(μ^-, n), E=1-30 MeV; calculated σ(E), μ-absorption rates.

doi: 10.1139/p73-311
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1972JO15      Phys.Rev. C6, 1742 (1972)

J.Joseph, F.Ledoyen, B.Goulard

Muon Absorption by Nuclei with N > 2

NUCLEAR REACTIONS ⁸⁸Sr(μ^-, ν), E approx 0; calculated reduced matrix elements.

doi: 10.1103/PhysRevC.6.1742
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1971GO23      Phys.Rev.Lett. 27, 1238 (1971)

B.Goulard, J.Joseph, F.Ledoyen

Isospin Splitting of the Giant Dipole Resonance, and Muon Capture

NUCLEAR STRUCTURE ^40,48Ca, ⁸⁸Sr, ¹⁴⁰Ce, ²⁰⁸Pb; analyzed isospin splitting in giant dipole resonance.

doi: 10.1103/PhysRevLett.27.1238
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1969JO23      Compt.Rend. 268B, 1039 (1969)

J.Joseph, R.Nahabetian, E.El Baz, J.Lafoucriere

Application de la Reaction (d, α) su l'Azote-14 a l'Etude du Niveau Fondamental et du Premier Niveau Excite du Carbone-12

NUCLEAR REACTIONS ¹⁴N(d, α), E not given; calculated σ(θ). ¹²C deduced ground-state configuration.

Note: The following list of authors and aliases matches the search parameter J.Joseph: , J.G.JOSEPH