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NSR database version of April 27, 2024.

Search: Author = S.Jain

Found 41 matches.

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2023JA02      Nucl.Phys. A1031, 122597 (2023)

A.Jain, P.K.Sharma, S.K.Jain, J.K.Deegwal, G.Saxena

Cluster radioactivity in trans-lead region: A systematic study with modified empirical formulas

RADIOACTIVITY ²²¹Fr, ^221,222,223Ra, ²²³Ac(¹⁴C), ²²³Ac(¹⁵N), ²²⁴Ra, ²²⁵Ac, ²²⁶Ra, ²²⁶Th(¹⁴C), ²²⁸Th(²⁰O), ²³⁰Th(²⁴Ne), ²³⁰U(²²Ne), ²³¹Pa(²⁴Ne), ²³²Th(²⁴Ne), (²⁶Ne), ²³²U(²⁴Ne), (²⁸Mg), ²³³U(²⁴Ne), (²⁵Ne), (²⁸Mg), ²³⁴U(²⁴Ne), (²⁶Ne), (²⁸Mg), ²³⁵U(²⁴Ne), (²⁵Ne), (²⁸Mg), (²⁹Mg), ²³⁶U(²⁴Ne), (²⁶Ne), (²⁸Mg), (³⁰Mg), ²³⁶Pu(²⁸Mg), ²³⁷Np(³⁰Mg), ²³⁸Pu(²⁸Mg), (³⁰Mg), (³²Si), ²⁴⁰Pu, ²⁴¹Am, ²⁴²Cm(³⁴Si), ²¹⁶Rn(⁸Be), ²²²Fr(¹⁴B), ²²¹Ra(¹³C), ²²³Ra(¹⁵C), ²²²Ac(¹⁴N), (¹⁵N), (¹⁶N), (¹⁷N), ²²⁴Th(¹⁶O), ²²⁵Th(¹⁷O), ²²⁶Th(¹⁸O), ²²⁷Th(¹⁹O), ²²⁸Th(²⁰O), ²²⁹Th(²¹O), ²³⁰Th(²²O), ²³¹Th(²³O), ²²⁸Pa(²⁰F), ²²⁹Pa(²¹F), ²³¹Pa(²³F), ²³¹U(²³Ne), (²⁵Ne); calculated T_1/2. Comparison with available data.

doi: 10.1016/j.nuclphysa.2022.122597
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2023SH10      Eur.Phys.J. A 59, 71 (2023)

H.Sharma, S.Jain, Amritpal, R.Kumar, M.K.Sharma

Fusion dynamics of spherical and deformed projectiles with hexadecapole deformed target nuclei

NUCLEAR STRUCTURE ^{147,148,149,150}Sm, ^152,154Sm, ^{172,174,176,178,180,182}Yb, ⁴⁰Sc, ⁴³Sc, ⁵⁵Sc, ⁷⁷Sc, ⁸²Sc, ⁷⁰Ge, ^72,73,74Ge, ¹⁶O, ⁴⁸Ca, ⁴⁸Ar, ⁶²Fe; analyzed available data; deduced quadrupole and hexadecapole deformation of target nuclei impact on fusion dynamics.

doi: 10.1140/epja/s10050-023-00981-1
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2023SH25      Phys.Rev. C 108, 044613 (2023)

H.Sharma, S.Jain, R.Kumar, M.K.Sharma

Optimum orientation of compact and elongated hexadecapole deformed actinide targets: Application to synthesizing superheavy nuclei

doi: 10.1103/PhysRevC.108.044613
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2022JA03      Chin.Phys.C 46, 014102 (2022)

S.Jain, M.K.Sharma, R.Kumar

Fusion of spherical-octupole pairs of colliding nuclei for compact and elongated configurations

NUCLEAR REACTIONS ¹⁴⁴Ba, ²⁸⁰Ra(¹⁶O, X), ^145,146,148Nd, ^149,150Sm(¹⁶O, X), (⁴⁸Ca, X), E not given; analyzed available data; calculated fusion σ using the Wong formula, transmission probability.

doi: 10.1088/1674-1137/ac2ed2
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2022JA07      Phys.Rev. C 105, 034605 (2022)

S.Jain, R.Kumar, S.K.Patra, M.K.Sharma

Investigation of octupole deformed fragments decaying from even-even isotopes of ^222-230Th

NUCLEAR REACTIONS ²⁰⁸Pb(¹⁶O, X)²²⁴Th^*, E^*=22.65-25.29 MeV; ²⁰⁸Pb(¹⁴O, X)²²²Th^*, (¹⁸O, X)²²⁶Th^*, (²⁰O, X)²²⁸Th^*, (²²O, X)²³⁰Th^*, E^*=24.37 MeV; calculated fragmentation potentials and preformation probabilities as functions of mass and charge distributions, fission σ(E) using dynamical cluster-decay model (DCM), with collective clusterization approach of quantum mechanical fragmentation theory, including quadrupole (β₂) and octupole (β₃) deformations of fission fragments. Comparison with available experimental data.

doi: 10.1103/PhysRevC.105.034605
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2022PA23      Phys.Scr. 97, 045303 (2022)

D.Pathak, N.Singh, P.Singh, P.Kaur, H.Kaur, S.R.Jain

Probable decay modes of even-even superheavy nuclei

RADIOACTIVITY ^222,224,226Ra(¹⁴C), ²²⁸Th(²⁰O), ^230,232Th(²⁴Ne), ²³²Th(²⁶Ne), ²³²U(²⁴Ne), (²⁸Mg), ²³⁴U(²⁴Ne), (²⁸Mg), (²⁶Ne), ²³⁶U(²⁴Ne), (²⁸Mg), (²⁶Ne), (³⁰Mg), ^236,238Pu(²⁸Mg), ²³⁸Pu(³⁰Mg), (³²Si), ²⁴⁰Pu, ²⁴²Cm(³⁴Si); calculated T_1/2. Comparison with available data.

NUCLEAR STRUCTURE ^{298,300,302,304,306,308,310,312}Og, ^{296,298,300,302,304,306,308,310}120; calculated heavy cluster decay T_1/2.

doi: 10.1088/1402-4896/ac5a8c
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2022SH29      Phys.Scr. 97, 045307 (2022)

R.Sharma, A.Jain, P.K.Sharma, S.K.Jain, G.Saxena

A comprehensive study of decay modes associated with Pb isotopes

RADIOACTIVITY ^{176,177,178,179,180,181,182,183,184,185,186,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,205}Pb(β⁺), (EC), ^{209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266}Pb(β^-), ^{178,179,180,181,182,183,184,185,186,187,188,189,190,191,192,193}Pb(α); calculated T_1/2. Comparison with available data.

doi: 10.1088/1402-4896/ac607c
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2021JA09      Hyperfine Interactions 242, 60 (2021)

A.Jain, R.Sharma, S.K.Jain, P.K.Sharma, G.Saxena

Cluster radioactivity in ^{294, 296}Og

RADIOACTIVITY ^294,296Og(α), (⁸Be), (¹²C), (¹⁴C), (¹⁶O), (¹⁸O), (²⁰O), (²²Ne), (²⁴Ne), (²⁶Mg), (²⁸Mg), (³⁰Si), (³²Si), (³⁴Si), (³⁶S), (³⁸S), (⁴⁰Ar), (⁴²Ar), (⁴⁴Ar), (⁴⁶Ca), (⁴⁸Ca), (⁵⁰Ca), (⁵²Ti), (⁵⁴Ti), (⁵⁶Cr), (⁵⁸Cr), (⁶⁰Cr), (⁶²Fe), (⁶⁴Fe), (⁶⁶Ni), (⁶⁸Ni), (⁷⁰Ni), (⁷²Zn), (⁷⁴Ge), (⁷⁶Zn), (⁷⁸Ge), (⁸⁰Ge), (⁸²Ge), (⁸⁴Se), (⁸⁶Kr), (⁸⁸Kr), (⁹⁰Sr), (⁹²Kr), (⁹⁴Sr), (⁹⁶Zr), (⁹⁸Zr), (¹⁰⁰Mo), (¹⁰²Mo); calculated T_1/2. Comparison with available data.

doi: 10.1007/s10751-021-01748-0
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2021PA24      J.Phys.(London) G48, 075103 (2021)

D.Pathak, N.Singh, H.Kaur, S.R.Jain

Prediction of half-lives of even-even superheavy nuclei

RADIOACTIVITY ²¹⁰Pb, ^214,216,218Po, ^220,222Rn, ^222,224,226Ra, ^{226,228,230,232}Th, ^{232,234,236,238}U, ^{232,234,236,238,240}Pu, ^{236,238,240,242,244,246,248,250}Cm, ²³⁸Cf, ^{242,244,246,248,250,252,254,256}Cf, ²⁴⁴Fm, ²⁴⁸Fm, ^252,254,256Fm, ^256,258No, ^{256,257,258,259}Rf, ²⁶¹Rf, ^259,260,261Sg, ²⁶³Sg, ^{264,265,266,267,268}Hs, ²⁷⁰Hs, ^269,270,271Ds, ²⁷³Ds, ²⁷⁷Cn, ^283,284,285Cn, ^{285,286,287,288,289}Fl, ^290,291,292Lv, ^291,292,293Og, ^257,259Db, ²⁵⁶Db, ²⁷⁰Db, ²⁶¹Bh, ²⁶⁵Bh, ^283,285Nh, ^287,289Mc, ²⁶⁰Bh, ²⁶⁶Bh, ²⁶⁶Mt, ^288,290Mc, ²⁹⁴Ts(α); calculated T_1/2. Comparison with available data.

doi: 10.1088/1361-6471/abe281
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2021SH29      Int.J.Mod.Phys. E30, 2150070 (2021)

R.Sharma, A.Jain, M.Kaushik, S.K.Jain, G.Saxena

Structural properties of nuclei with semi-magic number N(Z)=40

NUCLEAR STRUCTURE ⁵⁶S, ⁵⁸Ar, ⁶⁰Ca, ⁶²Ti, ⁶⁴Cr, ⁶⁶Fe, ⁶⁸Ni, ⁷⁰Zn, ⁷²Ge, ⁷⁴Se, ⁷⁶Kr, ⁷⁸Sr, ⁸⁰Zr, ⁸²Mo, ⁸⁴Ru, ⁸⁶Pd, ^{78,80,82,84,86,88,90,92,94,96,98,100,102,104,106,108,110,112,114,116,118,120,122,124}Zr; calculated binding energies, deformation parameters.

doi: 10.1142/S0218301321500701
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2021SH43      Hyperfine Interactions 242, 35 (2021)

R.Sharma, A.Jain, S.K.Jain, G.Saxena

Magicity in the nuclei with N = 32 and 34

NUCLEAR STRUCTURE ^46,48Si, ^48,50S, ^50,52Ar, ^52,54Ca, ^54,56Ti, ^56,58Cr, ^58,60Fe, ^60,62Ni, ^62,64Zn, ^64,66Ge, ^66,68Se, ^68,70Kr; analyzed available data; calculated potential energy surfaces, quadrupole deformation parameters, two proton shell gap, isotopic shift using relativistic mean-field (RMF) approach with density-dependent meson-nucleon couplings using DD-ME2 parameter.

doi: 10.1007/s10751-021-01751-5
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2021SI02      Nucl.Phys. A1006, 122066 (2021)

U.K.Singh, R.Sharma, P.K.Sharma, M.Kaushik, S.K.Jain, G.Saxena

Structural properties and α-decay chains of transfermium nuclei (101 ≤ Z ≤ 110)

RADIOACTIVITY ^{235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287}Md, ^{238,239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288}No, ^{241,242,243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289}Lr, ^{243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290}Rf, ^{245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290,291}Db, ^{248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290,291,292}Sg, ^{250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290,291,292,293}Bh, ^{253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290,291,292,293,294}Hs, ^{255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290,291,292,293,294,295}Mt, ^{255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290,291,292,293,294,295,296}Ds(α), (SF); calculated potential energy surfaces (PESs), occupancies of neutron single particle states, rms α-decay T_1/2, T_1/2. Comparison with available data.

doi: 10.1016/j.nuclphysa.2020.122066
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2020DW01      Eur.Phys.J. Special Topics 229, 2619 (2020)

N.Dwivedi, B.Agarwal, S.R.Jain

Spectral statistics of energy levels of ¹⁵²Dy

NUCLEAR STRUCTURE ¹⁵²Dy; calculated quadrupole deformations for neutrons and protons, octupole deformed configurations, the nearest-neighbor level spacing distributions. Comparison with available data.

doi: 10.1140/epjst/e2020-000151-y
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2020JA04      Nucl.Phys. A997, 121699 (2020)

S.Jain, M.K.Sharma, R.Kumar

Analysis of the barrier characteristics and related fusion properties using 2pF, 3pF and 3pG density functions

doi: 10.1016/j.nuclphysa.2020.121699
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2020JA07      Phys.Rev. C 101, 051601 (2020)

S.Jain, M.K.Sharma, R.Kumar

Optimum orientations for octupole deformed nuclei in fusion configurations

NUCLEAR REACTIONS ^110,111,148La, ^{224,226,232,274,276,280}Rn, ^276,278,280Ac(⁴⁸Ca, X), E(cm)=182.06-226.06 MeV; calculated fusion barrier, interaction radii of oriented octupole deformed target nuclei as function of soft or rigid-pear shaped deformation of colliding partners, and fusion σ(E) of ¹⁴²La, ²²⁰Rn(⁴⁸Ca, X)¹⁹⁰Ir^*/²⁶⁸Sg^* systems using Wong formula; deduced optimum orientations of participating nuclei as function of positive and negative signs of octupole deformation parameter β₃. Relevance to synthesis and subsequent decays of heavy and superheavy nuclei.

doi: 10.1103/PhysRevC.101.051601
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2020KU26      Int.J.Mod.Phys. E29, 2050068 (2020)

M.Kumawat, G.Saxena, M.Kaushik, S.K.Jain, J.K.Deegwal, M.Aggarwal

Novel feature of doubly bubble nuclei in 50 ≤ Z(N) ≤ 82 region along with magicity and weakly bound structure

NUCLEAR STRUCTURE Z=50-82; calculated the separation energies, s.p. energies, pairing energies, proton and neutron density profiles along with deformations of even-even nuclei using the Relativistic Mean-Field (RMF) approach; deduced central density depletion in both proton and neutron named as doubly bubble nuclei.

doi: 10.1142/S0218301320500688
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2020MO38      Int.J.Mod.Phys. E29, 2050071 (2020)

S.Monga, H.Kaur, S.R.Jain

Analysis of pairing phase transition in Sn-isotopes within semiclassical approach

NUCLEAR STRUCTURE ^{102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138}Sn; calculated pairing gaps and strengths, critical temperatures, shell structure energy.

doi: 10.1142/S0218301320500718
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2020PR13      Phys.Rev. C 102, 054605 (2020)

G.K.Prajapati, Y.K.Gupta, B.V.John, B.N.Joshi, H.Kaur, N.Kumar, L.S.Danu, S.Mukhopadhyay, S.Dubey, S.R.Jain, D.C.Biswas, B.K.Nayak

Temperature and isospin dependence of the level-density parameter in the A ≈ 110 mass region

NUCLEAR REACTIONS ⁹⁴Mo(¹⁶O, X)¹¹⁰Sn^*, E=55, 60, 70, 75, 80 MeV; ¹⁰⁰Mo(¹⁶O, X)¹¹⁶Sn^*, E=55, 60, 70, 75, 80, 95.5, 104.9, 114.6, 124.6, 136.6 MeV; measured reaction products, Eα, Iα, angular distributions using CsI(Tl) detectors in a Charge Particle Detector Array at the BARC-TIFR Pelletron Linac Accelerator facility; deduced double-differential σ(Eα), averaged α-particle energy spectra, inverse level-density parameter for Cd nuclei as a function of temperature and isospin. Statistical model analysis of experimental data using PACE2 code.

doi: 10.1103/PhysRevC.102.054605
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2020SI27      Nucl.Phys. A1004, 122035 (2020)

U.K.Singh, P.K.Sharma, M.Kaushik, S.K.Jain, D.T.Akrawy, G.Saxena

Study of decay modes in transfermium isotopes

RADIOACTIVITY ^{245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260}Md, ^{250,251,252,253,254,255,256,257,258,259,260,261,262}No, ^{252,253,254,255,256,257,258,259,260,261,262,263,264,265,266}Lr, ^{253,254,255,256,257,258,259,260,261,262,263,264,265}Rf, ^{255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270}Db, ^{258,259,260,261,262,263,264,265,266,267,268,269,270,271}Sg, ^{260,261,262,263,264,265,266,267,268,269,270,271,272,273,274}Bh, ^{263,264,265,266,267,268,269,270,271,272,273,274,275,276,277}Hs, ^{266,267,268,269,270,271,272,273,274,275,276,277,278}Mt(EC), (β^-), (α), (SF); calculated T_1/2. Comparison with available data.

doi: 10.1016/j.nuclphysa.2020.122035
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2019DW01      Int.J.Mod.Phys. E28, 1950061 (2019)

N.R.Dwivedi, S.Monga, H.Kaur, S.R.Jain

Ignatyuk damping factor: A semiclassical formula

NUCLEAR STRUCTURE ^48,58Ni, ^112,114,116Sn, ^{182,204,206,208,210}Pb; analyzed nuclear-level densities extracted from transmission data or gamma energy spectrum store the basic statistical information about nuclei at various temperatures.

doi: 10.1142/S0218301319500617
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2019SA02      Phys.Lett. B 788, 1 (2019)

G.Saxena, M.Kumawat, M.Kaushik, S.K.Jain, M.Aggarwal

Bubble structure in magic nuclei

NUCLEAR STRUCTURE ^{12,13,14,15,16,17,18,19,20,21,22,23,24}O, ^{34,35,36,37,38,39,40,41,42,43,44,45,46,47,48,49,50,51,52,53,54,55,56,57,58,59,60,61,62,63,64,65,66,67,68,69,70}Ca, ^{48,49,50,51,52,53,54,55,56,57,58,59,60,61,62,63,64,65,66,67,68,69,70,71,72,73,74,75,76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98}Ni, ^{80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150}Zr, ^{78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126}Sn, ^{178,179,180,181,182,183,184,185,186,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262}Pb, ²⁵¹Fr, ²⁹⁹Mc, ³⁰²Og, ²²Si, ³⁴Si, ⁴⁶Ar, ⁵⁶S, ⁵⁸Ar, ¹⁸⁴Ce, ³⁴⁷119, ²⁹²120, ³⁴¹Nh; calculated charge and matter densities, single particle levels and depletion fraction (DF) across the periodic chart; deduced that the central depletion is correlated to shell structure and occurs due to unoccupancy in s-orbit (2s, 3s, 4s) and inversion of (2s, 1d) and (3s, 1h) states in nuclei upto Z less or equal to 82. Bubble effect in superheavy region is a signature of the interplay between the Coulomb and nn-interaction where the depletion fraction is found to increase with Z (Coulomb repulsion) and decrease with isospin.

doi: 10.1016/j.physletb.2018.08.076
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2018DW01      Eur.Phys.J. A 54, 49 (2018)

N.R.Dwivedi, H.Kaur, S.R.Jain

Semiclassical triton

NUCLEAR STRUCTURE ³H; calculated binding-type potential energy surface and the scattering one vs radius using Feshbach-Pease potentials; deduced their intersection, ³H gs wave function components for S- and D-states, binding energy, Q.

doi: 10.1140/epja/i2018-12480-y
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2018JA18      Eur.Phys.J. A 54, 203 (2018)

S.Jain, R.Kumar, M.K.Sharma

Effect of different nuclear density approximations on fusion dynamics within Skyrme Energy Density Formalism

NUCLEAR REACTIONS ⁵⁸Ni(⁵⁸Ni, γ)¹¹⁶Ba^*, E(cm)=93.45-108.9 MeV; calculated density distribution, potentials for different density approaches, fusion σ, maximal orbital momentum. ⁵⁸Ni(¹⁸O, x), (¹⁸O, γ), (⁴⁰Ca, x), (⁴⁰Ca, γ), (⁵⁸Ni, x), (⁵⁸Ni, γ)(¹³²Sn, x), (¹³²Sn, γ), E not given; calculated fusion σ, reduced fusion σ; compared with data; deduced UFF (Universal Fusion Function).

doi: 10.1140/epja/i2018-12625-0
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2018KU17      Can.J.Phys. 96, 1413 (2018)

M.Kumawat, G.Saxena, M.Kaushik, R.Sharma, S.K.Jain

Description of nuclei with magic number Z (N) = 6

NUCLEAR STRUCTURE Z=6, N=6; calculated ground state properties of entire chains of isotopes (isotones) with Z (N) = 6 including even and odd mass nuclei using relativistic mean-field plus BCS, including quadrupole deformation, binding energy, separation energy, single particle energy, root mean squared radii, along with charge and neutron density profile. Comparison with available data.

doi: 10.1139/cjp-2017-1013
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2018SA44      Int.J.Mod.Phys. E27, 1850074 (2018)

G.Saxena, U.K.Singh, M.Kumawat, M.Kaushik, S.K.Jain, M.Aggarwal

Distinct ground state features and the decay chains of Z=121 superheavy nuclei

NUCLEAR STRUCTURE Z=121; calculated separation energies, shell corrections, deformation parameters, radial variation of charge density and neutron density using RMF+BCS approach.

RADIOACTIVITY ^{293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312}121(α); calculated Q-values, T_1/2. Comparison with available data.

doi: 10.1142/S021830131850074X
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2017SA69      Int.J.Mod.Phys. E26, 1750072 (2017)

G.Saxena, M.Kumawat, M.Kaushik, U.K.Singh, S.K.Jain, S.Somorendro Singh, M.Aggarwal

Implications of occupancy of 2_s1/2 state in sd-shell within RMF+BCS approach

NUCLEAR STRUCTURE ²²C, ^22,24O, ^34,36Ca, ²⁶S, ³⁶S, ⁵⁶S, ^22,34,48Si; calculated quadrupole deformation parameters, neutron single particle states, neutron density. Comparison with available data.

doi: 10.1142/S0218301317500720
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2017SA70      Phys.Lett. B 775, 126 (2017)

G.Saxena, M.Kumawat, M.Kaushik, S.K.Jain, M.Aggarwal

Two-proton radioactivity with 2p halo in light mass nuclei A = 18-34

NUCLEAR STRUCTURE ¹⁹Mg, ²²Si, ²⁶S, ³⁰Ar, ³⁴Ca; calculated variation of charge density, charge radii, RMF potential energy, centrifugal barrier energy for proton resonant states; deduced 2-proton halo.

doi: 10.1016/j.physletb.2017.10.055
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2008JA11      Pramana 71, 1271 (2008)

S.R.Jain, A.K.Jain, S.Kailas

Electric dipolarizability of ⁷Li

doi: 10.1007/s12043-008-0181-2
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2008PA26      Phys.Rev. C 78, 021601 (2008)

V.V.Parkar, V.Jha, B.J.Roy, S.Santra, K.Ramachandran, A.Shrivastava, A.Chatterjee, S.R.Jain, A.K.Jain, S.Kailas

Dipole polarizability of ⁷Li from precision measurement of the elastic scattering on ²⁰⁸Pb below the Coulomb barrier

NUCLEAR REACTIONS ²⁰⁸Pb(⁷Li, ⁷Li), E=18-28 MeV; measured reaction product spectra, scattering σ; ⁷Li; deduced dipole polarizability. Comparison with continuum discretized coupled channel calculations.

doi: 10.1103/PhysRevC.78.021601
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6073.

2004JA01      J.Phys.(London) G30, 157 (2004)

S.R.Jain

Semiclassical deuteron

NUCLEAR STRUCTURE ²H; calculated ground-state configuration, related features. Semiclassical approach.

doi: 10.1088/0954-3899/30/2/013
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2004JA13      Pramana 62, 561 (2004)

S.Jain, for the D0 Collaboration

Search for narrow-width t(t-bar) resonances in p(p-bar) collisions at √ s = 1.8 TeV

NUCLEAR REACTIONS ¹H(p-bar, X), E(cm)=1.8 TeV; measured t(t-bar) resonance production σ upper limit.

doi: 10.1007/BF02705318
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2004KE01      Nucl.Phys. A730, 121 (2004)

N.G.Kelkar, M.Nowakowski, K.P.Khemchandani, S.R.Jain

Time delay plots unflavoured baryons

doi: 10.1016/j.nuclphysa.2003.10.018
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2002MA58      Int.J.Mod.Phys. E11, 303 (2002)

S.S.Malik, A.K.Jain, S.R.Jain

Eigenvalue Spectrum for a Single Particle in a Spheroidal Cavity: A semiclassical approach

doi: 10.1142/S0218301302000867
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2001JA19      Pramana 57, 571 (2001)

S.R.Jain

Quantum Chaos, Thermalization and Dissipation in Nuclear Systems

doi: 10.1007/s12043-001-0063-3
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2001RA43      Pramana 57, 263 (2001)

R.Ramanna, S.R.Jain

An Empirical Approach to the Theory of Particle and Nuclear Phenomena: Review and some new ideas

doi: 10.1007/s12043-001-0037-5
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2000JA06      Nucl.Phys. A673, 423 (2000)

S.R.Jain

Dissipation in Finite Fermi Systems

doi: 10.1016/S0375-9474(00)00151-2
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2000JA09      Phys.Rev. D62, 095003 (2000)

S.Jain, A.K.Gupta, N.K.Mondal

Search for Quark-Lepton Compositeness at Fermilab Tevatron and CERN LHC

NUCLEAR REACTIONS ¹H(p-bar, X), (p, X), E=high; calculated dilepton invariant mass spectra. Implications for quark and lepton compositeness measurement discussed.

doi: 10.1103/PhysRevD.62.095003
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1996JA05      Phys.Lett. 370B, 1 (1996)

S.R.Jain, A.K.Jain, Z.Ahmed

Nonlinear Dynamics of High-j Cranking Model: A semi-classical approach

doi: 10.1016/0370-2693(95)01560-4
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1978GA16      Phys.Rev. C18, 1141 (1978)

J.B.Garg, S.Jain, J.A.Harvey

Neutron Total Cross Section and Resonance Parameters of ⁵⁸Fe

NUCLEAR REACTIONS ⁵⁸Fe(n, n), E=0.03-500 keV; measured total σ(E). ⁵⁹Fe deduced neutron resonance parameters.

doi: 10.1103/PhysRevC.18.1141
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset10753.

1970JA01      Can.J.Phys. 48, 7 (1970)

S.C.Jain

Binding Energy of the Alpha Particle with Tensor Forces and a Velocity-Dependent Potential

NUCLEAR STRUCTURE ⁴He; calculated binding energy, rms radius. Velocity-dependent potential, Irving wave function.

doi: 10.1139/p70-002
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1969JA07      Phys.Rev. 184, 1226 (1969)

S.C.Jain

Photoproduction of Positive Pions from ³He

NUCLEAR REACTIONS ³He(γ, π⁺), E = 182-252 MeV; calculated Q, σ(E;Q).

doi: 10.1103/PhysRev.184.1226
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Note: The following list of authors and aliases matches the search parameter S.Jain: , S.C.JAIN, S.K.JAIN, S.R.JAIN