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NSR database version of April 27, 2024.

Search: Author = M.Kaushik

Found 29 matches.

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2022MA13      Nucl.Phys. A1021, 122421 (2022)

I.Majeed Bhat, Mohd.S.M.S.Asnain, V.R.Sharma, A.Yadav, M.K.Sharma, P.P.Singh, D.P.Singh, U.Gupta, R.N.Sahoo, A.Sood, M.Kaushik, R.Kumar, B.P.Singh, R.Prasad

Effect of projectile structure on break-up fusion for ¹⁴N + ¹⁷⁵Lu system at intermediate energies

NUCLEAR REACTIONS ¹⁷⁵Lu(¹⁴N, X)¹⁸⁴Pt/¹⁸⁵Pt/¹⁸⁶Pt/¹⁸³Ir/¹⁸⁴Ir/¹⁸⁵Ir/¹⁸²Os/¹⁸³Os/¹⁸¹Re/¹⁷⁷W/¹⁷⁸Ta, E=87.11 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with PACE4 predictions. The Inter University Accelerator, New Delhi, India.

doi: 10.1016/j.nuclphysa.2022.122421
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6422.

2022MA25      Phys.Rev. C 105, 054607 (2022)

I.Majeed Bhat, M.Shuaib, M.S.Asnain, M.K.Sharma, A.Yadav, V.R.Sharma, P.P.Singh, D.P.Singh, S.Gupta, U.Gupta, R.N.Sahoo, A.Sood, M.Kaushik, S.Kumar, R.Kumar, B.P.Singh, R.Prasad

Role of precursor nuclei in heavy-ion induced reactions at low energies

NUCLEAR REACTIONS ¹⁷⁵Lu(¹⁴N, 4np), E=79.68, 87.11 MeV; ¹⁵⁹Tb(¹²C, 3np), E=69.15, 77.77 MeV; ¹⁵⁹Tb(¹³C, 4np), E=77.87, 84.59 MeV; measured Eγ, Iγ; deduced σ(E). Separated yields of the isotope produced in the direct reaction from feeding caused by decay of the isotopes from other channels. Pelletron accelerator facility of the Inter-University Accelerator Centre(IUAC), New Delhi. comparison to theoretical estimations.

RADIOACTIVITY ¹⁸⁴Pt(β⁺), (EC) [from ¹⁷⁵Lu(¹⁴N, 5n), E=79.68, 87.11 MeV]; ¹⁶⁷Lu(EC) [from ¹⁵⁹Tb(¹³C, 5n), E=77.87, 84.59 MeV; ¹⁵⁹Tb(¹²C, 4n), E=69.15, 77.77 MeV]; measured Eγ, Iγ; deduced T_1/2. Comparison to other experimental data.

doi: 10.1103/PhysRevC.105.054607
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6434. Data from this article have been entered in the XUNDL database. For more information, click here.

2021AS08      Phys.Rev. C 104, 034616 (2021)

M.S.Asnain, M.Shuaib, I.Majeed, M.K.Sharma, V.R.Sharma, A.Yadav, D.P.Singh, P.P.Singh, U.Gupta, R.N.Sahoo, A.Sood, M.Kaushik, S.Kumar, R.Kumar, B.P.Singh, R.Prasad

Effect of non-α-cluster projectile on incomplete-fusion dynamics: Experimental study of the ¹⁴N + ¹⁸¹Ta

NUCLEAR REACTIONS ¹⁸¹Ta(¹⁴N, 3n)¹⁹²Hg, (¹⁴N, 4n)¹⁹¹Hg/^191mHg, (¹⁴N, 5n)¹⁹⁰Hg, (¹⁴N, 6n)¹⁸⁹Hg/^189mHg, (¹⁴N, 3np)¹⁹¹Au, (¹⁴N, 4np)¹⁹⁰Au, (¹⁴N, 5np)¹⁸⁹Au/^189mAu, (¹⁴N, 2nα)¹⁸⁹Pt, (¹⁴N, 4nα)¹⁸⁷Pt, (¹⁴N, 5nα)¹⁸⁶Pt, (¹⁴N, 3npα)¹⁸⁷Ir, (¹⁴N, 4npα)¹⁸⁶Ir/^186mIr, (¹⁴N, 5npα)¹⁸⁵Ir, (¹⁴N, 4n2α)¹⁸³Os, (¹⁴N, 5np2α)¹⁸¹Re, E=65.53, 67.50, 69.47, 71.54, 73.65, 75.65, 77.08, 79.51, 81.42, 83.05, 85.17, 87.07 MeV; measured off-line Eγ, Iγ, σ(E) for radio-nuclides populated via complete fusion (CF) and/or incomplete fusion (ICF processes) by activation method at the ion-beam facility of the IUAC-New Delhi; deduced total fusion, total complete fusion, and total incomplete fusion σ(E). Comparison with statistical model calculations using PACE4 code. ¹⁹⁰Hg; measured nominal half-life from γ-decay curves as an example for the purpose of correct identification of different radioactive nuclei produced through various reaction channels.

doi: 10.1103/PhysRevC.104.034616
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6406.

2021KA37      Phys.Rev. C 104, 024615 (2021)

M.Kaushik, S.K.Pandit, V.V.Parkar, G.Gupta, S.Thakur, V.Nanal, H.Krishnamoorthy, A.Shrivastava, C.S.Palshetkar, K.Mahata, K.Ramachandran, S.Pal, R.G.Pillay, P.P.Singh

Investigating neutron transfer in the ⁹Be + ¹⁹⁷Au system

NUCLEAR REACTIONS ¹⁹⁷Au(⁹Be, ⁸Be)¹⁹⁸Au, (⁹Be, ¹⁰Be)¹⁹⁶Au, (⁹Be, X)¹⁹⁹Tl/²⁰⁰Tl/²⁰¹Bi/²⁰²Bi/²⁰³Bi, E=30-47 MeV from BARC-TIFR Pelletron Linac Facility, Mumbai; measured off-line Eγ, Iγ from the irradiated target; deduced σ(E) for one-neutron stripping and pickup reactions, complete-fusion (CF) and incomplete fusion (ICF). Comparison with coupled-reaction channel (CRC) calculations. ¹⁹⁷Au(⁶Li, ⁵Li), (⁶Li, ⁷Li), (⁷Li, ⁶Li), (⁷Li, ⁵Li), (⁶Li, X), (⁷Li, X), E(cm)=20-44 MeV; analyzed previous data for σ(E) for n-transfer, CF and ICF using CRC calculations.

doi: 10.1103/PhysRevC.104.024615
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6403.

2021KA41      Eur.Phys.J. A 57, 320 (2021)

M.Kaushik, G.Gupta, V.V.Parkar, S.K.Pandit, S.Thakur, V.Nanal, A.Shrivastava, R.G.Pillay, H.Krishnamoorthy, K.Mahata, S.Pal, C.S.Palshetkar, K.Ramachandran, P.P.Singh

Neutron transfer in ⁹Be + ¹⁵⁹Tb system

NUCLEAR REACTIONS ¹⁵⁹Tb(⁹Be, X)¹⁶⁰Tb, E=30-47 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with calculations.

doi: 10.1140/epja/s10050-021-00627-0
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6414.

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2020KA19      Phys.Rev. C 101, 034611 (2020)

M.Kaushik, G.Gupta, S.Thakur, H.Krishnamoorthy, PushpendraP.Singh, V.V.Parkar, V.Nanal, A.Shrivastava, R.G.Pillay, K.Mahata, K.Ramachandran, S.Pal, C.S.Palshetkar, S.K.Pandit

Fusion of the Borromean nucleus ⁹Be with a ¹⁹⁷Au target at near-barrier energies

NUCLEAR REACTIONS ¹⁹⁷Au(⁹Be, 3n), (⁹Be, 4n), E=33-46.7 MeV; measured Eγ, Iγ, evaporation residue σ(E) by off-beam γ counting method at the Pelletron Linac facility of BARC-TIFR. Comparison with theoretical calculations using CCFULL code, and previous experimental data for excitation functions of other weakly bound projectiles of ^4,6,8He, ^6,7Li, ^9,11Be on ¹⁹⁷Au target.

doi: 10.1103/PhysRevC.101.034611
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6383.

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
Citations: PlumX Metrics

2020SA32      Phys.Rev. C 102, 024615 (2020)

R.N.Sahoo, M.Kaushik, A.Sood, A.Sharma, S.Thakur, Pa.Kumar, M.M.Shaikh, R.Biswas, A.Yadav, M.K.Sharma, J.Gehlot, S.Nath, N.Madhavan, R.G.Pillay, E.M.Kozulin, G.N.Knyazheva, K.V.Novikov, P.P.Singh

Role of neutron transfer in sub-barrier fusion

NUCLEAR REACTIONS ¹³⁰Te(³⁵Cl, X), E(cm)=94.0, 95.6, 97.2, 98.8, 100.3, 101.9, 103.5, 105.0 MeV; measured evaporation residues (ERs), ΔE-time spectra, fusion σ(E) using recoil mass separator HIRA at IUAC-New Delhi accelerator facility. Comparison with experimental fusion σ(E) data for ¹³⁰Te(³⁷Cl, X), and other systems. Coupled-channels analysis using CCFULL code.

doi: 10.1103/PhysRevC.102.024615
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6389.

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
Citations: PlumX Metrics

2019AG14      Int.J.Mod.Phys. E28, 1950099 (2019)

M.Aggarwal, M.Kaushik, G.Saxena

High spin states of Zr isotopes around A=80 mass region- study on cold and hot rotating nuclei

NUCLEAR STRUCTURE ^{76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124}Zr; calculated ground state quadrupole deformation, parameters, high-spin states, proton and neutron pairing gaps, moments of inertia.

doi: 10.1142/S021830131950099X
Citations: PlumX Metrics

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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2019SA15      Nucl.Phys. A983, 145 (2019)

R.N.Sahoo, M.Kaushik, A.Sood, P.Kumar, V.R.Sharma, A.Yadav, P.P.Singh, M.K.Sharma, R.Kumar, B.P.Singh, S.Aydin, R.Prasad

Insights into the low energy incomplete fusion

NUCLEAR REACTIONS ¹⁶⁹Tm(¹²C, x), E(cm)=52.98 - 89.25 MeV; measured Eγ, Iγ(t); deduced production σ of evaporation residues. ¹⁶⁹Tm(¹²C, x), E=52.98 - 89.25 MeV;¹⁶⁰Gd(¹²C, x), Ei(cm)=83.7 MeV;¹⁰³Rh(¹⁶O, x), ¹⁵⁹Tb(¹⁶O, x), E not given; calculated ER production σ using PACE4 and with different level density parameters and using CCFULL; deduced potential parameters, radius parameter from the fit to the data, variation of incomplete fusion fraction with neutron skin thickness and with angular momentum.

doi: 10.1016/j.nuclphysa.2018.12.013
Citations: PlumX Metrics

2019SA17      Phys.Rev. C 99, 024607 (2019)

R.N.Sahoo, M.Kaushik, A.Sood, P.Kumar, A.Sharma, S.Thakur, P.P.Singh, P.K.Raina, M.M.Shaikh, R.Biswas, A.Yadav, J.Gehlot, S.Nath, N.Madhavan, V.Srivastava, M.K.Sharma, B.P.Singh, R.Prasad, A.Rani, A.Banerjee, U.Gupta, N.K.Deb, B.J.Roy

Sub-barrier fusion in the ³⁷Cl + ¹³⁰Te system

NUCLEAR REACTIONS ¹³⁰Te(³⁷Cl, X), E=121-155 MeV; measured reaction products, evaporation residues, time of flight of evaporation residue, fusion σ(E) using the HIRA recoil mass spectrometer at the 15UD Pelletron accelerator of IUAC-New Delhi; deduced fusion barrier distributions, astrophysical S factor, logarithmic derivative L(E) factor. Comparison with coupled-channels code calculations using CCFULL code. Systematics of reduced fusion excitation functions of ³⁷Cl projectiles on ^58,60,62,64Ni, ¹³⁰Te targets at sub-barrier energies.

doi: 10.1103/PhysRevC.99.024607
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6360.

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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2018SA38      Acta Phys.Pol. B49, 585 (2018)

R.N.Sahoo, M.Kaushik, A.Sood, P.Kumar, V.R.Sharma, A.Yadav, M.Shuaib, D.P.Singh, P.P.Singh, U.Gupta, M.K.Sharma, R.Kumar, B.P.Singh, S.Aydin, H.J.Wollersheim, R.Prasad

Entrance Channel Effect on Incomplete Fusion

NUCLEAR REACTIONS ¹⁶⁹Tm(¹²C, x), E=5-7.5 MeV/nucleon; measured evaporation residues (ER) Eγ, Iγ(time); deduced ¹⁷⁷Re σ_ER; calculated σ_ER using statistical model code PACE-IV with different level density parameter; calculated total (summed over all ERs) σ_T, complete and incomplete fusion σ_CF, σ_ICF. ¹⁰³Rh, ¹¹⁵In, ¹⁵⁹Tb, ¹⁶⁹Tm, ¹⁹⁷Au(¹²C, x), E not given;¹⁰³Rh, ¹⁵⁹Tb, ¹⁶⁹Tm(¹⁶O, x), E not given; measured reaction products Eγ, Iγ; deduced incomplete fusion fraction vs mass asymmetry (relative projectile-target velocity close to 0.05c vs asymmetry).

doi: 10.5506/aphyspolb.49.585
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6326.

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
Citations: PlumX Metrics

2017SA09      Acta Phys.Pol. B48, 309 (2017)

G.Saxena, M.Kaushik

Study of N = 16 Shell Closure Within RMF+BCS Approach

NUCLEAR STRUCTURE ²²C, ²⁴O, ²⁶Ne, ²⁸Mg, ³⁰Si, ³²S, ³⁴Ar, ³⁶Ca; calculated low-lying sp levels, J, π for N=16 isotones vs Z using RMF+BCS approach; deduced shell gap development. ^{10,12,14,16,18,20,22,24}C, ^{12,14,16,18,20,22,24,26}O; calculated pairing energy, two neutron shell gap using BCS+RMF(TMA) approach.

doi: 10.5506/APhysPolB.48.309
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2017SA33      Phys.Atomic Nuclei 80, 211 (2017)

G.Saxena, M.Kaushik

Ground-state properties of neutron magic nuclei

doi: 10.1134/s1063778817020259
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2017SA46      Chin.J.Phys.(Taiwan) 55, 1149 (2017)

G.Saxena, M.Kaushik

Behaviour of the pf shell under the RMF+BCS description

NUCLEAR STRUCTURE ^52,60Ca, ⁴⁸Si, ^84,116Se; calculated two neutron shell gaps, neutron single particle states, occupancy, quadrupole deformation parameters; deduced magicity. RMF+BCS approach.

doi: 10.1016/j.cjph.2017.03.022
Citations: PlumX Metrics

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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2015KA35      Phys.Part. and Nucl.Lett. 24, 516 (2015)

M.Kaushik, G.Saxena

High-spin structure of ⁸⁰Kr

NUCLEAR STRUCTURE ⁸⁰Kr; calculated energy levels, J, π, high-spin states, deformation parameters; deduced prolate deformation. Fully self-consistent cranked HFB approach.

doi: 10.1134/S1547477115040184
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2014SA13      Rom.J.Phys. 59, 86 (2014)

G.Saxena, D.Singh, M.Kaushik

Weakly Bound Neutron Rich C Isotopes within RMF+BCS Approach

NUCLEAR STRUCTURE ^{10,12,14,16,18,20,22}C; calculated neutron single-particle energies, occupancy, neutron density, RMF potential energy sum, binding and two-neutron separation energies, neutron radii. Relativistic Mean Field calculations, comparison with available data.

2013SA34      Phys.Part. and Nucl.Lett. 10, 220 (2013)

G.Saxena, D.Singh, M.Kaushik

Magicity in Exotic Nuclei

NUCLEAR STRUCTURE ^{34,36,38,40,42,44,46,48,50,52,54,56,58,60,62,64,66}Ca; calculated proton and neutron density distributions, two-neutron separation and neutron single-particle energies. Relativistic mean field (RMF) plus state-dependent BCS approach.

doi: 10.1134/S1547477113030114
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2004YA23      Int.J.Mod.Phys. E13, 647 (2004)

H.L.Yadav, M.Kaushik, H.Toki

Description of drip-line nuclei within the relativistic mean field plus BCS approach

NUCLEAR STRUCTURE ²⁰O, ⁶²Ca, ⁸⁴Ni, ¹³⁸Zr, ¹⁵⁰Sn, ²⁵⁰Pb; calculated neutron single-particle energies, configurations. O, Ca, Ni, Zr, Sn, Pb; calculated pairing energies, two-neutron separation energies, density distributions, radii. Relativistic mean field plus BCS approach.

doi: 10.1142/S0218301304002375
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2003AN34      Pramana 60, 1171 (2003)

A.Ansari, H.L.Yadav, M.Kaushik, U.R.Jakhar

High-spin structure of neutron-rich Dy Isotopes

NUCLEAR STRUCTURE ^{164,166,168,170}Dy; calculated high-spin level energies, g-factors, rotational band features. Cranked Hartree-Fock-Bogoliubov approach.

doi: 10.1007/BF02704284
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2002YA17      Part. and Nucl., Lett. 112, 66 (2002)

H.L.Yadav, M.Kaushik, I.R.Jakhar, A.Ansari

g Factors as a Probe for High-Spin Structure of Neutron-Rich Dy Isotopes

NUCLEAR STRUCTURE ^{164,166,168,170}Dy; calculated rotational bands deformation parameters, pair gaps, related features. ^{160,162,164,166,168,170}Dy; calculated rotational bands g factors vs angular momentum. Cranked mean-field approach, comparison with data.