NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = H.M.Mittal Found 26 matches. 2020KA60 Int.J.Mod.Phys. E29, 2050081 (2020) M.Karday, A.Dadwal, H.M.Mittal Examination of phenomenological formulae in superdeformed bands of A ∼ 190, 150 mass regions NUCLEAR STRUCTURE 194Hg, 193Tl, 192,194,196Pb, 152Dy; analyzed available data; calculated band-head spins for super deformed bands, rms deviations using rotational energy formulae.
doi: 10.1142/S0218301320500810
2020KA67 Phys.Scr. 95, 105303 (2020) M.Karday, A.Dadwal, H.M.Mittal Systematic study of superdeformed rotational bands in Hg isotopes NUCLEAR STRUCTURE 189,190,191,192,193,194,195Hg; analyzed available data; deduced band-head spin and the parameters, SD bands, γ-transition energies using a least-squares fitting method. The exponential model with pairing attenuation and the nuclear softness formula.
doi: 10.1088/1402-4896/abb49e
2019DA03 Eur.Phys.J. A 55, 12 (2019) Spins and moment of inertia of superdeformed bands in the Pb isotopes NUCLEAR STRUCTURE 194Hg, 193Tl, 192,194,196Pb; compiled, analyzed spin assignments for superdeformed (SD) bands. 192Tl, 192,193,194,195,196,197Pb; calculated spins of uperdeformed (SD) bands states, SD band head spins using VMI-IBM model; deduced parameters. 192Tl, 193,195,197Pb; calculated kinematic and dynamic moment of inertia vs rotational frequency; compared with data.
doi: 10.1140/epja/i2019-12678-5
2019DA06 Phys.Rev. C 99, 044305 (2019) Empirical evidence of a superrigid structure of "flat" uperdeformed bands NUCLEAR STRUCTURE 189,191,192,193,194,195Tl, 192,193,194,195,196,197Pb; analyzed experimental data for superdeformed bands, and gamma-transition energies using shape fluctuation model, semiclassical vibration distortion model, semiclassical particle rotor model, and exponential model with pairing attenuation; deduced fitting parameters.
doi: 10.1103/PhysRevC.99.044305
2018BI06 Nucl.Phys. A975, 48 (2018) The magnification of structural anomalies with Grodzins systematic in the framework of Asymmetric Rotor Model NUCLEAR STRUCTURE 142,144,146Ba, 144,146,148Ce, 144,146,148,150Nd, 148,150,152,154Sm, 152,154,156,158,160Gd(SF), 154,156,158,160,162,164Dy, 156,158,160,162,164,166,168,170Er, 160,164,166,168,170,172,174Yb, 172,174,176,178,180Hf, 180,182,184,186W, 182,184,186,188,190,192Os, 184,186,188,190,192,194,196Pt; calculated E(2+1) times B(E2) and E(SF) times B(E2) (Grodzins products) vs asymmetry parameter γ0 using ARM (Asymmetric Rotor Model); deduced Grodzins parameters, breakdown of coherence between rotational energy and γ-excitation strength B(E2), indication for a shape transition for Pt isotopes.
doi: 10.1016/j.nuclphysa.2018.04.004
2018DA10 J.Phys.(London) G45, 065103 (2018) Identical superdeformed bands in yrast 152Dy: a systematic description NUCLEAR STRUCTURE 151,152,153Dy, 151Tb; analyzed available data; deduced difference between the calculated and experimental intraband-γ transition energies for super deformed bands, parameters obtained from the least-squares fitting the identical bands.
doi: 10.1088/1361-6471/aac0d1
2018KA33 Pramana 91, 70 (2018) Systematic study of rigid triaxiality in Ba-Pt nuclei and role of Z=64 subshell effect subshell effect NUCLEAR STRUCTURE Z=50-82; analyzed available data; calculated deformation parameters, quadrupole moments. Comparison with available data.
doi: 10.1007/s12043-018-1645-7
2018SH19 Chin.Phys.C 42, 054104 (2018) Band head spin assignment of superdeformed bands in Hg isotopes through power index formula NUCLEAR STRUCTURE 189,190,191,192,193,194,195Hg; analyzed available data; deduced transition energies, head spins of super deformed band, moment of inertia using the power index formula.
doi: 10.1088/1674-1137/42/5/054104
2017BI06 Chin.Phys.C 41, 054102 (2017) Systematic dependence of SFE*B(E2)↑ and ROTE*B(E2)↑ on Np Nn in the framework of shape fluctuation model NUCLEAR STRUCTURE Z=56-64; analyzed available B(E2) data; deduced systematic trends.
doi: 10.1088/1674-1137/41/5/054102
2017DA05 Eur.Phys.J. A 53, 2 (2017) Spins of superdeformed rotational bands in Tl isotopes NUCLEAR STRUCTURE 191,192,193,194,195Tl, 194,196Pb; calculated rotational bands, SD band, excited SD band levels, J, dynamical moment of inertia using soft-rotor model. Compared with available data.
doi: 10.1140/epja/i2017-12190-0
2017DA18 Eur.Phys.J. A 53, 132 (2017) Description of identical superdeformed bands of the A ∼ 190 mass region NUCLEAR STRUCTURE 191,192,193,194,195Hg, 193,194,195Tl, 193,194Pb; calculated rotational superdeformed yrast, excited bands energy, J, band-head moment of inertia, alignment, γ-ray transition energies using two-parameter model (nuclear softness formula, semiclassical particle rotor model) and exponential model with pairing attenuation; deduced 12 identical (yrast, excited, middle-point identical) superdeformed rotational bands, parameters.
doi: 10.1140/epja/i2017-12308-4
2017SH22 Chin.Phys.C 41, 084104 (2017) H.Sharma, N.Sharma, H.M.Mittal Systematic study of kinematic and dynamic moments of inertia of superdeformed bands with NpNn scheme NUCLEAR STRUCTURE N=72-112; analyzed available data; deduced systematics of kinematic moment of inertia, dynamic moment of inertia of superdeformed bands in A ∼ 130, 150, 190 mass regions.
doi: 10.1088/1674-1137/41/8/084104
2017SH48 Int.J.Mod.Phys. E26, 1750074 (2017) Band head spin assignment of superdeformed bands in A∼60-80 mass region through nuclear softness formula NUCLEAR STRUCTURE 58Ni, 58Cu, 62,65,68Zn, 84,86Zr; analyzed available data; deduced the band head spin of superdeformed rotational bands, dynamic moment of inertia, the nuclear softness formula applicability.
doi: 10.1142/S0218301317500744
2017SH56 Chin.Phys.C 41, 124105 (2017) Systematic study of rotational energy formulae for superdeformed bands in La and Ce isotopes NUCLEAR STRUCTURE 130La, 131,132,133Ce; analyzed available data; calculated of superdeformed (SD) band head spins using four parameter formula.
doi: 10.1088/1674-1137/41/12/124105
2016DA01 Int.J.Mod.Phys. E25, 1650038 (2016) A.Dadwal, H.M.Mittal, N.Sharma Level spins of superdeformed bands in A ∼ 80 mass region NUCLEAR STRUCTURE 80,81,82,83Sr, 82,83Y, 83Zr; calculated band head spin, J parameters. Comparison with available data.
doi: 10.1142/S0218301316500385
2016DA10 Chin.Phys.C 40, 114103 (2016) Band head spin assignment of superdeformed bands in 86Zr NUCLEAR STRUCTURE 86Zr; analyzed available data; deduced the band head spins; calculated transition energies; deduced dynamic moment of inertia. VMI model.
doi: 10.1088/1674-1137/40/11/114103
2016KU18 Chin.Phys.C 40, 094104 (2016) Systematic study of the product ((E(2+2)/E(2+1))*B(E2) ↑) through the asymmetric rotor model NUCLEAR STRUCTURE Z=50-82; analyzed available data; calculated (E(2+2)/E(2+1))*B(E2)↑ product values.
doi: 10.1088/1674-1137/40/9/094104
2015KU14 Int.J.Mod.Phys. E24, 1550033 (2015) Systematic dependence of Grodzins product rule on NpNn NUCLEAR STRUCTURE Z=50-82, N=82-126; analyzed available data; deduced systematics of the Grodzins product rule.
doi: 10.1142/S0218301315500330
2015KU18 Phys.Scr. 90, 085304 (2015) Study of multiphonon γγ-band in neutron-rich 112Ru nucleus and molybdenum isotopes NUCLEAR STRUCTURE 112Ru, 104,106,108Mo; calculated γ and γγ band energies, J, π, staggering indices, constant energy terms. Comparison with available data.
doi: 10.1088/0031-8949/90/8/085304
2013SH09 Phys.Rev. C 87, 024322 (2013) N.Sharma, H.M.Mittal, S.Kumar, A.K.Jain Empirical evidence for magic numbers of superdeformed shapes NUCLEAR STRUCTURE A=57-137, 148-154, 189-198; analyzed γ-ray energy ratios for superdeformed structures; deduced nuclear softness parameter, superdeformed magic numbers.
doi: 10.1103/PhysRevC.87.024322
2013SH34 Int.J.Mod.Phys. E22, 1350053 (2013) Systematic study of nuclear softness of superdeformed bands in A = 190 mass region NUCLEAR STRUCTURE 191Au, 189,190,191,192,193,194,195Hg, 189,191,192,193,194,195Tl, 196,197Bi, 198Po; calculated superdeformed bands, nuclear softness parameter. Comparison with ENSDF and XUNDL databases.
doi: 10.1142/S0218301313500535
2011MI23 J.Phys.:Conf.Ser. 312, 092041 (2011) The odd-even staggering in 122-24Xe and 124-128Ba nuclei NUCLEAR STRUCTURE 122,123,124Xe, 124,125,126,127,128Ba; calculated levels, J, π, rotational bands, signature splitting. Compared to data.
doi: 10.1088/1742-6596/312/9/092041
2011MI24 J.Phys.:Conf.Ser. 312, 092042 (2011) Study of triaxiality in Xe-Hg nuclei NUCLEAR STRUCTURE Xe, Ba, Ce, Nd, Sm, Gd, Dy, Er, Yb, Hf, W, Os, Pt, Hg; calculated deformation parameters using rigid triaxial rotor model.
doi: 10.1088/1742-6596/312/9/092042
1991MI05 Phys.Scr. 43, 558 (1991) H.M.Mittal, S.Sharma, J.B.Gupta Tests of Rigid Triaxiality for Light Te-Sm Nuclei NUCLEAR STRUCTURE 118,120,122,124,126,128Te, 120,122,124,126,128,130,132Xe, 126,128,130,132,134Ba, 134,136Ce, 136,138Nd, 138,140Nd; analyzed B(E2) ratios; deduced shape features.
doi: 10.1088/0031-8949/43/6/004
1990GU06 Phys.Scr. 41, 660 (1990) J.B.Gupta, H.M.Mittal, S.Sharma Study of Shape Phase Transitions and the F-Spin Multiplets through the Shape Fluctuation Energy NUCLEAR STRUCTURE A=120-200; calculated shape fluctuation energy; deduced F-spin multiplet shape phase transition features. Interacting boson model, even-even nuclei.
doi: 10.1088/0031-8949/41/5/006
1990GU12 Phys.Rev. C42, 1373 (1990) J.B.Gupta, H.M.Mittal, J.H.Hamilton, A.V.Ramayya Systematic Dependence of the γ-g B(E2) Ratios on the N(p)N(n) Product NUCLEAR STRUCTURE A=120-200; analyzed B(E2) systematics; deduced N(p)N(n) scheme limitations.
doi: 10.1103/PhysRevC.42.1373
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