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NSR database version of May 1, 2024.

Search: Author = U.Gupta

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2023YA11      Phys.Rev. C 107, 044605 (2023)

A.Yadav, G.Ram, M.S.Asnain, I.Majeed, M.Shuaib, V.R.Sharma, I.Bala, U.Gupta, S.Gupta, D.P.Singh, P.P.Singh, M.Sharma, R.Kumar, B.P.Singh, R.Prasad

Understanding the low-energy incomplete fusion reactions

NUCLEAR REACTIONS ¹⁵⁹Tb(¹⁸O, 3n), (¹⁸O, 4n), (¹⁸O, 5n), (¹⁸O, 6n), (¹⁸O, 2nα), (¹⁸O, 5nα), (¹⁸O, 6nα), (¹⁸O, 5npα), E=82, 95, 97, 100 MeV; measured Eγ, Iγ; deduced σ(E), contributions of complete and incomplete fusion channels. Comparison to predictions done using the PACE4 code. Systematics of incomplete fusion with different projectiles - ¹²C, ¹³C, ¹⁴N, ¹⁶O, ¹⁸O, ¹⁹F, ²⁰Ne. Activation technique experiment at the Inter-University Accelerator Centre (IUAC, New Delhi).

doi: 10.1103/PhysRevC.107.044605
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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
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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
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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.

2021OJ01      Phys.Rev. C 104, 034615 (2021)

A.Ojha, S.Gupta, U.Gupta, P.P.Singh, A.Yadav, D.P.Singh, M.Shuaib, B.P.Singh, R.Prasad

Mass-number dependence of statistical model parameters and its impact on incomplete fusion fraction calculations

NUCLEAR REACTIONS ¹⁸¹Ta(¹⁶O, 3n)¹⁹⁴Tl, (¹⁶O, 4n)¹⁹³Tl, (¹⁶O, 5n)¹⁹²Tl, (¹⁶O, 3np)¹⁹³Hg, (¹⁶O, 4np)¹⁹²Hg, (¹⁶O, 5np)¹⁹¹Hg, E=75-105 MeV; ¹⁶⁵Ho(¹²C, 3n)¹⁷⁴Ta, (¹²C, 4n)¹⁷³Ta, (¹²C, 5n)¹⁷²Ta, (¹²C, 3np)¹⁷³Hf, E=55-85 MeV; ¹⁶³Dy(¹⁴N, 3n)¹⁷⁴Ta, (¹⁴N, 4n)¹⁷³Ta, (¹⁴N, 5n)¹⁷²Ta, E=65-85 MeV; ⁷⁴Ge(¹⁶O, 4n)⁸⁶Zr, (¹⁶O, 2np)⁸⁷Y, (¹⁶O, 3np)⁸⁶Y, (¹⁶O, 4np)⁸⁵Y, E=50-110 MeV; calculated σ(E) using statistical model based PACE4 code, with optical model potential (OMP) parameters, summed σ(E) using different sets of OMP parameters and impact on incomplete fusion (ICF) fraction, and effect of deformation parameter β₂ on incomplete fusion. Comparison with experimental data.

doi: 10.1103/PhysRevC.104.034615
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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.

2019SO21      Acta Phys.Pol. B50, 291 (2019)

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

Entrance Channel Effects on Fission Fragment Mass Distribution in ¹²C + ¹⁶⁹Tm System

NUCLEAR REACTIONS ¹⁶⁹Tm(¹²C, X), E= 77.18, 83.22, 89.25 MeV; measured Eγ, Iγ(t); deduced production σ of evaporation residues, isotopic yieldsmass distribution of fission fragments.

doi: 10.5506/aphyspolb.50.291
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6310.

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6326.

2017AL39      Nucl.Phys. A968, 403 (2017)

R.Ali, M.Afzal Ansari, D.Singh, R.Kumar, D.P.Singh, M.K.Sharma, U.Gupta, B.P.Singh, P.D.Shidling, D.Negi, S.Muralithar, R.P.Singh, R.K.Bhowmik

Observed side feeding in incomplete fusion dynamics in ¹⁶O + ¹⁶⁰Gd reaction at energy ∼ 5.6 MeV/A: Spin distribution measurements

NUCLEAR REACTIONS ¹⁶⁰Gd(¹⁶O, x), E≈5.6 MeV/nucleon; measured Eγ, Iγ(θ), Ep, Ip(θ), Eα, Iα(θ), pγ-coin, αγ-coin using GDA (Gamma Detector Array) consisting of 12 n-type Compton suppressed HPGE working together with CPDA (Charged Particle Detector Array); deduced relative spin distributions (relative yields vs spin) of different reaction channels, evaporation residues yrast bands side feeding intensities, mean input angular momentum for different reaction channels.

doi: 10.1016/j.nuclphysa.2017.09.005
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2017SO12      Phys.Rev. C 96, 014620 (2017)

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

Fission-like events in the ¹²C + ¹⁶⁹Tm system at low excitation energies

NUCLEAR REACTIONS ¹⁶⁹Tm(¹²C, X)^74mBr/⁷⁴Kr/⁷⁵Br/⁷⁵Ge/⁷⁵Kr/⁷⁶Kr/⁷⁷Kr/⁷⁸As/⁷⁹Rb/⁸¹Sr/⁸⁴Br/⁸⁵Zr/⁸⁶Y/⁸⁷Zr/⁸⁹Rb/⁹³Y/⁹⁴Ru/⁹⁵Ru/⁹⁷Nb/^98mNb/¹⁰¹Tc/^102mTc/¹⁰⁴Tc/¹⁰⁴Ag/¹⁰⁵Tc/¹⁰⁵In/¹⁷⁵Re/¹⁷⁶Re/¹⁷⁷Re/¹⁷⁸Re/¹⁷⁷W/¹⁷³Ta/¹⁷⁴Ta/¹⁷⁵Ta/¹⁷⁶Ta/¹⁷¹Lu, E=77.81, 83.22, 89.25 MeV; measured Eγ, Iγ, recoil-catcher activation technique, half-life of ⁷⁴Kr decay, production σ(E) of fission products and evaporation residues, charge and mass distribution of fission fragments at the pelletron accelerator facility of IUAC-New Delhi; deduced fission as one of the competing modes of deexcitation of complete and/or incomplete fusion composites at low excitation energies. Comparison with calculations using PACE code. ¹⁸¹Ta(¹⁶O, X), E*=67.04 MeV; ¹⁵⁹Tb(¹⁶O, X), E*=57.1 MeV; ¹⁶⁹Tm(¹⁶O, X), E*=61.06 MeV; ²³²Th(⁷Li, X), E*=41.7 MeV; ²³²Th(¹¹B, X), E*=55.7 MeV; ²³⁸U(¹¹B, X), E*=67.4 MeV; ²³⁸U(²²Ne, X), E*=64.5 MeV; ²⁰⁸Pb(²⁰Ne, X), E*=46.4 MeV; analyzed previous experimental data for isotopic yield distributions.

doi: 10.1103/PhysRevC.96.014620
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6310.

2012YA03      Phys.Rev. C 85, 034614 (2012)

A.Yadav, V.R.Sharma, P.P.Singh, D.P.Singh, M.K.Sharma, U.Gupta, R.Kumar, B.P.Singh, R.Prasad, R.K.Bhowmik

Large influence of incomplete fusion in ¹²C + ¹⁵⁹Tb at E_lab ≈ 4-7 MeV/nucleon

NUCLEAR REACTIONS ¹⁵⁹Tb(¹²C, X)¹⁶⁰Ho/^160mHo/¹⁶¹Ho/¹⁶³Tm/¹⁶⁵Tm/¹⁶⁵Lu/¹⁶⁷Yb/¹⁶⁷Lu/¹⁶⁸Lu/^168mLu, E=54-88 MeV; measured Eγ, Iγ, production σ(E) for complete fusion and incomplete fusion; deduced total fusion cross section, percentage fraction of incomplete fusion (ICF), mass asymmetry dependence on ICF fraction. Gamma-activation technique. Comparison with statistical model code PACE4 and previous studies.

doi: 10.1103/PhysRevC.85.034614
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6196.

2011YA17      Int.J.Mod.Phys. E20, 2133 (2011)

A.Yadav, P.P.Singh, V.R.Sharma, U.Gupta, D.P.Singh, M.K.Sharma, B.P.Singh, R.Prasad, R.Kumar, R.P.Singh, S.Muralithar, R.K.Bhowmik

Signature of pre-equilibrium-emission in forward-to-backward yield ratio measurement

NUCLEAR REACTIONS ¹⁶⁹Tm(¹⁶O, X)¹⁸¹Os/¹⁸¹Re/¹⁸²Re/¹⁸³Re/¹⁷⁹W/¹⁸¹W/¹⁸²W/¹⁷⁹Ta/¹⁸⁰Ta, E=5.6 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced normalized yield, yield ratios; deduced preequilibrium emission.

doi: 10.1142/S0218301311020198
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2009GU24      Phys.Rev. C 80, 024613 (2009)

U.Gupta, P.P.Singh, D.P.Singh, M.K.Sharma, A.Yadav, R.Kumar, S.Gupta, H.D.Bhardwaj, B.P.Singh, R.Prasad

Disentangling full and partial linear momentum transfer events in the ¹⁶O+¹⁶⁹Tm system at E_proj ≤ 5.4 MeV/nucleon

NUCLEAR REACTIONS ¹⁶⁹Tm(¹⁶O, X)¹⁷¹Lu/¹⁷²Lu/¹⁷¹Hf/¹⁷⁵Hf/¹⁸¹Re/¹⁸¹Os/¹⁸²Os/¹⁸²Ir, E=76, 81 MeV; measured σ, angular distributions, forward recoil ranges and most probable recoil ranges.

doi: 10.1103/PhysRevC.80.024613
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2009SI02      Phys.Lett. B 671, 20 (2009)

P.P.Singh, B.P.Singh, M.K.Sharma, U.Gupta, R.Kumar, D.Singh, R.P.Singh, S.Murlithar, M.A.Ansari, R.Prasad, R.K.Bhowmik

Probing of incomplete fusion dynamics by spin-distribution measurement

NUCLEAR REACTIONS ¹⁶⁹Tm(¹⁶O, X)¹⁷⁷Re/¹⁷⁸Re/¹⁷⁹Re/¹⁸⁰Os/¹⁸¹Os/¹⁸²Os/¹⁸⁰Ir/¹⁸¹Ir/¹⁸²Ir, E=5.6 MeV/nucleon; measured Eγ, Iγ, (charged-particle)γ-coin, yields, spin distributions; deduced γ cascade feeding intensities. Comparison with PACE4 calculations.

doi: 10.1016/j.physletb.2008.11.035
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2009SI34      Phys.Rev. C 80, 064603 (2009)

P.P.Singh, A.Yadav, D.P.Singh, U.Gupta, M.K.Sharma, R.Kumar, D.Singh, R.P.Singh, S.Muralithar, M.A.Ansari, B.P.Singh, R.Prasad, R.K.Bhowmik

Role of high ℓ values in the onset of incomplete fusion

NUCLEAR REACTIONS ¹⁶⁹Tm(¹²C, X)¹⁷¹Lu/¹⁷³Ta/¹⁷⁴Ta/¹⁷⁵Ta/¹⁷⁶W/¹⁷⁶Re/¹⁷⁷Re/¹⁷⁸Re/¹⁸⁰Ir/¹⁸⁰Os/, E=5.6, 6.5 MeV/nucleon; measured α spectra, Eγ, Iγ, γ(particle)-coin; deduced yields, spin distributions, and role of angular momentum on yields in incomplete fusion. Comparison with data for ¹⁶⁹Tm(¹⁶O, X) reaction.

doi: 10.1103/PhysRevC.80.064603
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2008GU13      Nucl.Phys. A811, 77 (2008)

U.Gupta, P.P.Singh, D.P.Singh, M.K.Sharma, A.Yadav, R.Kumar, B.P.Singh, R.Prasad

Observation of large incomplete fusion in ¹⁶O + ¹⁰³Rh system at ≈ 3-5 MeV/nucleon

NUCLEAR REACTIONS ¹⁰³Rh(¹⁶O, X)¹¹⁴Te/¹¹⁵Te/¹¹⁶Te/¹¹⁷Te/¹¹⁵Sb/¹¹⁶Sb/¹¹⁷Sb/¹¹⁰Sn/¹⁰⁸In/¹⁰⁹In/¹¹⁰In/¹¹¹In/¹⁰³Ag/¹⁰⁴Ag/¹⁰⁶Ag, E≈46-85 MeV; measured Eγ, Iγ, σ. Discussed fraction of (in)complete fusion. Comparison with PACE4 calculations. HPGe detector, stacked targets, energy degradation technique.

doi: 10.1016/j.nuclphysa.2008.07.013
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6069.

1979MI11      J.Phys.(London) G5, 855 (1979)

S.C.Misra, U.C.Gupta

The (n, 2n) Cross Sections of ⁸⁵Rb, ¹⁰⁷Ag and ¹⁸¹Ta at 14.6 MeV

NUCLEAR REACTIONS ⁸⁵Rb, ¹⁰⁷Ag, ¹⁸¹Ta(n, 2n), E=14.6 MeV; measured σ. Natural target, NaI(Tl) detector, activation technique.

doi: 10.1088/0305-4616/5/6/011
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30507.

1971MA14      Can.J.Phys. 49, 1053 (1971)

P.N.Maheshwari, U.C.Gupta, C.St-Pierre

Study of the ⁴⁸Ti(α, p)⁵¹V and ⁵⁰Ti(³He, d)⁵¹V Reactions

NUCLEAR REACTIONS ⁴⁸Ti(α, p), E=8-11 MeV; ⁵⁰Ti(³He, d), E=10 MeV; measured σ(Ep, θ), σ(Ed, θ). ⁵¹V deduced levels, J, π, L, S.

doi: 10.1139/p71-129
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1967SI01      Nucl.Phys. A91, 557 (1967)

N.P.S.Sidhu, U.C.Gupta

Lifetimes of the 1.10 and 1.29 MeV Excited States in ⁵⁹Co

RADIOACTIVITY ⁵⁹Fe [from ⁵⁸Fe(n, γ)]; measured βγ (t). ⁵⁹Co levels deduced T_1/2. Enriched target.

doi: 10.1016/0375-9474(67)90575-1
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1965DH01      Current Sci.(India) 34, 504 (1965)

K.C.Dhingra, U.C.Gupta, N.P.S.Sidhu

Decay of ⁵¹Cr

NUCLEAR STRUCTURE ⁵¹Cr; measured not abstracted; deduced nuclear properties.

1965GU06      Nucl.Phys. 73, 413 (1965)

U.C.Gupta, P.K.Srivastava, G.D.Khera

Decay of ⁸⁶Rb

RADIOACTIVITY ⁸⁶Rb[from ⁸⁵Rb(n, γ)]; measured Iγ, βγ-coin. Natural target.

doi: 10.1016/0029-5582(65)90686-3
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1964MI07      Nucl.Phys. 51, 174 (1964)

S.C.Misra, U.C.Gupta, N.P.S.Sidhu

Decay of ⁴⁷Sc

NUCLEAR STRUCTURE ⁴⁷Sc; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(64)90261-5
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1962GU09      J.Sci.Ind.Res.(India) 21B, 1 (1962)

U.C.Gupta, M.G.Shahani, P.K.Srivastava

Internal Conversion Coefficients of Au¹⁹⁸, Hg²⁰³, Cs¹³⁷ and Cr⁵¹ Using a CsI(Tl) Scintillation Spectrometer

NUCLEAR STRUCTURE ²⁰³Hg, ¹⁹⁸Au, ¹³⁷Cs, ⁵¹Cr; measured not abstracted; deduced nuclear properties.

1956MI17      Phys.Rev. 101, 740 (1956)

D.W.Miller, B.M.Carmichael, U.C.Gupta, V.K.Rasmussen, M.B.Sampson

Scattering of 22-MeV Alpha Particles by N¹⁴

doi: 10.1103/PhysRev.101.740
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1955RA41      Phys.Rev. 100, 851 (1955)

V.K.Rasmussen, D.W.Miller, M.B.Sampson, U.C.Gupta

Reactions Be⁹(α, α'), Be⁹(α, d), and Be⁹(d, d')

doi: 10.1103/PhysRev.100.851
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Note: The following list of authors and aliases matches the search parameter U.Gupta: , U.C.GUPTA