NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = C.Bhatia Found 14 matches. 2017TO16 Phys.Lett. B 773, 20 (2017) A.P.Tonchev, N.Tsoneva, C.Bhatia, C.W.Arnold, S.Goriely, S.L.Hammond, J.H.Kelley, E.Kwan, H.Lenske, J.Piekarewicz, R.Raut, G.Rusev, T.Shizuma, W.Tornow Pygmy and core polarization dipole modes in 206Pb: Connecting nuclear structure to stellar nucleosynthesis NUCLEAR REACTIONS 208Pb(γ, γ'), E=4.9-8.1 MeV; analyzed available data; deduced a range for the neutron-skin thickness of and a corresponding range for the slope of the symmetry energy, Maxwellian-averaged radiative σ.
doi: 10.1016/j.physletb.2017.07.062
2016GO02 Nucl.Data Sheets 131, 319 (2016) M.E.Gooden, C.W.Arnold, J.A.Becker, C.Bhatia, M.Bhike, E.M.Bond, T.A.Bredeweg, B.Fallin, M.M.Fowler, C.R.Howell, J.H.Kelley, Krishichayan, R.Macri, G.Rusev, C.Ryan, S.A.Sheets, M.A.Stoyer, A.P.Tonchev, W.Tornow, D.J.Vieira, J.B.Wilhelmy Energy Dependence of Fission Product Yields from 235U, 238U and 239Pu for Incident Neutron Energies Between 0.5 and 14.8 MeV NUCLEAR REACTIONS 235,238U, 239Pu(n, F), E=0.5-14.8 MeV; measured reaction products, Eγ, Iγ; deduced fission yields.
doi: 10.1016/j.nds.2015.12.006
2015BH09 Phys.Rev. C 91, 064604 (2015) C.Bhatia, B.F.Fallin, M.E.Gooden, C.R.Howell, J.H.Kelley, W.Tornow, C.W.Arnold, E.Bond, T.A.Bredeweg, M.M.Fowler, W.Moody, R.S.Rundberg, G.Y.Rusev, D.J.Vieira, J.B.Wilhelmy, J.A.Becker, R.Macri, C.Ryan, S.A.Sheets, M.A.Stoyer, A.P.Tonchev Exploratory study of fission product yields of neutron-induced fission of 235U, 238U, and 239Pu at 8.9 MeV NUCLEAR REACTIONS 235,238U, 239Pu(n, F), E=8.9 MeV; measured Eγ, Iγ of fission products of 92Sr, 97Zr, 99Mo, 105Ru, 132Te, 133I, 140Ba, 143Ce, 147Nd at TUNL facility; deduced absolute fission product yields by γ activation method. Comparison with previous experimental results.
doi: 10.1103/PhysRevC.91.064604
2014BH10 Nucl.Data Sheets 119, 176 (2014) C.Bhatia, M.E.Gooden, W.Tornow, A.P.Tonchev Measurements of the (n, 2n) Reaction Cross Section of 181Ta from 8 to 15 MeV NUCLEAR REACTIONS 181Ta(n, 2n), E=8-15 MeV; measured activation Eγ, Iγ; deduced γ transitions, σ. Compared with other data, ENDF/B-VII.1, TUNL-2012 and TENDL-2011.
doi: 10.1016/j.nds.2014.08.049
2014BH11 Nucl.Data Sheets 119, 324 (2014) C.Bhatia, B.Fallin, C.Howell, W.Tornow, M.Gooden, J.Kelley, C.Arnold, E.Bond, T.Bredeweg, M.Fowler, W.Moody, R.Rundberg, G.Rusev, D.Vieira, J.Wilhelmy, J.Becker, R.Macri, C.Ryan, S.Sheets, M.Stoyer, A.Tonchev Fission Product Yield Study of 235U, 238U and 239Pu Using Dual-Fission Ionization Chambers NUCLEAR REACTIONS 235,238U, 239Pu(n, F), E=4.6, 9.0, 14.5 MeV; measured Eγ, Iγ(t) from fission fragments using dual fission chamber; deduced fission products yield ratio. Compared with other data and libraries.
doi: 10.1016/j.nds.2014.08.089
2014MA05 Phys.Rev.Lett. 112, 072501 (2014) R.Massarczyk, R.Schwengner, F.Donau, S.Frauendorf, M.Anders, D.Bemmerer, R.Beyer, C.Bhatia, E.Birgersson, M.Butterling, Z.Elekes, A.Ferrari, M.E.Gooden, R.Hannaske, A.R.Junghans, M.Kempe, J.H.Kelley, T.Kogler, A.Matic, M.L.Menzel, S.Muller, T.P.Reinhardt, M.Roder, G.Rusev, K.D.Schilling, K.Schmidt, G.Schramm, A.P.Tonchev, W.Tornow, A.Wagner Nuclear Deformation and Neutron Excess as Competing Effects for Dipole Strength in the Pygmy Region NUCLEAR REACTIONS 124,128,132,134Xe(γ, X), E<12 MeV; measured reaction products, Eγ, Iγ. 124,128,132,134Xe; deduced photoabsorption σ, summed B(E1) strength, nuclear deformation in the region of the pygmy dipole resonance. Nuclear resonance fluorescence experiment, random-phase approximation calculations, comparison with available data.
doi: 10.1103/PhysRevLett.112.072501
2014MA90 Phys.Rev. C 90, 054310 (2014) R.Massarczyk, G.Rusev, R.Schwengner, F.Donau, C.Bhatia, M.E.Gooden, J.H.Kelley, A.P.Tonchev, W.Tornow Magnetic dipole strength in 128Xe and 134Xe in the spin-flip resonance region NUCLEAR REACTIONS 128,134Xe(polarized γ, γ'), E=6.0-9.6 MeV; measured Eγ, Iγ, γ(pol, θ) using HIγS facility at TUNL. 128,134Xe; deduced branching ratios and comparison with γ-ray cascade simulations, photoabsorption σ(E) for M1 and E1 transitions, B(M1), B(E1). Comparison of σ(E) with previous experimental results, predictions of phenomenological expressions, RIPL3 recommendations, triple-Lorentzian (TLO) model for E1 and the triple-Gaussian for M1, and QRPA calculations.
doi: 10.1103/PhysRevC.90.054310
2013BH01 Phys.Rev. C 87, 011601 (2013) C.Bhatia, S.W.Finch, M.E.Gooden, W.Tornow 136Xe(n, 2n)135Xe cross section between 9 and 15 MeV NUCLEAR REACTIONS 136Xe(n, 2n), E=9.0-14.9 MeV; measured Eγ, Iγ, σ(E) for production of g.s. and isomer of 135Xe by activation method. 135Xe; deduced half-lives of g.s. and isomer, and compared with literature values. Comparison of σ(E) with previous studies, and with evaluations. Relevance to background contributions in search for neutrinoless double-β decay of 136Xe.
doi: 10.1103/PhysRevC.87.011601
2013BH03 Phys.Rev. C 87, 031601 (2013) C.Bhatia, M.E.Gooden, W.Tornow, A.P.Tonchev Ground-state and isomeric-state cross sections for 181Ta(n, 2n)180Ta between 8 and 15 MeV NUCLEAR REACTIONS 181Ta(n, 2n)180Ta, E=8-15 MeV; measured Eγ, Iγ, σ(E) at TUNL facility. Comparison with previous experimental results, and with evaluated libraries ENSDF VII.1 and TENDL 2011.
doi: 10.1103/PhysRevC.87.031601
2012BH09 Phys.Rev. C 86, 041602 (2012) C.Bhatia, S.W.Finch, M.E.Gooden, W.Tornow 40Ar(n, p)40Cl reaction cross section between 9 and 15 MeV NUCLEAR REACTIONS 40Ar(n, p)40Cl, E=9-15 MeV; measured Eγ, Iγ, σ(E), activation method. Comparison with previous experimental data, evaluations and theoretical predictions. Relevance to background contributions in experiments for 0νββ decay mode, dark matter, and neutrino detection.
doi: 10.1103/PhysRevC.86.041602
2011AD18 Eur.Phys.J. A 47, 85 (2011) J.Adam, C.Bhatia, K.Katovsky, V.Kumar, M.Majerle, V.S.Pronskikh, A.M.Khilmanovich, B.A.Martsynkevich, I.V.Zhuk, V.M.Golovatiouk, W.Westmeier, A.A.Solnyshkin, V.M.Tsoupko-Sitnikov, A.S.Potapenko A study of reaction rates of (n, f), (n, γ) and (n, 2n) reactions in natU and 232Th by the neutron fluence produced in the graphite set-up (GAMMA-3) irradiated by 2.33 GeV deuteron beam NUCLEAR REACTIONS 232Th, U(n, f), (n, γ), (n, 2n), E=1.E-10-1.E3 MeV; measured reaction products, Eγ, Iγ. 85mKr, 93Y, 97Zr, 99Mo, 103Ru, 105Rh, 132Te, 131,133I, 133,135Xe, 140Ba, 141,143Ce, 231Th, 233Pa, 237U, 239Np deduced reaction rates, T1/2. 232Th, U(n, 2n), E=10-2000 MeV; calculated σ using TALYS. 232Th(n, f), E=400 keV, 14, 25, 50, 100, 200 MeV; measured fission products, deduced mass distribution; calculated mass distribution at two lowest energies using TALYS. Neutron flux calculated using MCNPX with LA150 cross section library.
doi: 10.1140/epja/i2011-11085-4
2010AD13 Eur.Phys.J. A 43, 159 (2010) J.Adam, K.Katovsky, M.Majerle, M.I.Krivopustov, V.Kumar, C.Bhatia, M.Sharma, A.A.Solnyshkin, V.M.Tsoupko-Sitnikov A study of nuclear transmutation of Th and natU with neutrons produced in a Pb target and U blanket irradiated by 1.6 GeV deuterons NUCLEAR REACTIONS 232Th(n, γ), (n, 2n), (n, F)99Mo, 235,238U(n, γ), (n, F)99Mo/132Te/133I/135I/135Xe/140Ba/143Ce, E=thermal-1000 MeV [from 208Pb(d, X), E=1.6 GeV spallation source]; measured Eγ, Iγ using HPGe detectors; deduced σ, reaction and transmutation rates. Comparison with simulations and TARC experimental data.
doi: 10.1140/epja/i2010-10909-y
2010BH02 Phys.Rev. C 81, 024614 (2010) Determination of neutron multiplication coefficients for fuel elements irradiated by spallation neutrons NUCLEAR REACTIONS 232Th, 233,235,238U(n, X), E=spallation neutrons; analyzed σ, neutron multiplication coefficient keff in capture, fission, and non-elastic channels for irradiation of fuel elements by spallation neutrons of energies up to 250 MeV, neutron removal and production rates. Discussed neutron poisoning of thermal and fast neutrons.
doi: 10.1103/PhysRevC.81.024614
2009KU17 Eur.Phys.J. A 40, 231 (2009) V.Kumar, C.Bhatia, H.Kumawat, J.Adam Validation of CASCADE code using the monitor reactions NUCLEAR REACTIONS 27Al(n, X), (p, X), E=10-25000 MeV; 27Al(d, X), E=10-25000 MeV/nucleon; calculated non-elastic σ. 27Al(n, X)22Na/24Na, E=1-25000 MeV; 27Al(p, X)22Na/24Na, E=10-25000 MeV; 27Al(d, X)24Na, E=200-25000 MeV/nucleon; calculated σ. Comparison of the CASCADE code with experimental data.
doi: 10.1140/epja/i2009-10760-9
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