NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = A.Saha Found 93 matches. 2022MA08 Phys.Rev. C 105, L021603 (2022) S.Manna, C.Bhattacharya, T.K.Rana, S.Kundu, R.Pandey, A.Sen, T.K.Ghosh, P.Roy, G.Mukherjee, S.Mukhopadhyay, K.Banerjee, J.K.Meena, P.Karmakar, D.Paul, S.Dalal, J.K.Sahoo, R.M.Saha, A.K.Saha, S.Bhattacharya Signature of fusion suppression in complex fragment emission NUCLEAR REACTIONS 9Be(20Ne, 6Li), (20Ne, 7Li), (20Ne, 7Be), (20Ne, 9Be) E=157.2-193 MeV; 12C(16O, 6Li), (16O, 7Li), (16O, 7Be), (16O, 9Be), E=135.9-161.1 MeV; measured reaction products; deduced σ(θ), σ(E). Comparison to CASCADE calculations. ChAKRA array of DSSD detectors at Variable Energy Cyclotron Centre, Kolkata.
doi: 10.1103/PhysRevC.105.L021603
2022SA32 Phys.Rev. C 106, 014901 (2022) Machine-learning model-driven prediction of the initial geometry in heavy-ion collision experiments
doi: 10.1103/PhysRevC.106.014901
2021BA35 Phys.Rev. C 104, 024320 (2021) S.Basak, S.S.Alam, D.Kumar, A.Saha, T.Bhattacharjee Shape coexistence scenario in 150Sm from a γ-γ fast-timing measurement RADIOACTIVITY 150Pm(β-)[from 150Nd(p, n), E=8.0 MeV at VECC-Kolkata]; measured Eγ, Iγ, γγ-coin, level half-lives by γγ(t) using an array of six Compton-suppressed Clover HPGe detectors and VENTURE array of eight CeBr3 detectors. 150Sm; deduced levels, J, π, B(E2), ρ2(E0), shape coexistence and shape mixing. Comparison with IBM and DPPQ calculations. Systematics of B(E2) and ρ2(E0) values for 150,152Sm, 156,158Gd.
doi: 10.1103/PhysRevC.104.024320
2021DA02 Nucl.Phys. A1006, 122079 (2021) S.Das, A.Adhikari, S.S.Alam, S.Sharma, S.Aich, A.Gupta, Y.Sapkota, A.Das, A.Saha, S.K.Dey, D.Pramanik, A.Bisoi, I.Ray, T.Bhattacharjee, C.C.Dey, S.Sarkar, M.S.Sarkar Decay spectroscopy of 117, 118Sn RADIOACTIVITY 117,118Sb(EC), 117Sn(IT) [from In(α, X), E=32 MeV]; measured decay products, Eγ, Iγ, γ-γ-coin.; deduced γ-ray energies and intensities, J, π, level T1/2. Comparison with available data, shell model calculations.
doi: 10.1016/j.nuclphysa.2020.122079
2021MA77 Eur.Phys.J. A 57, 286 (2021) S.Manna, T.K.Rana, C.Bhattacharya, S.Kundu, R.Pandey, K.Banerjee, P.Roy, A.Sen, T.K.Ghosh, G.Mukherjee, D.Mondal, M.M.Shaikh, J.K.Meena, P.Karmakar, D.Paul, K.Atreya, S.Basu, V.Srivastava, A.Chaudhuri, T.Roy, A.Asgar, A.Dey, A.Dhal, M.Sinha, J.K.Sahoo, A.K.Saha, R.M.Saha, S.Bhattacharya Search for the Hoyle analogue state in 16O NUCLEAR REACTIONS 16O, 12C(α, X), E=45 MeV; measured reaction products, Eα, Iα. 16O, 12C, 8Be; deduced σ, specific decay channels, lack of evidence for the Hoyle analogue state.
doi: 10.1140/epja/s10050-021-00592-8
2021MO18 Int.J.Mod.Phys. E30, 2150039 (2021) A.K.Mondal, C.Basu, S.Adhikari, C.Bhattacharya, T.K.Rana, S.Kundu, S.Manna, R.Pandey, P.Roy, A.Sen, J.K.Meena, A.K.Saha, J.K.Sahoo, D.Basak, T.Bar, H.Pai, A.Bisoi, A.K.Mitra, P.Biswas 12C(20Ne, 16O)16O α-transfer reaction and astrophysical S-factors at 300 keV NUCLEAR REACTIONS 12C(20Ne, 16O), E=150 MeV; measured reaction products; deduced energy spectra, σ(θ, E), σ(θ), S-factors. Asymptotic Normalization Constant (ANC). FRESCO calculations.
doi: 10.1142/S0218301321500397
2021PA41 Phys.Lett. B 823, 136760 (2021) D.Pandit, D.Mondal, T.K.Ghosh, S.Mukhopadhyay, S.Pal, A.Sen, A.K.Saha, V.N.Jha, S.Saha, C.Bhattacharya, A.K.Mohanty Search for coherent bremsstrahlung from spontaneous fission at 555 meter deep underground laboratory RADIOACTIVITY 252Cf(SF); measured decay products, Eγ, Iγ, γ-γ-coin.; deduced a new upper limit for γ-ray emission from the nucleus-nucleus coherent bremsstrahlung in 25-180 MeV energy region, which is two orders of magnitude lower than the previous value.
doi: 10.1016/j.physletb.2021.136760
2021RA05 Phys.Rev. C 103, 034614 (2021) T.K.Rana, S.Kundu, C.Bhattacharya, S.Manna, P.Roy, R.Pandey, A.Sen, T.K.Ghosh, G.Mukherjee, K.Banerjee, S.Mukhopadhyaya, D.Paul, M.M.Shaikh, S.Nandi, V.Srivastava, J.K.Sahoo, J.K.Meena, A.K.Saha, R.M.Saha, S.Dalal, S.Bhattacharya Complex fragment emission in dissipative binary decay of 74, 76Kr NUCLEAR REACTIONS 56Fe(20Ne, X)6Li/7Li/7Be/9Be/10B/11B/11C/12C/13C/14C, E=147.5, 166.5 MeV; 58Ni(16O, X)6Li/7Li/7Be/9Be/10B/11B/11C/12C/13C/14C, E=143.8, 161.6 MeV; measured emitted reaction products, two-dimensional particle identification spectra using two silicon strip detector ΔE-E telescopes of the ChAKRA array at the Variable Energy Cyclotron Centre in Kolkata; deduced double-differential σ(E, θ) for fragments, Q-value distributions of different isotopes, total cross sections and ratio of isotopic cross sections, variation of angular-momentum dissipation factor with different isotopes of the fragments, lifetimes of the dinuclear composites compared with compound-nuclear lifetimes; discussed fragment emission mechanism from hot dinuclear composites.
doi: 10.1103/PhysRevC.103.034614
2021SU25 Nat.Phys. 17, 687 (2021), Erratum Nat.Phys. 18, 473 (2022) V.Sulkosky, C.Peng, J.Chen, A.Deur, S.Abrahamyan, K.A.Aniol, D.S.Armstrong, T.Averett, S.L.Bailey, A.Beck, P.Bertin, F.Butaru, W.Boeglin, A.Camsonne, G.D.Cates, C.-C.Chang, S.Choi, E.Chudakov, L.Coman, J.C.Cornejo, B.Craver, F.Cusanno, R.De Leo, C.W.de Jager, J.D.Denton, S.Dhamija, R.Feuerbach, J.M.Finn, S.Frullani, K.Fuoti, H.Gao, F.Garibaldi, O.Gayou, R.Gilman, A.Glamazdin, C.Glashausser, J.Gomez, J.-O.Hansen, D.Hayes, F.W.Hersman, D.W.Higinbotham, T.Holmstrom, T.B.Humensky, C.E.Hyde, H.Ibrahim, M.Iodice, X.Jiang, L.J.Kaufman, A.Kelleher, K.E.Keister, W.Kim, A.Kolarkar, N.Kolb, W.Korsch, K.Kramer, G.Kumbartzki, L.Lagamba, V.Laine, G.Laveissiere, J.J.Lerose, D.Lhuillier, R.Lindgren, N.Liyanage, H.-J.Lu, B.Ma, D.J.Margaziotis, P.Markowitz, K.R.McCormick, M.Meziane, Z.-E.Meziani, R.Michaels, B.Moffit, P.Monaghan, S.Nanda, J.Niedziela, M.Niskin, R.Pandolfi, K.D.Paschke, M.Potokar, A.Puckett, V.A.Punjabi, Y.Qiang, R.D.Ransome, B.Reitz, R.Roche, A.Saha, A.Shabetai, S.Sirca, J.T.Singh, K.Slifer, R.Snyder, P.Solvignon, R.Stringer, R.Subedi, W.A.Tobias, N.Ton, P.E.Ulmer, G.M.Urciuoli, A.Vacheret, E.Voutier, K.Wang, L.Wan, B.Wojtsekhowski, S.Woo, H.Yao, J.Yuan, X.Zhan, X.Zheng, L.Zhu Measurement of the generalized spin polarizabilities of the neutron in the low-Q2 region NUCLEAR REACTIONS 3He(polarized e-, e-), E=1.1-4.4 GeV; measured reaction products, Eβ, Iβ. 1NN; deduced transverse-transverse and longitudinal-transverse interference σ, generalized neutron spin polarizabilities. Comparison with chiral effective field theory calculations.
doi: 10.1038/s41567-021-01245-9
2020AL17 Eur.Phys.J. A 56, 269 (2020) S.S.Alam, D.Banerjee, T.Bhattacharjee, P.Blaha, D.Kumar, A.Saha, M.S.Sarkar, S.Sarkar, S.K.Das Measurement of electric quadrupole moment in neutron rich 131, 132I RADIOACTIVITY 131,132Te(β-) [from U(α, F), E=40 MeV]; measured decay products, quadrupole frequencies, Eγ, Iγ; deduced γ-ray energies, J, π, electric quadrupole moments, deformation parameters, evolution of collectivity. Comparison with a large basis shell model calculations.
doi: 10.1140/epja/s10050-020-00281-y
2020SA28 Eur.Phys.J. A 56, 189 (2020) A.Saha, T.Bhattacharjee, D.Banerjee, D.Pandit, P.Das, S.Bhattacharya, R.Guin, S.K.Das, S.R.Banerjee β-Decay endpoint energy measurement in 150Pm → 150Sm using β - γ coincidence
doi: 10.1140/epja/s10050-020-00194-w
2019AL03 Phys.Rev. C 99, 014306 (2019) S.S.Alam, T.Bhattacharjee, D.Banerjee, A.Saha, S.Das, M.S.Sarkar, S.Sarkar Lifetimes and transition probabilities for the low-lying states in 131I and 132Xe RADIOACTIVITY 131mTe[from 238U(α, F), E=40 MeV]; 132I(β-)[from decay of 132Te formed in 238U(α, F), E=40 MeV]; measured Eγ, Iγ, γγ-coin, level half-lives by γγ(t) fast-timing method, and half-life of 1797-keV nanosecond isomer in 131I by slope method using the VENTURE array of CeBr3 scintillators and VENUS arrays of six Compton-suppressed Clover HPGe detectors at the K-130 cyclotron facility of VECC, Kolkata. 131I, 132Xe; deduced levels, J, π, configurations, B(E1), B(E2), B(E3). Systematics of E1 decays from 11/2- levels in 121,123,125,127,131I, and 13/2- and 15/2- levels in 129Sb, 131,133I. Comparison with large-basis shell model calculations using the NUSHELLX code. NUCLEAR STRUCTURE 131I, 132Xe; calculated levels, J, π, dominant particle partitions, configurations, and level half-lives using the large-basis shell model (LBSM) with the NUSHELLX code. Comparison with experimental data.
doi: 10.1103/PhysRevC.99.014306
2019RA29 Phys.Lett. B 793, 130 (2019) T.K.Rana, S.Bhattacharya, C.Bhattacharya, S.Manna, S.Kundu, K.Banerjee, R.Pandey, P.Roy, A.Dhal, G.Mukherjee, V.Srivastava, A.Dey, A.Chaudhuri, T.K.Ghosh, A.Sen, Md.A.Asgar, T.Roy, J.K.Sahoo, J.K.Meena, A.K.Saha, R.M.Saha, M.Sinha, A.Roy New high precision study on the decay width of the Hoyle state in 12C RADIOACTIVITY 12C(3α) [from 12C(α, α), E=15 MeV/nucleon]; measured decay products, EnullIα; deduced Dalitz plots, the upper limit for direct decay.
doi: 10.1016/j.physletb.2019.04.028
2019SA61 J.Phys.(London) G46, 055102 (2019); Corrigendum J.Phys.(London) G46, 109501 (2019) A.Saha, T.Bhattacharjee, D.Curien, J.Dudek, I.Dedes, K.Mazurek, A.Gozdz, S.Tagami, Y.R.Shimizu, S.R.Banerjee, S.Rajbanshi, A.Bisoi, G.de Angelis, S.Bhattacharya, S.Bhattacharyya, S.Biswas, A.Chakraborty, S.Das Gupta, B.Dey, A.Goswami, D.Mondal, D.Pandit, R.Palit, T.Roy, R.P.Singh, M.S.Sarkar, S.Saha, J.Sethi Spectroscopy of a tetrahedral doubly magic candidate nucleus 16070Yb90 NUCLEAR REACTIONS 148Sm(16O, 4n)160Yb, E=90 MeV; measured reaction products, Eγ, Iγ, γγ-coin, γγ(θ)(DCO), γγ(θ)(ADO) and γγ(linearpol) using INGA array of 20 Compton-suppressed HPGe clover detectors at TIFR pelletron facility. 160Yb; deduced high-spin levels, J, π, multipolarities, rotational bands, alignments, tetrahedral deformation. Systematics of g.s. and negative-parity bands in 152,154,156Gd.
doi: 10.1088/1361-6471/ab0573
2018BH06 Phys.Rev. C 98, 044311 (2018) S.Bhattacharya, S.Bhattacharyya, R.Banik, S.Das Gupta, G.Mukherjee, A.Dhal, S.S.Alam, Md.A.Asgar, T.Roy, A.Saha, S.Nandi, T.Bhattacharjee, A.Choudhury, D.Mondal, S.Mukhopadhyay, P.Mukhopadhyay, S.Pal, D.Pandit, I.Shaik, S.R.Banerjee Yrast and non-yrast spectroscopy of 199Tl using α-induced reactions NUCLEAR REACTIONS 197Au(α, 2n), E=30 MeV; measured Eγ, Iγ, γγ-coin, and γγ(θ)(DCO), and γγ(lin pol)(IPDCO) using VENUS array of HPGe detectors at VECC-Kolkata cyclotron facility. 199Tl; deduced high-spin levels, J, π, bands, multipolarities, alignment and staggering plots, and configurations; calculated total Routhian surface (TRS) contours in (β2, γ) plane. Systematics of band structures in 193,195,197,199,201Tl.
doi: 10.1103/PhysRevC.98.044311
2018KU06 Eur.Phys.J. A 54, 63 (2018) S.Kundu, C.Bhattacharya, T.K.Rana, S.Bhattacharya, R.Pandey, K.Banerjee, P.Roy, J.K.Meena, G.Mukherjee, T.K.Ghosh, S.Mukhopadhyay, A.K.Saha, J.K.Sahoo, R.M.Saha, V.Srivastava, M.Sinha, M.A.Asgar Effect of clustering on the emission of light charged particles NUCLEAR REACTIONS 27Al(p, α), E=18 MeV; measured Eα, Iα(θ); deduced σ(Eα, θ); calculated σ(Eα, θ) using CASCADE code with RLDM values of spin-dependent deformation parameters; deduced critical angular momentum, deformation parameters; compared with published results for 15 heavy-ion reactions.
doi: 10.1140/epja/i2018-12494-5
2018SA07 Phys.Scr. 93, 034001 (2018) A.Saha, T.Bhattacharjee, D.Curien, I.Dedes, K.Mazurek, S.R.Banerjee, S.Rajbanshi, A.Bisoi, G.de Angelis, S.Bhattacharya, S.Bhattacharyya, S.Biswas, A.Chakraborty, S.Das Gupta, B.Dey, A.Goswami, D.Mondal, D.Pandit, R.Palit, T.Roy, R.P.Singh, M.S.Sarkar, S.Saha, J.Sethi Excited negative parity bands in 160Yb NUCLEAR REACTIONS 148Sm(16O, 4n)160Yb, E=90 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies, J, π, B(E2)/B(E1) ratios, non-yrast negative parity structures, bands. Comparison with energy calculation results obtained using the standard Woods-Saxon universal Hamiltonian.
doi: 10.1088/1402-4896/aaa1fa
2018SA22 Nucl.Phys. A976, 1 (2018) A.Saha, T.Bhattacharjee, S.S.Alam, D.Banerjee, M.S.Sarkar, S.Sarkar, J.B.Gupta, P.Das, S.Bhattacharya, D.Pandit, R.Guin, S.K.Das, S.R.Banerjee Spectroscopy of low lying states in 150Sm NUCLEAR REACTIONS 150Nd(p, n)150Sm, E=8.0 MeV; measured Eγ, Iγ, γγ-coin using VENUS array of six Compton-suppressed Clover HPGe. 150Sm deduced γ transitions, levels, J, π, spin and parity using NNDC logft calculator and angular correlations; estimated possible M2 admixture, B(E1).
doi: 10.1016/j.nuclphysa.2018.05.005
2017AL45 Nucl.Instrum.Methods Phys.Res. A874, 103 (2017) S.S.Alam, T.Bhattacharjee, D.Banerjee, A.Saha, D.Pandit, D.Mondal, S.Mukhopadhyay, S.Pal, P.Bhaskar, S.K.Das, S.R.Banerjee VECC array for Nuclear fast Timing and angUlar corRElation studies (VENTURE) RADIOACTIVITY 132Te(β-) [ from 238U(α, F), E not given]; measured decay products, Eγ, Iγ; deduced γ-ray energies, angular correlations. RADIOACTIVITY 60Ni, 106Pd, 133Cs(IT); measured decay products, Eγ, Iγ; deduced γ-ray energies, level T1/2. Comparison with a Monte Carlo simulation with GEANT3 package.
doi: 10.1016/j.nima.2017.08.037
2017SR04 Int.J.Mod.Phys. E26, 1750064 (2017) V.Srivastava, C.Bhattacharya, T.K.Rana, S.Manna, S.Kundu, S.Bhattacharya, K.Banerjee, P.Roy, R.Pandey, G.Mukherjee, T.K.Ghosh, J.K.Meena, T.Roy, A.Chaudhuri, M.Sinha, A.K.Saha, Md.A.Asgar, A.Dey, S.Roy, Md.M.Shaikh Study of 26Mg through 1p pick-up reaction 27Al(d, 3He) NUCLEAR REACTIONS 27Al(d, 3He), E=25 MeV; measured reaction products; deduced excitation energy spectra, σ(θ), spectroscopic factors. Comparison with DWBA calculations.
doi: 10.1142/S0218301317500641
2016RO31 Phys.Rev. C 94, 064607 (2016) P.Roy, K.Banerjee, C.Bhattacharya, R.Pandey, A.Sen, S.Manna, S.Kundu, T.K.Rana, T.K.Ghosh, G.Mukherjee, T.Roy, A.Dhal, A.Dey, J.K.Meena, A.K.Saha, D.Pandit, S.Mukhopadhyay, S.Bhattacharya Excitation energy dependence of the level density parameter close to the doubly magic 208Pb NUCLEAR REACTIONS 208Pb, 209Bi(α, n), E=28, 31, 35, 40, 60 MeV; measured E(n), I(n), σ(θ, E), time-of-flight at Variable Energy Cyclotron Centre (VECC); deduced shell-damping parameter, inverse level density parameters and temperatures. Comparison with the Thomas-Fermi model predictions.
doi: 10.1103/PhysRevC.94.064607
2016SR02 Phys.Rev. C 93, 044601 (2016) V.Srivastava, C.Bhattacharya, T.K.Rana, S.Manna, S.Kundu, S.Bhattacharya, K.Banerjee, P.Roy, R.Pandey, G.Mukherjee, T.K.Ghosh, J.K.Meena, T.Roy, A.Chaudhuri, M.Sinha, A.K.Saha, Md.A.Asgar, A.Dey, S.Roy, Md.M.Shaikh Experimental investigation of T=1 analog states of 26Al and 26Mg NUCLEAR REACTIONS 27Al(d, 3He)26Mg, E=25 MeV; measured 3He spectra, σ(θ) at VECC, Kolkata. 26Mg; deduced levels, J, π, spectroscopic factors of the lowest (T=1) states using zero-range distorted wave Born approximation. Comparison with T=1 analog states in 26Al.
doi: 10.1103/PhysRevC.93.044601
2015BA10 Phys.Rev. C 91, 024617 (2015) D.Banerjee, A.Saha, T.Bhattacharjee, R.Guin, S.K.Das, P.Das, D.Pandit, A.Mukherjee, A.Chowdhury, S.Bhattacharya, S.Das Gupta, S.Bhattacharyya, P.Mukhopadhyay, S.R.Banerjee Role of p-induced population of medium-mass (A∼150) neutron-rich nuclei NUCLEAR REACTIONS 150Nd(p, n), (p, 2n), (p, p'n), (p, d), E=7-15 MeV; measured Eγ, Iγ, σ(E), half-lives by activation method using K=130 AVF cyclotron at VECC facility. Comparison with previous experimental results, and with model calculations using CASCADE, ALICE, and EMPIRE3.1 computer codes. RADIOACTIVITY 149Nd, 149,150Pm(β-); measured Eγ, Iγ, ground state half-lives of 149Nd, 149,150Pm.
doi: 10.1103/PhysRevC.91.024617
2015CH55 Phys.Rev. C 92, 041601 (2015) A.Chaudhuri, T.K.Ghosh, K.Banerjee, S.Bhattacharya, J.Sadhukhan, S.Kundu, C.Bhattacharya, J.K.Meena, G.Mukherjee, A.K.Saha, Md.A.Asgar, A.Dey, S.Manna, R.Pandey, T.K.Rana, P.Roy, T.Roy, V.Srivastava, P.Bhattacharya, D.C.Biswas, B.N.Joshi, K.Mahata, A.Shrivastava, R.P.Vind, S.Pal, B.R.Behera, V.Singh No influence of a N=126 neutron-shell closure in fission-fragment mass distributions NUCLEAR REACTIONS 194Pt(12C, F)206Po*, 198Pt(12C, F)210Po*, E=58-78 MeV; measured fission fragment spectra, distributions of folding angles and mass distributions of complementary fission fragments using multi-wire proportional counters (MWPC) at BARC-TIFR Pelletron facility; deduced effect of shell correction in the saddle ridge on the mass distribution of fission fragments, no evidence for the modification of potential energy surface at the saddle point due to N=126 neutron shell closure in 210Po.
doi: 10.1103/PhysRevC.92.041601
2015SR03 Phys.Rev. C 91, 054611 (2015) V.Srivastava, C.Bhattacharya, T.K.Rana, S.Manna, S.Kundu, S.Bhattacharya, K.Banerjee, P.Roy, R.Pandey, G.Mukherjee, T.K.Ghosh, J.K.Meena, T.Roy, A.Chaudhuri, M.Sinha, A.Saha, Md.A.Asgar, A.Dey, S.Roy, Md.M.Shaikh Experimental study of 26Al through the 1n pick-up reaction 27Al(d, t) NUCLEAR REACTIONS 27Al(d, t), E=25 MeV; measured E(t), I(t), σ(θ) at VECC-Kolkata facility. 26Al; deduced levels, J, π, spectroscopic factors. DWBA calculations using DWUCK4 computer code. Comparison with experimental results from other particle-transfer experiments.
doi: 10.1103/PhysRevC.91.054611
2014BH17 Nucl.Instrum.Methods Phys.Res. A767, 19 (2014) T.Bhattacharjee, D.Pandit, S.K.Das, A.Chowdhury, P.Das, D.Banerjee, A.Saha, S.Mukhopadhyay, S.Pal, S.R.Banerjee Measurement of β-decay end point energy with planar HPGe detector RADIOACTIVITY 106Rh(β-); measured Eβ, Iβ, βγ-coin; deduced β end-point energies using planar HPGe detectors.
doi: 10.1016/j.nima.2014.08.008
2014KA30 Phys.Rev.Lett. 113, 022502 (2014) J.Katich, X.Qian, Y.X.Zhao, K.Allada, K.Aniol, J.R.M.Annand, T.Averett, F.Benmokhtar, W.Bertozzi, P.C.Bradshaw, P.Bosted, A.Camsonne, M.Canan, G.D.Cates, C.Chen, J.-P.Chen, W.Chen, K.Chirapatpimol, E.Chudakov, E.Cisbani, J.C.Cornejo, F.Cusanno, M.M.Dalton, W.Deconinck, C.W.de Jager, R.De Leo, X.Deng, A.Deur, H.Ding, P.A.M.Dolph, C.Dutta, D.Dutta, L.El Fassi, S.Frullani, H.Gao, F.Garibaldi, D.Gaskell, S.Gilad, R.Gilman, O.Glamazdin, S.Golge, L.Guo, D.Hamilton, O.Hansen, D.W.Higinbotham, T.Holmstrom, J.Huang, M.Huang, H.F.Ibrahim, M.Iodice, X.Jiang, G.Jin, M.K.Jones, A.Kelleher, W.Kim, A.Kolarkar, W.Korsch, J.J.LeRose, X.Li, Y.Li, R.Lindgren, N.Liyanage, E.Long, H.-J.Lu, D.J.Margaziotis, P.Markowitz, S.Marrone, D.McNulty, Z.-E.Meziani, R.Michaels, B.Moffit, C.Munoz Camacho, S.Nanda, A.Narayan, V.Nelyubin, B.Norum, Y.Oh, M.Osipenko, D.Parno, J.C.Peng, S.K.Phillips, M.Posik, A.J.R.Puckett, Y.Qiang, A.Rakhman, R.D.Ransome, S.Riordan, A.Saha, B.Sawatzky, E.Schulte, A.Shahinyan, M.H.Shabestari, S.Sirca, S.Stepanyan, R.Subedi, V.Sulkosky, L.-G.Tang, A.Tobias, G.M.Urciuoli, I.Vilardi, K.Wang, Y.Wang, B.Wojtsekhowski, X.Yan, H.Yao, Y.Ye, Z.Ye, L.Yuan, X.Zhan, Y.Zhang, Y.-W.Zhang, B.Zhao, X.Zheng, L.Zhu, X.Zhu, X.Zong Measurement of the Target-Normal Single-Spin Asymmetry in Deep-Inelastic Scattering from the Reaction 3He ↑ (e, e')X
doi: 10.1103/PhysRevLett.113.022502
2014MO25 J.Phys.(London) G41, 105109 (2014) P.Monaghan, R.Shneor, R.Subedi, B.D.Anderson, K.Aniol, J.Annand, J.Arrington, H.B.Benaoum, F.Benmokhtar, P.Bertin, W.Bertozzi, W.Boeglin, J.P.Chen, S.Choi, E.Chudakov, C.Ciofi degli Atti, E.Cisbani, W.Cosyn, B.Craver, C.W.de Jager, R.J.Feuerbach, E.Folts, S.Frullani, F.Garibaldi, O.Gayou, S.Gilad, R.Gilman, O.Glamazdin, J.Gomez, O.Hansen, D.W.Higinbotham, T.Holmstrom, H.Ibrahim, R.Igarashi, E.Jans, X.Jiang, L.Kaufman, A.Kelleher, A.Kolarkar, E.Kuchina, G.Kumbartzki, J.J.LeRose, R.Lindgren, N.Liyanage, D.J.Margaziotis, P.Markowitz, S.Marrone, M.Mazouz, D.Meekins, R.Michaels, B.Moffit, H.Morita, S.Nanda, C.F.Perdrisat, E.Piasetzky, M.Potokar, V.Punjabi, Y.Qiang, J.Reinhold, B.Reitz, G.Ron, G.Rosner, J.Ryckebusch, A.Saha, B.Sawatzky, J.Segal, A.Shahinyan, S.Sirca, K.Slifer, P.Solvignon, V.Sulkosky, N.Thompson, P.E.Ulmer, G.M.Urciuoli, E.Voutier, K.Wang, J.W.Watson, L.B.Weinstein, B.Wojtsekhowski, S.Wood, H.Yao, X.Zheng, L.Zhu Measurement of the 12C(e, e'p)11B two-body breakup reaction at high missing momentum NUCLEAR REACTIONS 12C(E, E'P), E200-400 MeV; measured reaction products, Ep, Ip; deduced σ(θ, E). Comparison with WS+Glauber calculations.
doi: 10.1088/0954-3899/41/10/105109
2013RA20 Phys.Rev. C 88, 021601 (2013); Pub.note Phys.Rev. C 88, 029904 (2013) T.K.Rana, S.Bhattacharya, C.Bhattacharya, S.Kundu, K.Banerjee, T.K.Ghosh, G.Mukherjee, R.Pandey, P.Roy, V.Srivastava, M.Gohil, J.K.Meena, H.Pai, A.K.Saha, J.K.Sahoo, R.M.Saha Estimation of direct components of the decay of the Hoyle state NUCLEAR REACTIONS 12C(α, α'), E=60 MeV; measured α spectra at VECC, Kolkata facility. High statistics experiment for complete kinematical measurement. Dalitz plot. 12C; deduced contribution of direct 3α decay mechanisms (DDE, DDL, DDΦ) of decay of Hoyle state, nonzero branching ratios for direct decay in phase space (DDΦ mode). Comparison with previous experimental results.
doi: 10.1103/PhysRevC.88.021601
2012CO25 J.Phys.:Conf.Ser. 381, 012101 (2012) J.C.Cornejo, J.L.Herraiz, A.Camsonne, A.Saha, J.M.Udias, G.Urciuoli, J.R.Vignote, K.A.Aniol, for the Jefferson Lab Hall A Collaboration Quasi elastic cross sections for the 209Bi(e, e'p)208Pb reaction: Jefferson Lab experiment E06007 NUCLEAR REACTIONS 209Bi(e, e'p), E=2.652 GeV; measured reaction products; deduced σ(θ). Compared with RDWIA calculations of Madrid group.
doi: 10.1088/1742-6596/381/1/012101
2006HU09 Phys.Rev. C 73, 064004 (2006) B.Hu, M.K.Jones, P.E.Ulmer, H.Arenhovel, O.K.Baker, W.Bertozzi, E.J.Brash, J.Calarco, J.-P.Chen, E.Chudakov, A.Cochran, S.Dumalski, R.Ent, J.M.Finn, F.Garibaldi, S.Gilad, R.Gilman, C.Glashausser, J.Gomez, V.Gorbenko, J.-O.Hansen, J.Hovdebo, C.W.de Jager, S.Jeschonnek, X.Jiang, C.Keppel, A.Klein, A.Kozlov, S.Kuhn, G.Kumbartzki, M.Kuss, J.J.LeRose, M.Liang, N.Liyanage, G.J.Lolos, P.E.C.Markowitz, D.Meekins, R.Michaels, J.Mitchell, Z.Papandreou, C.F.Perdrisat, V.Punjabi, R.Roche, D.Rowntree, A.Saha, S.Strauch, L.Todor, G.Urciuoli, L.B.Weinstein, K.Wijesooriya, B.B.Wojtsekhowski, R.Woo Polarization transfer in the 2H(e(pol), e'p(pol))n reaction up to Q2 = 1.61 (GeV/c)2 NUCLEAR REACTIONS 1,2H(polarized e, e'p), E=1.669 GeV; measured recoil proton polarization vs momentum transfer, missing momentum; deduced form factor ratios. Comparison with model predictions.
doi: 10.1103/PhysRevC.73.064004
2005QA01 Phys.Rev.Lett. 94, 142301 (2005) I.A.Qattan, J.Arrington, R.E.Segel, X.Zheng, K.Aniol, O.K.Baker, R.Beams, E.J.Brash, J.Calarco, A.Camsonne, J.-P.Chen, M.E.Christy, D.Dutta, R.Ent, S.Frullani, D.Gaskell, O.Gayou, R.Gilman, C.Glashausser, K.Hafidi, J.-O.Hansen, D.W.Higinbotham, W.Hinton, R.J.Holt, G.M.Huber, H.Ibrahim, L.Jisonna, M.K.Jones, C.E.Keppel, E.Kinney, G.J.Kumbartzki, A.Lung, D.J.Margaziotis, K.McCormick, D.Meekins, R.Michaels, P.Monaghan, P.Moussiegt, L.Pentchev, C.Perdrisat, V.Punjabi, R.Ransome, J.Reinhold, B.Reitz, A.Saha, A.Sarty, E.C.Schulte, K.Slifer, P.Solvignon, V.Sulkosky, K.Wijesooriya, B.Zeidman Precision Rosenbluth Measurement of the Proton Elastic Form Factors NUCLEAR REACTIONS 1H(e, e), E=1.9-4.7 GeV; measured recoil proton spectra, σ(θ), σ. 1H deduced electromagnetic form factors.
doi: 10.1103/PhysRevLett.94.142301
2005SA12 Eur.Phys.J. A 24, Supplement 1, 81 (2005) A.Saha, for the Hall A Collaboration Detailed study of the few nucleon systems with (e, e'p) reactions NUCLEAR REACTIONS 3He(e, e'p), E=4.8 GeV; measured σ(E, θ), asymmetries. 3He deduced bound state momentum distributions. Comparisons with model predictions.
doi: 10.1140/epjad/s2005-05-013-y
2003SA69 Mod.Phys.Lett. A 18, 235 (2003) A.Saha, for the Jefferson Lab Hall A Collaboration Detailed study of the few nucleon systems at Jefferson Lab NUCLEAR REACTIONS 2H, 3He(e, e'p), E=4.8 GeV; measured σ(E, θ), asymmetry. Comparison with model predictions.
doi: 10.1142/S0217732303010284
2003ST13 Phys.Rev.Lett. 91, 052301 (2003) S.Strauch, S.Dieterich, K.A.Aniol, J.R.M.Annand, O.K.Baker, W.Bertozzi, M.Boswell, E.J.Brash, Z.Chai, J.-P.Chen, M.E.Christy, E.Chudakov, A.Cochran, R.De Leo, R.Ent, M.B.Epstein, J.M.Finn, K.G.Fissum, T.A.Forest, S.Frullani, F.Garibaldi, A.Gasparian, O.Gayou, S.Gilad, R.Gilman, C.Glashausser, J.Gomez, V.Gorbenko, P.L.J.Gueye, J.O.Hansen, D.W.Higinbotham, B.Hu, C.E.Hyde-Wright, D.G.Ireland, C.Jackson, C.W.de Jager, X.Jiang, C.Jones, M.K.Jones, J.D.Kellie, J.J.Kelly, C.E.Keppel, G.Kumbartzki, M.Kuss, J.J.LeRose, K.Livingston, N.Liyanage, S.Malov, D.J.Margaziotis, D.Meekins, R.Michaels, J.H.Mitchell, S.K.Nanda, J.Nappa, C.F.Perdrisat, V.A.Punjabi, R.D.Ransome, R.Roche, G.Rosner, M.Rvachev, F.Sabatie, A.Saha, A.Sarty, J.M.Udias, P.E.Ulmer, G.M.Urciuoli, J.F.J.van den Brand, J.R.Vignote, D.P.Watts, L.B.Weinstein, K.Wijesooriya, B.Wojtsekhowski Polarization Transfer in the 4He(e(pol), e'p(pol))3H Reaction up to Q2=2.6 (GeV/c)2 NUCLEAR REACTIONS 4He(polarized e, e'p), E=3400, 4237, 4239 MeV; measured polarization transfer; deduced medium modification effects. Comparison with model predictions.
doi: 10.1103/PhysRevLett.91.052301
2003XU02 Phys.Rev. C 67, 012201 (2003) W.Xu, B.Anderson, L.Auberbach, T.Averett, W.Bertozzi, T.Black, J.Calarco, L.Cardman, G.D.Cates, Z.W.Chai, J.P.Chen, S.Choi, E.Chudakov, S.Churchwell, G.S.Corrado, C.Crawford, D.Dale, A.Deur, P.Djawotho, T.W.Donnelly, D.Dutta, J.M.Finn, H.Gao, R.Gilman, A.V.Glamazdin, C.Glashausser, W.Glockle, J.Golak, J.Gomez, V.G.Gorbenko, J.-O.Hansen, F.W.Hersman, D.W.Higinbotham, R.Holmes, C.R.Howell, E.Hughes, B.Humensky, S.Incerti, C.W.de Jager, J.S.Jensen, X.Jiang, C.E.Jones, M.Jones, R.Kahl, H.Kamada, A.Kievsky, I.Kominis, W.Korsch, K.Kramer, G.Kumbartzki, M.Kuss, E.Lakuriqi, M.Liang, N.Liyanage, J.LeRose, S.Malov, D.J.Margaziotis, J.W.Martin, K.McCormick, R.D.McKeown, K.McIlhany, Z.-E.Meziani, R.Michaels, G.W.Miller, J.Mitchell, S.Nanda, E.Pace, T.Pavlin, G.G.Petratos, R.I.Pomatsalyuk, D.Pripstein, D.Prout, R.D.Ransome, Y.Roblin, M.Rvachev, A.Saha, G.Salme, M.Schnee, T.Shin, K.Slifer, P.A.Souder, S.Strauch, R.Suleiman, M.Sutter, B.Tipton, L.Todor, M.Viviani, B.Vlahovic, J.Watson, C.F.Williamson, H.Witala, B.Wojtsekhowski, F.Xiong, J.Yeh, P.Zolnierczuk Plane-wave impulse approximation extraction of the neutron magnetic form factor from quasielastic 3He(pol)(e(pol), e') at Q2 = 0.3 to 0.6 (GeV/c)2 NUCLEAR REACTIONS 3He(polarized e, e'), E=0.778, 1.727 GeV; measured transverse spin-dependent asymmetry. 1n deduced magnetic form factor. Polarized target.
doi: 10.1103/PhysRevC.67.012201
2002SC41 Phys.Rev. C66, 042201 (2002) E.C.Schulte, A.Afanasev, M.Amarian, K.Aniol, S.Becher, K.Benslama, L.Bimbot, P.Bosted, E.Brash, J.Calarco, Z.Chai, C.Chang, T.Chang, J.P.Chen, S.Choi, E.Chudakov, S.Churchwell, D.Crovelli, S.Dieterich, S.Dumalski, D.Dutta, M.Epstein, K.Fissum, B.Fox, S.Frullani, H.Gao, J.Gao, F.Garibaldi, O.Gayou, R.Gilman, A.Glamazdin, C.Glashausser, J.Gomez, V.Gorbenko, J.-O.Hansen, R.J.Holt, J.Hovdebo, G.M.Huber, C.W.de Jager, X.Jiang, C.Jones, M.K.Jones, J.Kelly, E.Kinney, E.Kooijman, G.Kumbartzki, M.Kuss, J.LeRose, M.Liang, R.Lindgren, N.Liyanage, S.Malov, D.Margaziotis, P.Markowitz, K.McCormick, D.Meekins, Z.-E.Meziani, R.Michaels, J.Mitchell, L.Morand, C.Perdrisat, R.Pomatsalyuk, V.Punjabi, A.Radyushkin, R.Ransome, R.Roche, M.Rvachev, A.Saha, A.Sarty, D.Simon, S.Strauch, R.Suleiman, L.Todor, P.Ulmer, G.M.Urciuoli, K.Wijesooriya, B.Wojtsekhowski, F.Xiong, W.Xu High energy angular distribution measurements of the exclusive deuteron photodisintegration reaction NUCLEAR REACTIONS 2H(γ, p), E=1.6, 1.9, 2.4 GeV; measured σ(θ), forward-backward asymmetry. Comparison with model predictions.
doi: 10.1103/PhysRevC.66.042201
2002UL01 Phys.Rev.Lett. 89, 062301 (2002) P.E.Ulmer, K.A.Aniol, H.Arenhovel, J.-P.Chen, E.Chudakov, D.Crovelli, J.M.Finn, K.G.Fissum, O.Gayou, J.Gomez, J.-O.Hansen, C.W.de Jager, S.Jeschonnek, M.K.Jones, M.Kuss, J.J.LeRose, M.Liang, R.A.Lindgren, S.Malov, D.Meekins, R.Michaels, J.Mitchell, C.F.Perdrisat, V.Punjabi, R.Roche, F.Sabatie, A.Saha, R.Suleiman, L.Todor, B.B.Wojtsekhowski 2H(e, e'p)n Reaction at High Recoil Momenta NUCLEAR REACTIONS 2H(e, e'p), E=3.110 GeV; measured Ep, σ vs recoil momentum. Comparison with model predictions.
doi: 10.1103/PhysRevLett.89.062301
2001SC37 Phys.Rev.Lett. 87, 102302 (2001) E.C.Schulte, A.Ahmidouch, C.S.Armstrong, J.Arrington, R.Asaturyan, S.Avery, O.K.Baker, D.H.Beck, H.P.Blok, C.W.Bochna, W.Boeglin, P.Y.Bosted, M.Bouwhuis, H.Breuer, D.S.Brown, A.Bruell, R.V.Cadman, R.Carlini, N.S.Chant, A.Cochran, L.Cole, S.Danagoulian, D.B.Day, J.A.Dunne, D.Dutta, R.Ent, H.C.Fenker, B.Fox, L.Gan, H.Gao, K.Garrow, D.Gaskell, A.Gasparian, D.F.Geesaman, R.Gilman, C.Glashausser, P.Gueye, M.Harvey, R.J.Holt, H.E.Jackson, X.Jiang, C.E.Keppel, E.R.Kinney, Y.Liang, W.Lorenzon, A.F.Lung, D.J.Mack, P.E.Markowitz, J.Martin, K.McIlhany, D.McKee, D.G.Meekins, M.A.Miller, R.G.Milner, J.H.Mitchell, H.Mkrtchyan, B.A.Mueller, A.M.Nathan, G.Niculescu, I.Niculescu, T.G.O'Neill, V.Papavassiliou, S.F.Pate, R.B.Piercey, D.H.Potterveld, R.D.Ransome, J.Reinhold, E.Rollinde, P.Roos, A.Saha, A.J.Sarty, R.Sawafta, E.Segbefia, T.Shin, S.Stepanyan, S.Strauch, M.F.Sutter, V.Tadevosyan, L.Tang, R.Tieulent, A.Uzzle, W.F.Vulcan, S.A.Wood, F.Xiong, L.Yuan, M.Zeier, B.Zihlmann, V.Ziskin Measurement of the High Energy Two-Body Deuteron Photodisintegration Differential Cross Section NUCLEAR REACTIONS 2H(γ, p), E < 5.5 GeV; measured σ(E, θ); deduced angle-dependent scaling threshold.
doi: 10.1103/PhysRevLett.87.102302
2001XI04 Phys.Rev.Lett. 87, 242501 (2001) F.Xiong, D.Dutta, W.Xu, B.Anderson, L.Auberbach, T.Averett, W.Bertozzi, T.Black, J.Calarco, L.Cardman, G.D.Cates, Z.W.Chai, J.P.Chen, S.Choi, E.Chudakov, S.Churchwell, G.S.Corrado, C.Crawford, D.Dale, A.Deur, P.Djawotho, B.W.Filippone, J.M.Finn, H.Gao, R.Gilman, A.V.Glamazdin, C.Glashausser, W.Glockle, J.Golak, J.Gomez, V.G.Gorbenko, J.-O.Hansen, F.W.Hersman, D.W.Higinbotham, R.Holmes, C.R.Howell, E.Hughes, B.Humensky, S.Incerti, C.W.de Jager, J.S.Jensen, X.Jiang, C.E.Jones, M.Jones, R.Kahl, H.Kamada, A.Kievsky, I.Kominis, W.Korsch, K.Kramer, G.Kumbartzki, M.Kuss, E.Lakuriqi, M.Liang, N.Liyanage, J.LeRose, S.Malov, D.J.Margaziotis, J.W.Martin, K.McCormick, R.D.McKeown, K.McIlhany, Z.-E.Meziani, R.Michaels, G.W.Miller, E.Pace, T.Pavlin, G.G.Petratos, R.I.Pomatsalyuk, D.Pripstein, D.Prout, R.D.Ransome, Y.Roblin, M.Rvachev, A.Saha, G.Salme, M.Schnee, T.Shin, K.Slifer, P.A.Souder, S.Strauch, R.Suleiman, M.Sutter, B.Tipton, L.Todor, M.Viviani, B.Vlahovic, J.Watson, C.F.Williamson, H.Witala, B.Wojtsekhowski, J.Yeh, P.Zolnierczuk Precision Measurement of the Spin-Dependent Asymmetry in the Threshold Region of 3He(pol)(e(pol), e') NUCLEAR REACTIONS 3He(polarized e, e'), E=0.778, 1.727 GeV; measured spin-dependent asymmetry. Polarized target, comparison with model predictions.
doi: 10.1103/PhysRevLett.87.242501
2000XU07 Phys.Rev.Lett. 85, 2900 (2000) W.Xu, D.Dutta, F.Xiong, B.Anderson, L.Auberbach, T.Averett, W.Bertozzi, T.Black, J.Calarco, L.Cardman, G.D.Cates, Z.W.Chai, J.P.Chen, S.Choi, E.Chudakov, S.Churchwell, G.S.Corrado, C.Crawford, D.Dale, A.Deur, P.Djawotho, B.W.Filippone, J.M.Finn, H.Gao, R.Gilman, A.V.Glamazdin, C.Glashausser, W.Glockle, J.Golak, J.Gomez, V.G.Gorbenko, J.-O.Hansen, F.W.Hersman, D.W.Higinbotham, R.Holmes, C.R.Howell, E.Hughes, B.Humensky, S.Incerti, C.W.de Jager, J.S.Jensen, X.Jiang, C.E.Jones, M.Jones, R.Kahl, H.Kamada, A.Kievsky, I.Kominis, W.Korsch, K.Kramer, G.Kumbartzki, M.Kuss, E.Lakuriqi, M.Liang, N.Liyanage, J.LeRose, S.Malov, D.J.Margaziotis, J.W.Martin, K.McCormick, R.D.McKeown, K.McIlhany, Z.-E.Meziani, R.Michaels, G.W.Miller, E.Pace, T.Pavlin, G.G.Petratos, R.I.Pomatsalyuk, D.Pripstein, D.Prout, R.D.Ransome, Y.Roblin, M.Rvachev, A.Saha, G.Salme, M.Schnee, T.Shin, K.Slifer, P.A.Souder, S.Strauch, R.Suleiman, M.Sutter, B.Tipton, L.Todor, M.Viviani, B.Vlahovic, J.Watson, C.F.Williamson, H.Witala, B.Wojtsekhowski, J.Yeh, P.Zolnierczuk Transverse Asymmetry AT' from the Quasielastic 3He(pol)(e(pol), e') Process and the Neutron Magnetic Form Factor NUCLEAR REACTIONS 3He(polarized e, e'), E=0.778, 1.727 GeV; measured transverse asymmetry. 1n deduced magnetic form factor. Polarized target.
doi: 10.1103/PhysRevLett.85.2900
1999GL06 Fizika(Zagreb) B8, 91 (1999) A.V.Glamazdin, V.G.Gorbenko, L.G.Levchuk, R.I.Pomatsalyuk, A.L.Rubashkin, P.V.Sorokin, D.S.Dale, B.Doyle, T.Gorringe, W.Korsch, V.Zeps, J.P.Chen, E.Chudakov, S.Nanda, A.Saha, A.Gasparian Electron Beam Moller Polarimeter at JLab Hall A
1995SE03 Phys.Rev.Lett. 74, 642 (1995); Erratum Phys.Rev.Lett. 74, 3306 (1995) K.K.Seth, R.Soundranayagam, A.Saha, C.W.de Jager, H.de Vries, B.A.Brown, B.H.Wildenthal Absence of M3 Quenching in 26Mg NUCLEAR REACTIONS 26Mg(e, e'), E not given; measured σ(θ). 26Mg level deduced B(λ).
doi: 10.1103/PhysRevLett.74.642
1994BU09 Phys.Rev. C49, 2226 (1994) G.Burleson, G.Blanpied, W.Cottingame, G.Daw, B.Park, K.K.Seth, D.Barlow, S.Iversen, M.Kaletka, H.Nann, A.Saha, D.Smith, R.P.Redwine, W.Burger, M.Farkhondeh, B.Saghai, R.Anderson Negative Pion-Nucleus Elastic Scattering at 20 and 40 MeV NUCLEAR REACTIONS 12C, 16O, 48Ca, 90Zr, 208Pb(π-, π-), E=20 MeV; 12C, 16,18O, 40Ca, 58Ni, 208Pb(π-, π-), E=40 MeV; measured σ(θ); deduced optical model parameters. Range telescope.
doi: 10.1103/PhysRevC.49.2226
1994FE05 Phys.Rev. C49, 2068 (1994) A.E.Feldman, J.J.Kelly, B.S.Flanders, M.A.Khandaker, H.Seifert, P.Boberg, S.D.Hyman, P.H.Karen, B.E.Norum, P.Welch, Q.Chen, A.D.Bacher, G.P.A.Berg, E.J.Stephenson, S.Nanda, A.Saha, A.Scott Neutron Transition Densities for 48Ca from Proton Scattering at 200 and 318 MeV NUCLEAR REACTIONS 48Ca(polarized p, p'), (polarized p, p), E=200, 318 MeV; measured σ(θ), analyzing power vs θ. 48Ca levels deduced nucleon transition densities, multipole moments. Extended random phase approximation.
doi: 10.1103/PhysRevC.49.2068
1991CH39 Phys.Rev.Lett. 67, 568 (1991) L.Chinitz, M.Bernheim, G.P.Capitani, A.Catarinella, J.F.Danel, E.De Sanctis, S.Frullani, F.Garibaldi, F.Ghio, M.Iodice, L.Lakehal-Ayat, J.M.Le Goff, J.LeRose, A.Magnon, C.Marchand, R.Minehart, J.Morgenstern, J.Mougey, S.Nanda, C.Perdrisat, R.Powers, V.Punjabi, A.Saha, P.Ulmer, P.Vernin Separation of the Interference Response Function R(LT) in the 16O(e, e'p)15N Reaction NUCLEAR REACTIONS 16O(e, e'p), E=580 MeV; measured σ(θ(e'), E(e'), θp') vs recoil momentum. 15N levels deduced nuclear response function, momentum distribution, spectroscopic factor strength depletion. Relativistic DWIA.
doi: 10.1103/PhysRevLett.67.568
1991KE09 Phys.Rev. C44, 1963 (1991) J.J.Kelly, M.A.Khandaker, P.Boberg, A.E.Feldman, B.S.Flanders, S.Hyman, H.Seifert, P.Karen, B.E.Norum, P.Welch, S.Nanda, A.Saha Neutron and Proton Transition Densities from 32,34S(p, p') at E(p) = 318 MeV. I. Isoscalar Densities for 32S NUCLEAR REACTIONS 32,34S(polarized p, p'), E=318 MeV; measured σ(θ), analyzing powers. 32S levels deduced isoscalar transition densities. DWIA analysis. Shell model.
doi: 10.1103/PhysRevC.44.1963
1991KE13 Phys.Rev. C44, 2602 (1991) J.J.Kelly, P.Boberg, A.E.Feldman, B.S.Flanders, M.A.Khandaker, S.D.Hyman, H.Seifert, P.Karen, B.E.Norum, P.Welch, S.Nanda, A.Saha Effective Interaction for 40Ca(p, p') at E(p) = 318 MeV NUCLEAR REACTIONS 40Ca(polarized p, p'), (polarized p, p), E=318 MeV; measured σ(θ), analyzing power vs θ; deduced nucleon-nucleon effective interaction. Dirac phenomenology, global optical potentials.
doi: 10.1103/PhysRevC.44.2602
1991KH06 Phys.Rev. C44, 1978 (1991) M.A.Khandaker, J.J.Kelly, P.Boberg, A.E.Feldman, B.S.Flanders, S.Hyman, H.Seifert, P.Karen, B.E.Norum, P.Welch, S.Nanda, A.Saha Neutron and Proton Transition Densities from 32,34S(p, p') at E(p) = 318 MeV. II. Neutron Densities for 34S NUCLEAR REACTIONS 32,34S(polarized p, p'), E=318 MeV; measured σ(θ), analyzing powers. 34S levels deduced isoscalar transition densities, neutron, proton transition matrix elements ratio. DWIA analysis. Shell model.
doi: 10.1103/PhysRevC.44.1978
1989EN01 Phys.Rev.Lett. 62, 24 (1989) R.Ent, B.L.Berman, H.P.Blok, J.F.J.van den Brand, W.J.Briscoe, E.Jans, G.J.Kramer, J.B.J.M.Lanen, L.Lapikas, B.E.Norum, E.N.M.Quint, A.Saha, G.van der Steenhoven, P.K.A.de Witt Huberts Deuteron Formation in the Reaction 12C(e, e'd)10B(T = 1) NUCLEAR REACTIONS 12C(e, e'd), E=466 MeV; measured σ(θ(e'), E(e'), θd) vs excitation. 10B deduced T=0, T=1 relative level excitation, mechanism.
doi: 10.1103/PhysRevLett.62.24
1988BA14 Phys.Rev. C37, 1977 (1988) D.B.Barlow, A.Saha, K.K.Seth, T.S.Bhatia, G.Glass, J.C.Hiebert, R.A.Kenefick, S.Nath, L.C.Northcliffe, W.B.Tippens, J.J.Jarmer, J.E.Simmons, R.H.Jeppesen, G.E.Tripard Measurement of the Spin Correlation Parameters A(ll) and A(sl) for the Reaction pp → dπ+ in the Energy Region 500-800 MeV NUCLEAR REACTIONS 1H(polarized p, π+), E=500-800 MeV; measured spin correlation parameters; deduced no dibaryon resonances. Coupled-channels, partial wave analyses. Polarized target.
doi: 10.1103/PhysRevC.37.1977
1988SO09 Phys.Lett. 212B, 13 (1988) R.Soundranayagam, A.Saha, K.K.Seth, C.W.de Jager, H.de Vries, H.Blok, G.van der Steenhoven Ground State Charge Distribution of 26Mg NUCLEAR REACTIONS 26Mg(e, e), E=85-360 MeV; measured σ(θ); deduced form factors. 26Mg deduced charge density, rms charge radius.
doi: 10.1016/0370-2693(88)91227-0
1987KA45 Phys.Lett. 199B, 336 (1987) M.Kaletka, K.K.Seth, A.Saha, D.Barlow, D.Kielczewska Correlation Effects in Pion Double Charge Exchange in the f7/2 Shell NUCLEAR REACTIONS 48Ca, 48Ti(π+, π-), E=130, 180, 235, 292 MeV; measured σ(E(π)). 48Ti, 48Cr deduced analog, nonanalog transition σ ratios.
doi: 10.1016/0370-2693(87)90929-4
1986EN05 Phys.Rev.Lett. 57, 2367 (1986) R.Ent, H.P.Blok, J.F.A.van Hienen, G.van der Steenhoven, J.F.J.van den Brand, J.W.A.den Herder, E.Jans, P.H.M.Keizer, L.Lapikas, E.N.M.Quint, P.K.A.de Witt Huberts, B.L.Berman, W.J.Briscoe, C.T.Christou, D.R.Lehman, B.E.Norum, A.Saha Reaction 6Li(e, e'd)4He and the α-d Momentum Distribution in the Ground State of 6Li NUCLEAR REACTIONS 6Li(e, e'd), E=480 MeV; measured missing mass spectrum, σ(θ(e'), E(e'), θd) vs momentum transfer, α-d momentum distribution; deduced reaction mechanism. Partial kinematics, enriched target. DWIA analysis, α-nucleon-nucleon model.
doi: 10.1103/PhysRevLett.57.2367
1986SE04 Phys.Lett. 173B, 397 (1986) K.K.Seth, S.Iversen, M.Kaletka, D.Barlow, A.Saha, R.Soundranayagam Mass of Proton-Rich 58Zn by Pion Double Charge Exchange NUCLEAR REACTIONS 58Ni(π+, π-), E=292 MeV; measured missing mass spectra. 58Zn deduced mass excess.
doi: 10.1016/0370-2693(86)90402-8
1985GL02 Phys.Rev. C31, 288 (1985) G.Glass, T.S.Bhatia, J.C.Hiebert, R.A.Kenefick, S.Nath, L.C.Northcliffe, W.B.Tippens, D.B.Barlow, A.Saha, K.K.Seth, J.G.J.Boissevain, J.J.Jarmer, J.E.Simmons, R.H.Jeppesen, G.E.Tripard Measurements of Spin-Correlation Parameters A(LL) and A(SL) for p(pol)p(pol) → πd between 500 and 800 MeV NUCLEAR REACTIONS 1H(polarized p, π), E=500, 650, 800 MeV; measured spin correlation parameters vs θ.
doi: 10.1103/PhysRevC.31.288
1985SE10 Phys.Lett. 155B, 339 (1985) K.K.Seth, M.Kaletka, D.Barlow, D.Kielczewska, A.Saha, L.Casey, D.Godman, R.Seth, J.Stuart Observation of Double Analog States in 88Zr and 90Mo and the Neutron Excess and Mass Systematics of Pion Double Charge Exchange NUCLEAR REACTIONS 88Sr, 90Zr(π+, π-), E=180, 292 MeV; measured σ(θ=5°), missing mass spectra; deduced neutron excess, mass systematics of reaction mechanism. 88Zr, 90Mo deduced double IAS excitation, energy, T.
doi: 10.1016/0370-2693(85)91583-7
1985SE14 Phys.Lett. 158B, 23 (1985) K.K.Seth, D.Barlow, A.Saha, R.Soundranayagam, S.Iversen, M.Kaletka, M.Bosko, D.Smith, G.W.Hoffmann, M.L.Barlett, R.Fergerson, J.McGill, E.C.Milner Polarized Proton Inelastic Scattering from 40Ca and 48Ca at 500 MeV NUCLEAR REACTIONS 40,48Ca(polarized p, p'), E=500 MeV; measured σ(θ), analyzing power vs θ. 40Ca(polarized p, p), E=500 MeV; analyzed spin rotation parameter vs θ; deduced optical potential parameters. 40,48Ca deduced mass deformation parameters, lengths.
doi: 10.1016/0370-2693(85)90731-2
1984BL19 Phys.Lett. 149B, 441 (1984) H.Blok, H.P.Blok, J.F.A.van Hienen, G.van der Steenhoven, C.W.de Jager, H.de Vries, A.Saha, K.K.Seth Contribution of 2(h-bar x Omega) Transition to the Excitation of 0+ States in 58Ni and 26Mg in Inelastic Electron Scattering NUCLEAR REACTIONS 58Ni, 26Mg(e, e'), E not given; measured monopole form factors. 26Mg, 58Ni levels deduced monopole matrix element, EWSR, normalization factors. Shell model.
doi: 10.1016/0370-2693(84)90362-9
1984HA29 Phys.Rev.Lett. 53, 152 (1984) P.Harihar, K.K.Seth, D.Barlow, S.Iversen, M.Kaletka, H.Nann, A.Saha, C.F.Williamson, J.W.Wong, M.Deady, W.J.Gerace Direct Verification of the Coexistence Model for 40Ca: Electroexcitation of the second monopole state NUCLEAR REACTIONS 40Ca(e, e'), E=81.6-380 MeV; measured σ(E(e')), form factors. 40Ca level deduced electroexcitation transition density.
doi: 10.1103/PhysRevLett.53.152
1984SA11 Phys.Rev.Lett. 52, 1876 (1984) A.Saha, K.K.Seth, M.Artuso, B.Harris, R.Seth, H.Nann, W.W.Jacobs Determination of the Relative Sign of Neutron and Proton Transition Matrix Elements for the 34S(0 → 22+) Transition NUCLEAR REACTIONS 34S(α, α), (α, α'), E=120 MeV; measured σ(Eα), σ(θ). 34S levels deduced neutron, proton matrix element relative sign. DWBA, CCBA analyses.
doi: 10.1103/PhysRevLett.52.1876
1984SE04 Phys.Rev.Lett. 52, 894 (1984) K.K.Seth, M.Kaletka, S.Iversen, A.Saha, D.Barlow, D.Smith, L.C.Liu Core-Excitation Effects in Pion Double Charge Exchange NUCLEAR REACTIONS 42Ca(π+, π-), E ≈ 125-300 MeV; measured σ(θ); deduced pion-nucleus potential characteristics. 42Ca deduced ground state core excitation components. Optical model, first-, second-order one-body density terms.
doi: 10.1103/PhysRevLett.52.894
1984VA31 Nucl.Phys. A429, 1 (1984); Erratum Nucl.Phys. A441, 757 (1985) A.M.Van Den Berg, A.Saha, G.D.Jones, L.W.Put, R.H.Siemssen Study of Even-A Zirconium and Strontium Isotopes with the (d, 6Li) Reaction NUCLEAR REACTIONS 90,92Zr, 92,94,96,98,100Mo(d, 6Li), E=45 MeV; measured σ(E(6Li), θ). 86,88Sr, 88,90,92,94,96Zr levels deduced S(α), J, π. DWBA analysis, shell model wave functions. Enriched targets, magnetic spectograph.
doi: 10.1016/0375-9474(84)90147-7
1983SA01 Phys.Rev. C27, 405 (1983) Systematics of Ground State (p, t) Transitions in Calcium Isotopes NUCLEAR REACTIONS 48,44,43,42,40Ca(p, t), E=40 MeV; measured absolute σ(θ), σ(Et). 46,42,41,40,38Ca level deduced L=0 transition probability. DWBA analysis, pure f7/2 pickup.
doi: 10.1103/PhysRevC.27.405
1983SA19 Phys.Rev.Lett. 51, 759 (1983) A.Saha, K.K.Seth, D.Kielczewska, S.Iversen, M.Kaletka, D.Barlow, D.Smith Energy Variation of the Analyzing Power in the Reaction p(pol) + p → d + π+ NUCLEAR REACTIONS 1H(polarized p, π+), E ≈ 550, 600, 650, 700, 800 MeV; measured analyzing power vs θ; deduced isobar dominance in pion production. Phenomenological analysis, other data input, Legendre polynomial fits.
doi: 10.1103/PhysRevLett.51.759
1983SA29 Phys.Lett. 130B, 152 (1983) A.Saha, K.K.Seth, B.A.Brown, H.Nann The (p, t) Reaction to 48Ti and 49V in the (f7/2)(n) Model NUCLEAR REACTIONS 50Ti, 51V(p, t), E=40.2 MeV; measured σ(θ); deduced angle-integrated σ. 48Ti, 49V deduced levels, J, π, S. DWBA analysis, (f7/2)(n) model.
doi: 10.1016/0370-2693(83)91031-6
1983SA31 Phys.Lett. 132B, 51 (1983) A.Saha, K.K.Seth, L.Casey, D.Godman, D.Kielczewska, R.Seth, J.Stuart, O.Scholten Isovector Properties of Collective States and the IBA-2 Model NUCLEAR REACTIONS 104,106,108,110Pd(π+, π+'), (π-, π-'), E=180 MeV; measured σ(E(π)), σ(θ). 104,106,108,110Pd levels deduced neutron, proton matrix elements, ratios. Interacting boson model.
doi: 10.1016/0370-2693(83)90220-4
1983SE13 Phys.Lett. 126B, 164 (1983) K.K.Seth, A.Saha, D.Kielczewska, S.Iversen, M.Kaletka, D.Barlow, B.Hoistad Analyzing Power for the p(pol) + p → d + π+ Reaction at 0.8 GeV and Effects of Dibaryon Admixtures NUCLEAR REACTIONS 1H(polarized p, π+), E=0.8 GeV; measured σ(θ(π)), analyzing power vs θ; deduced no dibaryon admixtures. Legendre polynomial analysis.
doi: 10.1016/0370-2693(83)90583-X
1982SA15 Phys.Lett. 114B, 419 (1982) A.Saha, K.K.Seth, D.Barlow, H.Nann, W.W.Jacobs Measurement of the Relative Sign of Neutron and Proton Transition Matrix Elements of the 2+ States in 30Si NUCLEAR REACTIONS 30Si(α, α'), E=120 MeV; measured σ(θ). 30Si level deduced neutron, proton matrix element relative sign. DWBA analysis.
doi: 10.1016/0370-2693(82)90083-1
1982VA08 Nucl.Phys. A379, 239 (1982) A.M.Van Den Berg, R.V.F.Janssens, G.T.Emery, A.Saha, R.H.Siemssen First Excited 0+ States in the Germanium Isotopes Via the Se(d, 6Li) Reaction NUCLEAR REACTIONS 74,76,78,80,82Se(d, 6Li), E=45 MeV, measured σ(E(6Li), θ). 70,72,74,76,78Ge levels deduced Sα, L, J, π. Magnetic spectrograph, enriched targets.
doi: 10.1016/0375-9474(82)90392-X
1981HO26 Phys.Rev.Lett. 47, 1436 (1981) G.W.Hoffmann, L.Ray, M.L.Barlett, R.Fergerson, J.McGill, E.C.Milner, K.K.Seth, D.Barlow, M.Bosko, S.Iversen, M.Kaletka, A.Saha, D.Smith Elastic Scattering of 500-MeV Polarized Protons from 40,48Ca, 90Zr, and 208Pb, and Breakdown of the Impulse Approximation at Small Momentum Transfer NUCLEAR REACTIONS 40,48Ca, 90Zr, 208Pb(polarized p, p), E=500 MeV; measured σ(θ), A(θ); deduced impulse approximation breakdown. Second-order. Kerman-McManus-Thaler optical potential.
doi: 10.1103/PhysRevLett.47.1436
1981NA01 Phys.Rev. C23, 606 (1981) H.Nann, A.Saha, B.H.Wildenthal Energy Levels in 23Mg from the 25Mg(p, t)23Mg Reaction NUCLEAR REACTIONS 25Mg(p, t), E=40 MeV; measured σ(Et, θ). 23Mg deduced levels, L, J, π. DWBA analysis, shell model spectroscopic amplitudes. Enriched target.
doi: 10.1103/PhysRevC.23.606
1980HA33 Nucl.Phys. A344, 15 (1980) M.N.Harakeh, J. Van Popta, A.Saha, R.H.Siemssen Strong Coupled-Channels Effects in the 9Be(α, t)10B Reaction NUCLEAR REACTIONS 9Be(α, α'), (α, t), (α, 3He), E=65 MeV; measured σ(Eα, θ), σ(Et, θ), σ(E(3He), θ); deduced optical-model parameters; 9Be levels deduced β2. 10B, 10Be levels deduced L, S. DWBA, coupled-channel analyses.
doi: 10.1016/0375-9474(80)90429-7
1979KU08 Phys.Rev.Lett. 43, 341 (1979) Method of Finite-Range Distorted-Wave Born Approximation for Pickup to Unbound Ejectiles NUCLEAR REACTIONS 12C(α, αp), E=65 MeV; calculated σ. Finite range DWBA for pickup to unbound ejectiles.
doi: 10.1103/PhysRevLett.43.341
1979SA12 Phys.Lett. 82B, 208 (1979) A.Saha, G.D.Jones, L.W.Put, R.H.Siemssen Unusually Strong Excitation of the 1.59 MeV 0+ State in the 100Mo(d, 6Li)96Zr Reaction NUCLEAR REACTIONS 94,96,98,100Mo(d, 6Li), E=45 MeV; measured σ(E(6Li)), σ(θ). 90,92,94,96Zr deduced change in proton configuration with neutron number. DWBA analysis. Enriched targets.
doi: 10.1016/0370-2693(79)90737-8
1979SA16 Phys.Rev. C19, 2065 (1979) Q and A Dependence of Rare-Earth (p, t) Strengths NUCLEAR REACTIONS Sm, Gd, Dy, Er, Yb, Hf(p, t), E=18, 19 MeV; calculated σ(θ); deduced Q, Z, A dependence. DWBA calculations.
doi: 10.1103/PhysRevC.19.2065
1979SA22 Phys.Lett. 85B, 215 (1979) A.Saha, O.Scholten, D.C.J.M.Hageman, H.T.Fortune Two Neutron Transfer in Samarium Isotopes and IBA Model Predictions NUCLEAR REACTIONS 148,150,152,154Sm(p, t), E=40 MeV; measured σ(Et, θt). 144,146,148,150,152,154Sm deduced relative (p, t) to (t, p) cross sections for ground, first excited 0+ states. Enriched targets, high resolution magnetic spectrograph. Comparison with interacting boson approximation.
doi: 10.1016/0370-2693(79)90582-3
1978FO32 Phys.Lett. 79B, 205 (1978) H.T.Fortune, J.C.Vermeulen, A.Saha, A.G.Drentje, L.W.Put, R.R.de Ruyter van Steveninck, J.F.A.van Hienen Configuration of 3.59 MeV 0+ State in 44Ca NUCLEAR REACTIONS 48Ti(d, 6Li), E=55 MeV; measured σ(E(6Li), θ). 44Ca deduced relative α-pickup S for 0+ states.
doi: 10.1016/0370-2693(78)90223-X
1978NA11 Phys.Rev. C18, 1619 (1978) Energy Levels in 57Ni from a Study of the 59Ni(p, t)57Ni Reaction NUCLEAR REACTIONS 59Ni(p, t), E=40 MeV; measured σ(θ). 57Ni deduced levels, L, J, π. DWBA analysis. Enriched target.
doi: 10.1103/PhysRevC.18.1619
1978SA26 Phys.Lett. 79B, 363 (1978) A.Saha, R.Kamermans, J.van Driel, H.P.Morsch Unbound Li Nuclei as Ejectiles in α-Induced Pickup NUCLEAR REACTIONS 12C, 24Mg(α, 5Li'), (α, 6Li'), (α, 7Li'), E corresponds to 65 MeV/c; measured relative energy distribution of correlated decay products.
doi: 10.1016/0370-2693(78)90383-0
1977NA10 Phys.Rev. C15, 1959 (1977) H.Nann, W.S.Chien, A.Saha, B.H.Wildenthal High-Spin States of (fp)2 Character in 34,35,36Cl and 37,39Ar NUCLEAR REACTIONS 32,33,34S, 35,37Cl(α, d), E=40 MeV; measured σ(Ed, θ). 34,35,36Cl, 37,39Ar levels deduced L, J, π.
doi: 10.1103/PhysRevC.15.1959
1977NA25 Nucl.Phys. A292, 195 (1977) H.Nann, W.S.Chien, A.Saha, B.H.Wildenthal The 40Ca(α, d)42Sc Reaction NUCLEAR REACTIONS 40Ca(α, d), E=40 MeV; measured σ(Ed, θ). 42Sc deduced levels, L-transfer. Enriched target.
doi: 10.1016/0375-9474(77)90367-0
1977NA30 Nucl.Phys. A292, 205 (1977) Four-Particle One-Hole States in 43Ca Strongly Populated by the 41K(α, d) Reaction NUCLEAR REACTIONS 41K(α, d), E=40 MeV; measured σ(Ed, θ). 43Ca levels deduced L-transfer, J, π. Enriched target.
doi: 10.1016/0375-9474(77)90368-2
1976NA23 Phys.Rev. C14, 2338 (1976) H.Nann, E.Kashy, D.Mueller, A.Saha, S.Raman Mass of 57Ni NUCLEAR REACTIONS 59Ni(p, t), E=40 MeV; 58Ni(3He, α), E=70 MeV; measured σ(θ); deduced Q. 57Ni deduced mass excess.
doi: 10.1103/PhysRevC.14.2338
1975NA10 Phys.Rev.Lett. 35, 609 (1975); Erratum Phys.Rev.Lett. 35, 1051 (1975) H.Nann, B.H.Wildenthal, A.Saha, K.K.Seth Comment on 'Prediction of Weak-Coupling Structure from a Shell-Model Basis' NUCLEAR REACTIONS 34S, 35Cl(p, t), E=40 MeV; measured σ(Et, θ). 32S, 33Cl levels deduced L, S.
doi: 10.1103/PhysRevLett.35.609
1975NA14 Phys.Rev. C12, 1524 (1975) H.Nann, W.S.Chien, A.Saha, B.H.Wildenthal (f7/2)27, 0d3/2-1 Configuration States in 41Ca Strongly Populated by the 39K(α, d) Reaction NUCLEAR REACTIONS 39K(α, d), E=40 MeV; measured σ(Ed, θ). 41Ca levels deduced L.
doi: 10.1103/PhysRevC.12.1524
1975NA18 Phys.Lett. 60B, 32 (1975) H.Nann, W.S.Chien, A.Saha, B.H.Wildenthal The Strongest L=6 Transitions Observed in the (α, d) Reaction on Odd-Mass A=33-41 Target Nuclei NUCLEAR REACTIONS 33S, 35,37Cl, 39,41K(α, α), (α, d), E=40 MeV; measured σ(Ed, θ). 35Cl, 37,39Ar, 41,43Ca levels deduced L.
doi: 10.1016/0370-2693(75)90519-5
1975SE17 Phys.Lett. 59B, 333 (1975) K.K.Seth, A.Saha, H.Nann, B.H.Wildenthal Structure of Positive Parity States in 29P and Two-Step Processes in (p, t) Reactions NUCLEAR REACTIONS 30Si, 31P(p, t), E=40 MeV; measured σ(Et, θ). 29P, 28Si deduced levels, L.
doi: 10.1016/0370-2693(75)90085-4
1974SE04 Phys.Lett. 49B, 157 (1974) K.K.Seth, A.Saha, W.Stewart, W.Benenson, W.A.Lanford, H.Nann, B.H.Wildenthal (p, t) Reactions on Odd-A Nuclei and the Weak-Coupling Core-Excitation Model NUCLEAR REACTIONS 43Ca(p, t), E=42 MeV; 42Ca, 59Co, 60Ni(p, t), E=40 MeV; measured reaction products. 40,41Ca, 57Co, 58Ni; deduced σ(θ), levels, negative-parity states, L, weak-coupling. The Michigan State University cyclotron and an Enge split-pole spectrograph equipped with a single-wire proportional counter.
doi: 10.1016/0370-2693(74)90497-3
1974SE05 Phys.Rev.Lett. 33, 233 (1974) K.K.Seth, A.Saha, W.Benenson, W.A.Lanford, H.Nann, B.H.Wildenthal Discovery of the Missing Two-Particle, Two-Hole 0+ States in 40Ca NUCLEAR REACTIONS 42Ca(p, t), E=40.27 MeV; measured Q, σ(E(t), θ). 40Ca deduced levels, J, π.
doi: 10.1103/PhysRevLett.33.233
1973SE09 Phys.Rev.Lett. 31, 552 (1973) High-Spin States in 41Ca; K = 3/2+ and K = 3/2- Rotational Bands (Question) NUCLEAR REACTIONS 40Ca(d, p), E=11 MeV; measured σ(Ep, θ). 41Ca levels deduced J, π, L, S.
doi: 10.1103/PhysRevLett.31.552
1967SH04 Nucl.Phys. A97, 567 (1967) On the Collective Octupole State of 88Sr
doi: 10.1016/0375-9474(67)90521-0
1966SH13 Nucl.Phys. 85, 393 (1966) On the Electric Dipole and Octupole Transition in 88Sr NUCLEAR STRUCTURE 88Sr; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(66)90631-6
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