NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = M.Afzal Ansari Found 34 matches. 2023MA05 Phys.Rev. C 107, 014601 (2023) A.Mahato, D.Singh, N.Sharma, P.K.Giri, S.B.Linda, H.Kumar, S.A.Tali, A.Ali, M.Afzal Ansari, N.K.Deb, N.P.M.Sathik, S.Kumar, R.Kumar, S.Muralithar, R.P.Singh Disentangling fractional momentum transfer in the 19F + 154Sm system NUCLEAR REACTIONS 154Sm(19F, 5n)168Lu, (19F, 6n)167Lu, (19F, 5np)167Yb, (19F, 3nα)166Tm, (19F, 4nα)165Tm, (19F, 5nα)164Tm, (19F, 3n2α)162Ho, (19F, 4n2α)161Ho, E=107 MeV; measured reaction products, evaporation residues (ERs), Eγ, Iγ; deduced ERs yields as a function of range in stopping medium, forward recoil range distributions (FRRDs) for the evaporation residues, range integrated σ, relative contributions of complete and incomplete fusion, mean ranges in stopping medium. Discussed linear momentum transfer from the projectile to target accounting also for projectile breakup α+15N and 2α+11B. Activation technique. Beam from 15UD Pelletron accelerator facility at Inter University Accelerator Center (IUAC, India). ERs were collected with a stack of 26 aluminium catcher foils of different thicknesses placed immediately after the target. The decay of ERs on the catcher foils measured with HPGe detector.
doi: 10.1103/PhysRevC.107.014601
2022MA34 Phys.Rev. C 106, 014613 (2022) A.Mahato, D.Singh, N.Sharma, P.K.Giri, S.B.Linda, H.Kumar, S.A.Tali, M.Afzal Ansari, A.Ali, N.K.Deb, N.P.M.Sathik, S.Kumar, R.Kumar, S.Muralithar, R.P.Singh Effects of entrance channels on breakup fusion induced by 19F projectiles NUCLEAR REACTIONS 154Sm(19F, X), (19F, 4n), (19F, 5n), (19F, 6n), (19F, 5np), (19F, 3nα), (19F, 4nα), (19F, 5nα), (19F, 3n2α), (19F, 4n2α)E=78-110 MeV; measured Eγ, Iγ; deduced complete fusion and evaporation residues production σ(E), critical angular momentum, excitation functions for complete, incomplete fusion and total fusion. Incomplete fusion strength functions systematics for 16O, 19F, 20Ne induced reactions. Activation technique measurement with HPGe detector. Comparison to statistical model calculations (PACE-4 code) and coupled channels (CCFULL code). 15UD Pelletron accelerator facility at the Inter-University Accelerator Center (IUAC), New Delhi.
doi: 10.1103/PhysRevC.106.014613
2020MA22 Eur.Phys.J. A 56, 131 (2020) A.Mahato, D.Singh, P.K.Giri, S.B.Linda, H.Kumar, S.A.Tali, M.Afzal Ansari, R.Kumar, S.Muralithar, R.P.Singh Probing of incomplete fusion dynamics in 14N + 124Sn system and its correlation with various entrance channel effects
doi: 10.1140/epja/s10050-020-00126-8
2019GI15 Phys.Rev. C 100, 024621 (2019) P.K.Giri, D.Singh, A.Mahato, S.B.Linda, H.Kumar, S.A.Tali, S.Parasari, A.Ali, M.Afzal Ansari, R.Dubey, R.Kumar, S.Muralithar, R.P.Singh Systematic study of low-energy incomplete-fusion dynamics in the 16O + 148Nd system: Role of target deformation NUCLEAR REACTIONS 148Nd(16O, 3n)161Er, 148Nd(16O, 5n)159Er, 148Nd(16O, 6n)158Er, 148Nd(16O, 2np)161Ho, 148Nd(16O, 3np)160Ho, 148Nd(16O, 4np)159Ho, 148Nd(16O, 3nα)157Dy, 148Nd(16O, 5nα)155Dy, 148Nd(16O, 4npα)155Tb, E=67.2, 72.4, 77.4, 84.1, 89.1, 94.7, 99.9 MeV; measured Eγ, Iγ; deduced σ(E), incomplete fusion (ICF) σ(E), effect of target deformation; analyzed previous experimental σ(E) data for many other systems for fraction of incomplete fusion. Measured σ compared with statistical model code PACE-4, and with previous experimental data. Experiment was performed using the 15UD Pelletron accelerator facility at Inter-University Accelerator Centre (IUAC), New Delhi, India.
doi: 10.1103/PhysRevC.100.024621
2019GI17 Phys.Rev. C 100, 054604 (2019) P.K.Giri, A.Mahato, D.Singh, S.B.Linda, H.Kumar, S.A.Tali, M.Afzal Ansari, R.Kumar, S.Muralithar, R.P.Singh Examination of break-up fusion in the 16O + 148Nd system through measurements of forward recoil range distributions and angular distributions NUCLEAR REACTIONS 148Nd(16O, 6n)158Er, (16O, 5n)159Er, (16O, 4np)159Ho, (16O, 3np)160Ho, (16O, 5nα)155Dy, (16O, 3nα)157Dy, (16O, 4npα)155Tb, E AP 6 MeV/nucleon; measured Eγ, Iγ off-line, σ(θ) and forward recoil range distributions (FRRD) for evaporation residues, yields of evaporation residues using the 15 UD Pelletron facility at IUAC-New Delhi; deduced σ(θ) for total and complete fusion; analyzed incomplete fusion (ICF) fraction for several parameters using data from the present system, and previous experimental data for 16 other systems (six with 16O beam, four with 13C beam and three each for 12C and 20Ne beams). Comparison of angular distributions with calculations using PACE4 code.
doi: 10.1103/PhysRevC.100.054604
2019KU07 Phys.Rev. C 99, 034610 (2019) H.Kumar, S.A.Tali, M.Afzal Ansari, D.Singh, R.Ali, A.Ali, S.Parashari, P.K.Giri, S.B.Linda, R.Kumar, R.P.Singh, S.Muralithar Systematic study of incomplete-fusion dynamics below 8 MeV/nucleon energy NUCLEAR REACTIONS 175Lu(13C, 4n), (13C, 5n), (13C, 6n), (13C, 4np), (13C, 5np), (13C, nα), (13C, 3nα), (13C, 5nα), (13C, 2n2α), (13C, 3n2α), (13C, 4n2α)182Ir/183Ir/184Ir/182Os/183Os/183mOs/179Re/181Re/183Re/176Ta/177Ta/178mTa, E AP 88 MeV; measured Eγ, Iγ, σ for evaporation residues by γ-activation method, and forward recoil range distributions (FRRDs) at IUAC, New Delhi; deduced most probable mean ranges, normalized peak widths for residues produced via complete fusion (CF), and/or incomplete fusion (ICF), relative contribution of CF and/or ICF components; calculated Fusion l-distributions for 175Lu(12C, X), (13C, X), E=88 MeV systems using the CCFULL code. Comparison with results from previous experimental data for incomplete fusion fraction in 169Tm, 165Ho, 159Tb, 115In(12C, X), (13C, X), (16O, X), and 209Bi(6Li, X), (7Li, X) systems, and deduced no systematic trend for dependency on the target deformation parameter β2 in the study of the incomplete fusion (ICF) process.
doi: 10.1103/PhysRevC.99.034610
2019SI31 Eur.Phys.J. A 55, 164 (2019) D.Singh, P.K.Giri, A.Mahato, S.B.Linda, R.Tripathi, H.Kumar, M.Afzal Ansari, N.P.M.Sathik, R.Ali, R.Kumar, S.Muralithar, R.P.Singh Probing incomplete fusion dynamics and role of the projectile deformation in the 19F + 154Sm system NUCLEAR REACTIONS 154Sm(19F, X)160Dy/162Dy/163Dy/162Ho; 154Sm(19F, X)165Er/164Tm/165Tm/168Tm; 154Sm(19F, X)167Yb/158Yb, E=5.1 MeV/nucleon; measured reaction pr oducts populated via complete and incomplete fusion; deduced multiplicity spectra for Z=1, 2 and for α-particles. complete fusion-evaporation α-particle energy profile in forward cone, γ-ray energy spectra, transition intensity distributions for Evaporation Residuals (ER) 161Dy, 162Ho, 165Er, transition intensity distributions, normalized yields for Incomplete Fusion (ICF) populated 163Dy and 164,165Tm from Complete Fusion (CF) together with ICF in interaction; deduced ratios for 19F+154Sm and 16O+160Gd.
doi: 10.1140/epja/i2019-12860-9
2019SI43 Int.J.Mod.Phys. E28, 1950069 (2019) D.Singh, S.B.Linda, P.K.Giri, A.Mahato, H.Kumar, S.A.Tali, M.Afzal Ansari, R.Kumar, S.Muralithar, R.P.Singh Investigation of breakup fusion in 16O + 124Sn system and its correlation with various entrance channel parameters NUCLEAR REACTIONS 124Sn(16O, X)135Ce/133Ce/133La/133Ba/131Ba/132Cs/129Ba/135Cs/131Xe/131I, E ∼ 6.2 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced complete fusion (CF) and incomplete fusion (ICF) channels, evaporation residues, N/Z ratio of the target as an important entrance channel parameter which strongly affects the ICF dynamics.
doi: 10.1142/S0218301319500691
2019TA15 Phys.Rev. C 100, 024622 (2019) S.A.Tali, H.Kumar, M.Afzal Ansari, A.Ali, D.Singh, R.Ali, P.K.Giri, S.B.Linda, R.Kumar, S.Parashari, S.Muralithar, R.P.Singh Systematic study of the break-up fusion process in the 12C + 165Ho system and interplay of entrance channel parameters NUCLEAR REACTIONS 165Ho(12C, 3n)174Ta, 165Ho(12C, 4n)173Ta, 165Ho(12C, 5n)172Ta, 165Ho(12C, 6n)171Ta, 165Ho(12C, 3np)173Hf, 165Ho(12C, 5np)171Hf, 165Ho(12C, nα)172Lu, 165Ho(12C, 2nα)171Lu, 165Ho(12C, 3nα)170Lu, 165Ho(12C, 4nα)169Lu, 165Ho(12C, 3npα)169Yb, 165Ho(12C, 2n2α)167Tm, 165Ho(12C, 3n2α)166Tm, E=57.39, 61.78, 66.13, 70.38, 74.59, 78.88, 83.05, 87.38 MeV; measured Eγ, Iγ; deduced σ(E), fraction of incomplete fusion (ICF); analyzed previous experimental σ(E) data for many other systems for fraction of incomplete fusion. Measured σ compared with statistical model code PACE-4, and with previous experimental data. Experiment was performed using the 15UD Pelletron accelerator facility at Inter-University Accelerator Centre (IUAC), New Delhi, India.
doi: 10.1103/PhysRevC.100.024622
2018SI14 Phys.Rev. C 97, 064604 (2018) D.Singh, S.B.Linda, P.K.Giri, A.Mahato, R.Tripathi, H.Kumar, M.Afzal Ansari, N.P.M.Sathik, R.Ali, R.Kumar, S.Muralithar, R.P.Singh Role of input angular momentum and target deformation on the incomplete-fusion dynamics in the 16O + 154Sm system at ELab = 6.1 MeV/nucleon NUCLEAR REACTIONS 154Sm(16O, 6n), (16O, 6np), (16O, 2p), (16O, n2p), (16O, 2npα), (16O, 3npα), (16O, 4npα), (16O, 2pα), (16O, 2n2α), E=97.5 MeV; measured Eγ, γ(θ), Eα, α(θ), Ep, p(θ), γα-coin, γp-coin and spin distributions, feeding intensity patterns, and average mean driving input angular momenta of complete fusion (CF) and incomplete fusion (ICF) populated evaporation residues, multiplicity spectra recorded for charged particles using the Gamma Detector Array (GDA) and Charged Particle Detector Array at the 15UD Pelletron Accelerator facility of the IUAC-New Delhi. Comparison with earlier experimental data, and with statistical model calculations using PACE4 code. Complete- and incomplete-fusion reactions.
doi: 10.1103/PhysRevC.97.064604
2018SI15 Phys.Rev. C 97, 064610 (2018) D.Singh, S.B.Linda, P.K.Giri, A.Mahato, R.Tripathi, H.Kumar, S.A.Tali, S.Parashari, A.Ali, Ra.Dubey, M.Afzal Ansari, R.Kumar, S.Muralithar, R.P.Singh Measurement of excitation functions of evaporation residues in the 16O + 124Sn reaction and investigation of the dependence of incomplete fusion dynamics on entrance channel parameters NUCLEAR REACTIONS 124Sn(16O, 3n), (16O, 5n), (16O, 7n), (16O, 6np), (16O, 3nα), (16O, 5nα), (16O, 7nα), (16O, pα), (16O, 3npα), (16O, n2α), (16O, p2α), E=3-7 MeV/nucleon; measured Iγ, Eγ, evaporation residues populated from complete fusion and incomplete fusion reactions, σ(E) by activation method, and incomplete fusion fractions at 15UD Pelletron heavy ion accelerator facility of IUAC, New Delhi. Comparison with theoretical excitation functions using PACE-4 code, and with previous experimental results. 133,133m,135,137,137mCe, 133La, 129,129m,131,131m,133mBa, 131I, 131mXe, 132,135mCs; measured γ spectra from isotopes produced in different reaction channels.
doi: 10.1103/PhysRevC.97.064610
2018TA03 Nucl.Phys. A970, 208 (2018) S.A.Tali, H.Kumar, M.Afzal Ansari, A.Ali, D.Singh, R.Ali, P.K.Giri, S.B.Linda, S.Parashari, R.Kumar, R.P.Singh, S.Muralithar Study of incomplete fusion reaction dynamics in 13C + 165Ho system and its dependence on various entrance channel parameters NUCLEAR REACTIONS 165Ho(13C, x), E=4-7 MeV/nucleon; measured ER (Evaporation Residues) activation off-line Eγ, Iγ using HPGe coupled to CAMAC-based data acquisition system CANDLE; deduced γ-ray energy spectra. 174Ta; deduced T1/2, σ; calculated σ. 166,167Tm, 169Yb, 173Hf, 169,170,171,172Lu, 172,173,174,175Ta; deduced state, J, π, γ-ray energy Eγ, branching ratio, σ, incomplete fusion fraction vs Atarg/(Aproj+Atarg); calculated σ. Calculations done using statistical code PACE4. Incomplete fusion fraction compared also with published data from 165Ho(12C, x), (16O, x), (20Ne, x), E=4-7 MeV/nucleon.
doi: 10.1016/j.nuclphysa.2017.11.012
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
2017KU05 Nucl.Phys. A960, 53 (2017) H.Kumar, S.A.Tali, M.Afzal Ansari, D.Singh, R.Ali, K.Kumar, N.P.M.Sathik, S.Parashari, A.Ali, R.Dubey, I.Bala, R.Kumar, R.P.Singh, S.Muralithar Investigation of incomplete fusion dynamics at energy 4-8 MeV/nucleon NUCLEAR REACTIONS 175Lu(12C, xn), (12C, xnp), (12C, xnα), (12C, xn2α), (13C, xn), (13C, xnp), (13C, xnα), (13C, xn2α), E=4-8 MeV/nucleon; measured Eγ, Iγ, γγ-coin; deduced residues, γ transitions, γ-ray intensity, T1/2, levels, J, π, σ, α-decay Q value systematics; calculated σ using statistical (Hauser-Feshbach) model code PACE-4; deduced ICF (InComplete Fusion) fraction systematics with projectile-target mass asymmetry.
doi: 10.1016/j.nuclphysa.2017.01.009
2017SI24 Phys.Lett. B 774, 7 (2017) D.Singh, S.B.Linda, P.K.Giri, A.Mahato, R.Tripathi, H.Kumar, M.Afzal Ansari, N.P.M.Sathik, R.Ali, R.Kumar, S.Muralithar, R.P.Singh Spin distribution of evaporation residues formed in complete and incomplete fusion in 16O+154Sm system NUCLEAR REACTIONS 154Sm(16O, X)162Er/158Dy/163Dy/159Tb/164Tm/165Tm/165Yb/166Yb, E=6.2 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced γ-ray energies, normalized yields, feeding intensity profiles of evaporation residues.
doi: 10.1016/j.physletb.2017.09.034
2012SI03 Nucl.Phys. A879, 107 (2012) D.Singh, R.Ali, M.Afzal Ansari, B.S.Tomar, M.H.Rashid, R.Guin, S.K.Das Observation of entrance channel mass-asymmetry effect on incomplete fusion reaction for 20Ne + 165Ho system NUCLEAR REACTIONS 165Ho(20Ne, 3n), (20Ne, 2np), (20Ne, 3np), (20Ne, α), (20Ne, 2nα), (20Ne, 3nα), (20Ne, 4nα), (20Ne, 3npα), (20Ne, 4npα), (20Ne, 6npα), (20Ne, n2pα), (20Ne, 2α), (20Ne, n2α), (20Ne, 2n2α), (20Ne, 3n2α), (20Ne, 4n2α), (20Ne, 3np2α), (20Ne, 3n4α), E=88=165 MeV; measured ER Eγ, Iγ using recoil catcher; deduced direct, cumulative yields, direct σ, ICF σ, total σ, critical angular momentum, mass-asymmetry effect; calculated σ, yields using statistical model with Monte Carlo de-excitation with different level density parameters. ICF fraction compared with literature data for other systems.
doi: 10.1016/j.nuclphysa.2012.01.020
2011SI12 Phys.Rev. C 83, 054604 (2011) D.Singh, R.Ali, M.Afzal Ansari, B.S.Tomar, M.H.Rashid, R.Guin, and S.K.Das Reaction mechanism in the 20Ne+59Co system at 3-7 MeV/nucleon, and observation of entrance-channel mass-asymmetry of the incomplete fusion fraction NUCLEAR REACTIONS 59Co(20Ne, np)77Kr, 59Co(20Ne, 2np)76Kr, 59Co(20Ne, n2p)76Br, 59Co(20Ne, α)75Br, 59Co(20Ne, nα)74mBr, 59Co(20Ne, npα)73Se, 59Co(20Ne, 4npα)70Se, 59Co(20Ne, n2pα)72As, 59Co(20Ne, 2α)71As, 59Co(20Ne, n2α)70As, 59Co(20Ne, 2n2α)69As, 59Co(20Ne, np2α)69Ge, 59Co(20Ne, 3np2α)67Ge, 59Co(20Ne, 4np2α)66Ge, 59Co(20Ne, 3α)67Ga, 59Co(20Ne, n3α)66Ga, 59Co(20Ne, 2n3α)65Ga, 59Co(20Ne, 2n4α)61Cu, E=62-150 MeV; measured Eγ, Iγ, γ-activation methods, production cross sections of evaporation residues in incomplete fusion reactions. Comparison with PACE-2 predictions.
doi: 10.1103/PhysRevC.83.054604
2010AL19 J.Phys.(London) G37, 115101 (2010) R.Ali, D.Singh, M.Afzal Ansari, M.H.Rashid, R.Guin, S.K.Das Investigation of incomplete fusion in 20Ne + 55Mn reactions at 3-8 MeV/nucleon NUCLEAR REACTIONS 55Mn(20Ne, X)70Se/70As/71As/72As/66Ge/67Ge/69Ge/65Ga/66Ga/67Ga/63Zn/60Cu/61Cu, E=51-164 MeV; measured reaction products recoils, Eγ, Iγ; deduced σ, angular momentum.Comparison with statistical code PACE-2.
doi: 10.1088/0954-3899/37/11/115101
2010SI04 Phys.Rev. C 81, 027602 (2010) D.Singh, R.Ali, M.Afzal Ansari, K.S.Babu, P.P.Singh, M.K.Sharma, B.P.Singh, R.K.Sinha, R.Kumar, S.Muralithar, R.P.Singh, R.K.Bhowmik Incomplete fusion dynamics by spin distribution measurements NUCLEAR REACTIONS 124Sn(16O, X)133Ce/134Ce/135Ce/133La/135La/131Ba/132Ba/133Ba/128,130,133Xe/131Cs/127I, E=6.3 MeV/nucleon; measured Eγ, Iγ; deduced spin distributions of evaporation residues formed in xn, pxn, αxn, αpxn and 2αxn reaction channels.
doi: 10.1103/PhysRevC.81.027602
2009SI10 Phys.Rev. C 79, 054601 (2009) D.Singh, R.Ali, M.Afzal Ansari, M.H.Rashid, R.Guin, S.K.Das Reaction mechanisms in the system 20Ne+165Ho: Measurement and analysis of forward recoil range distributions NUCLEAR REACTIONS 165Ho(20Ne, 2np), (20Ne, 3np), (20Ne, α), (20Ne, 2nα), (20Ne, 3npα), (20Ne, 4npα), (20Ne, 6npα), (20Ne, n2pα), (20Ne, 2α), (20Ne, n2α), (20Ne, 2n2α), (20Ne, 3n2α), (20Ne, 4n2α), (20Ne, 3np2α), (20Ne, 3n4α), E=164 MeV; measured Eγ, Iγ, yields, forward recoil range distributions and relative contributions of complete and incomplete fusion channels.
doi: 10.1103/PhysRevC.79.054601
2008SI05 Chin.J.Phys.(Taiwan) 46, 27 (2008) D.Singh, M.Afzal Ansari, R.Ali, N.P.M.Sathik, M.Ismail A Study of Excitation Functions for Some Residues Produced in 16O+74Ge System Below 7 MeV/nucleon NUCLEAR REACTIONS 74Ge(16O, 4n), (16O, 2np), (16O, 3np), (16O, 4np), (16O, nα), (16O, 3nα), (16O, 2npα), (16O, 3npα), (16O, 3n2α), E=60.2-111.6 MeV; measured Eγ, Iγ, cross sections using stacked foil activation. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6092. 2005AF02 J.Phys.Soc.Jpn. 74, 1150 (2005) M.Afzal Ansari, N.P.M.Sathik, D.Singh, M.H.Rashid Measurement and Analysis of Alpha Particle Induced Reactions on Praseodymium NUCLEAR REACTIONS 141Pr(α, n), (α, 2n), E=15-45 MeV; measured σ. Stacked-foil activation technique. Comparison with model predictions.
doi: 10.1143/JPSJ.74.1150
2004AF03 Int.J.Mod.Phys. E13, 585 (2004) M.Afzal Ansari, M.A.Abd.Alslam, N.P.Sathik, M.Ismail, M.H.Rashid Excitation functions of α-induced reactions in cobalt and pre-equilibrium effects NUCLEAR REACTIONS 59Co(α, 2n), (α, nα), (α, 2nα), E=17-50 MeV; 59Co(α, 2nα), (α, n2p), E=40-50 MeV; measured excitation functions; deduced pre-equilibrium effects. Stacked-foil activation.
doi: 10.1142/S0218301304002405
2002SA34 Phys.Rev. C66, 014602 (2002); Erratum Phys.Rev. C67, 059903 (2003) N.P.M.Sathik, M.Afzal Ansari, B.P.Singh, M.Ismail, M.H.Rashid Preequilibrium Emission in α Induced Reactions on Bromine and Thallium NUCLEAR REACTIONS 203Tl(α, n), 79Br, 203Tl(α, 2n), 203,205Tl(α, 3n), 81Br, 203,205Tl(α, 4n), E ≈ 20-50 MeV; measured production σ. Stacked-foil activation technique, comparison with model predictions.
doi: 10.1103/PhysRevC.66.014602
2001SI34 Chin.J.Phys.(Taiwan) 39, 336 (2001) R.K.Y.Singh, M.Afzal Ansari, R.P.Gautam Pre-Equilibrium Particle Emission in α-Induced Excitation Functions in Niobium NUCLEAR REACTIONS 93Nb(α, n), (α, 2n), (α, 3n), (α, nα), E < 40 MeV; measured σ. Stacked-foil activation, comparison with model predictions. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0456. 1996SA48 Pramana 47, 401 (1996) N.P.M.Sathik, M.Afzal Ansari, B.P.Singh, R.Prasad Measurement and Analysis of Excitation Functions for Alpha Induced Reactions on Iodine and Cesium NUCLEAR REACTIONS, ICPND 127I(α, 2n), E=18-50 MeV; 127I(α, 4n), E=40-50 MeV; 133Cs(α, 2n), E=18-48 MeV; 133Cs(α, 4n), E=40-48 MeV; measured total σ vs E; deduced preequilibrium effects. Weisskopf-Ewing model calculations. Stacked foil activation technique.
doi: 10.1007/BF02847827
1993SI03 Phys.Rev. C47, 2055 (1993) B.P.Singh, M.G.V.Sankaracharyulu, M.Afzal Ansari, H.D.Bhardwaj, R.Prasad Equilibrium and Preequilibrium Emission in Some α-Induced Reactions on Enriched Isotopes 128,130Te at Moderate Excitation Energies NUCLEAR REACTIONS, ICPND 130,128Te(α, np), E ≈ 22.56-44.96 MeV; measured σ(E); deduced preequilibrium fraction energy, target mass dependences. Statistical model.
doi: 10.1103/PhysRevC.47.2055
1990CH11 Appl.Radiat.Isot. 41, 401 (1990) A.K.Chaubey, M.K.Bhardwaj, R.P.Gautam, R.K.Y.Singh, M.Afzal Ansari, I.A.Rizvi, H.Singh Pre-Equilibrium Decay Process in the Alpha Induced Reactions of Silver Isotopes NUCLEAR REACTIONS, ICPND 107Ag(α, n), (α, 2n), 109Ag(α, 2n), (α, 3n), E=threshold-50 MeV; measured σ(E). Stacked foil technique. Model calculations.
doi: 10.1016/0883-2889(90)90150-F
1989RI06 Can.J.Phys. 67, 870 (1989) I.A.Rizvi, M.K.Bhardwaj, M.Afzal Ansari, A.K.Chaubey Nonequilibrium Effects in α-Particle Induced Reactions on Gallium Isotopes NUCLEAR REACTIONS 69Ga(α, n), (α, 2n), (α, 3n), (α, 3np), 71Ga(α, 4n), (α, n), E ≈ threshold-60 MeV; measured σ(E); deduced nonequilibrium effects role. Stacked foil activation technique. Geometry dependent hybrid model.
doi: 10.1139/p89-150
1989RI08 Can.J.Phys. 67, 1091 (1989) I.A.Rizvi, M.K.Bhardwaj, M.Afzal Ansari, A.K.Chaubey Preequilibrium Emission of Multiparticles in α-Induced Reactions with 55Mn Nucleus NUCLEAR REACTIONS, ICPND Mn(α, n), (α, 2n), (α, 3n), (α, 4n), (α, nα), (α, 3n2p), (α, 3nα), E=7-60 MeV; measured σ(E). γ-spectroscopy, Ge(Li) detector. Exciton model.
doi: 10.1139/p89-188
1987RI09 J.Phys.Soc.Jpn. 56, 3135 (1987) I.A.Rizvi, M.Afzal Ansari, R.P.Gautam, R.K.Y.Singh, A.K.Chaubey Excitation Function Studies of (α, xpyn) Reactions for 63,65Cu and Pre-Equilibrium Effect NUCLEAR REACTIONS, ICPND 63,65Cu(α, xnyp)66Ga/65Zn/65Ga/68Ga/67Ga, E=40 MeV; measured residual production σ(E). Stacked foil activation technique. Preequilibrium emission, geometry dependent hybrid model. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0090. 1981AG03 Nuovo Cim. 61A, 141 (1981) H.M.Agrawal, M.Afzal Ansari, M.Wasim, M.L.Sehgal Neutron Capture Cross-Sections in the keV Energy Region NUCLEAR REACTIONS 51V(n, γ), E=415 keV; 65Cu(n, γ), E=415, 610 keV; 69Ga(n, γ), E=460, 650 keV; 80Se, 107Ag(n, γ), E=610 keV; 110Pd(n, γ), E=380 keV; 154Sm(n, γ), E=400, 650 keV; 198Pt(n, γ), E=475 keV; measured σ. Statistical model analysis.
doi: 10.1007/BF02902447
1981AG04 Z.Phys. A300, 313 (1981) H.M.Agrawal, M.Wasim, M.Afzal Ansari, M.L.Sehgal Activation Cross-Sections for 209Bi(n, α)206Tl Reaction NUCLEAR REACTIONS 209Bi(n, α), E=340, 575 keV; measured σ. Natural target, activation technique. Hauser-Feshbach calculations.
doi: 10.1007/BF01419861
1980AG01 Nucl.Phys. A337, 227 (1980) H.M.Agrawal, M.Wasim, M.Afzal Ansari, M.L.Sehgal 181Ta(n, α)178mLu, 178Lu Reactions and Isomeric States of 178Lu NUCLEAR REACTIONS 181Ta(n, α), E=270, 615, 690, 875 keV; measured isomer production σ ratio. 178Lu deduced levels, J, π.
doi: 10.1016/0375-9474(80)90052-4
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