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NSR database version of April 11, 2024.

Search: Author = C.Samanta

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2022SU03      Prog.Theor.Exp.Phys. 2022, 013D01 (2022)

K.N.Suzuki, T.Gogami, B.Pandey, K.Itabashi, S.Nagao, K.Okuyama, S.N.Nakamura, L.Tang, D.Abrams, T.Akiyama, D.Androic, K.Aniol, C.Ayerbe Gayoso, J.Bane, S.Barcus, J.Barrow, V.Bellini, H.Bhatt, D.Bhetuwal, D.Biswas, A.Camsonne, J.Castellanos, J.-P.Chen, J.Chen, S.Covrig, D.Chrisman, R.Cruz-Torres, R.Das, E.Fuchey, K.Gnanvo, F.Garibaldi, T.Gautam, J.Gomez, P.Gueye, T.J.Hague, O.Hansen, W.Henry, F.Hauenstein, D.W.Higinbotham, C.E.Hyde, M.Kaneta, C.Keppel, T.Kutz, N.Lashley-Colthirst, S.Li, H.Liu, J.Mammei, P.Markowitz, R.E.McClellan, F.Meddi, D.Meekins, R.Michaels, M.Mihovilovic, A.Moyer, D.Nguyen, M.Nycz, V.Owen, C.Palatchi, S.Park, T.Petkovic, S.Premathilake, P.E.Reimer, J.Reinhold, S.Riordan, V.Rodriguez, C.Samanta, S.N.Santiesteban, B.Sawatzky, S.Sirca, K.Slifer, T.Su, Y.Tian, Y.Toyama, K.Uehara, G.M.Urciuoli, D.Votaw, J.Williamson, B.Wojtsekhowski, S.A.Wood, B.Yale, Z.Ye, J.Zhang, X.Zheng

The cross-section measurement for the 3H(e, e'K+)nnΛ reaction

NUCLEAR REACTIONS 3H(e-, e-'K+), E not given; measured reaction products; deduced σ(θ), missing mass. Comparison with Monte Carlo simulations.

doi: 10.1093/ptep/ptab158
Citations: PlumX Metrics


2010FU13      Int.J.Mod.Phys. E19, 2480 (2010)

Y.Fujii, A.Chiba, D.Doi, T.Gogami, O.Hashimoto, H.Kanda, M.Kaneta, D.Kawama, K.Maeda, T.Maruta, A.Matsumura, S.Nagao, S.N.Nakamura, A.Shichijo, H.Tamura, N.Taniya, T.Yamamoto, K.Yokota, S.Kato, Y.Sato, T.Takahashi, H.Noumi, T.Motoba, E.Hiyama, I.Albayrak, O.Ates, C.Chen, M.Christy, C.Keppel, M.Kohl, Y.Li, A.Liyanage, L.Tang, T.Walton, Z.Ye, L.Yuan, L.Zhu, P.Baturin, W.Boeglin, S.Dhamija, P.Markowitz, B.Raue, J.Reinhold, Ed.V.Hungerford, R.Ent, H.Fenker, D.Gaskell, T.Horn, M.Jones, G.Smith, W.Vulcan, S.A.Wood, C.Johnston, N.Simicevic, S.Wells, C.Samanta, B.Hu, J.Shen, W.Wang, X.Zhang, Y.Zhang, J.Feng, Y.Fu, J.Zhou, S.Zhou, Y.Jiang, H.Lu, X.Yan, Y.Ye, L.Gan, A.Ahmidouch, S.Danagoulian, A.Gasparian, M.Elaasar, F.R.Wesselmann, A.Asaturyan, A.Margaryan, A.Mkrtchyan, H.Mkrtchyan, V.Tadevosyan, D.Androic, M.Furic, T.Petkovic, T.Seva, G.Niculescu, I.Niculescu, V.M.Rodriguez Lopez, E.Cisbani, F.Cusanno, F.Garibaldi, G.M.Uuciuoli, R.De Leo, S.Maronne

Hypernuclear spectroscopy with electron beam at JLab HALL C

NUCLEAR REACTIONS 7Li, 12C, 28Si(E, EK+)7He/12B/28Al, E=1.2 GeV; measured reaction products; deduced hypernuclear spectroscopy, missing mass spectrum.

doi: 10.1142/S0218301310016983
Citations: PlumX Metrics


2009BA53      Phys.Rev. C 80, 057304 (2009)

D.N.Basu, P.Roy Chowdhury, C.Samanta

Isobaric incompressibility of isospin asymmetric nuclear matter

doi: 10.1103/PhysRevC.80.057304
Citations: PlumX Metrics


2009RO15      Phys.Rev. C 80, 011305 (2009)

P.Roy Chowdhury, D.N.Basu, C.Samanta

Isospin dependent properties of asymmetric nuclear matter

doi: 10.1103/PhysRevC.80.011305
Citations: PlumX Metrics


2008BA32      Nucl.Phys. A811, 140 (2008)

D.N.Basu, P.Roy Chowdhury, C.Samanta

Nuclear equation of state at high baryonic density and compact star constraints

RADIOACTIVITY 105Sb, 145,147Tm, 150,151Lu, 155,156,157Ta, 160,161Re, 164,165,166,167Ir, 171Au, 177Tl, 185Bi(p); calculated T1/2 using a mean-field approach with the DDM3Y folding potential. Comparison with data.

doi: 10.1016/j.nuclphysa.2008.07.009
Citations: PlumX Metrics


2008HO10      Phys.Rev. C 78, 047302 (2008)

M.E.Howard, R.G.T.Zegers, Sam M.Austin, D.Bazin, B.A.Brown, A.L.Cole, B.Davids, M.Famiano, Y.Fujita, A.Gade, D.Galaviz, G.W.Hitt, M.Matos, S.D.Reitzner, C.Samanta, L.J.Schradin, Y.Shimbara, E.E.Smith, C.Simenel

Gamow-Teller strengths in 24Na using the 24Mg(t, 3He) reaction at 115A MeV

NUCLEAR REACTIONS 24Mg(t, 3He), E=115 MeV/nucleon; measured particle spectra, σ(θ); deduced levels, B(GT). Comparisons of GT values with 24Mg(3He, t), (d, 2He) reactions and USDA, USDB calculations.

doi: 10.1103/PhysRevC.78.047302
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1663. Data from this article have been entered in the XUNDL database. For more information, click here.


2008RO10      Phys.Rev. C 77, 044603 (2008)

P.Roy Chowdhury, C.Samanta, D.N.Basu

Search for long lived heaviest nuclei beyond the valley of stability

NUCLEAR STRUCTURE Z=102-120, N=120-200; calculated α-, β- and SF-decay half-lives. 266Sg, 267Bh, 266,267,269,270Hs, 268Mt, 267,268,269,270,271,273Ds, 272Rg, 277,283Cn; calculated α-decay half-lives, comparison with experimental data. Quantum tunneling model with DDM3Y interaction using three different mass formulae.

doi: 10.1103/PhysRevC.77.044603
Citations: PlumX Metrics


2008RO25      At.Data Nucl.Data Tables 94, 781 (2008)

P.Roy Chowdhury, C.Samanta, D.N.Basu

Nuclear half-lives for α-radioactivity of elements with 100 ≤ Z ≤ 130

NUCLEAR STRUCTURE Z=100-130; calculated α-decay half-lives and Q-values within a WKB framework using microscopic nuclear potentials.

doi: 10.1016/j.adt.2008.01.003
Citations: PlumX Metrics


2008SA17      J.Phys.(London) G35, 065101 (2008)

C.Samanta, P.Roy Chowdhury, D.N.Basu

Lambda hyperonic effect on the normal drip lines

NUCLEAR STRUCTURE Li, Be, B, C, N, O, F, Ne, Na, Mg, Al, Si, P, S, Cl, Ar, K, Ca, Sc, Ti, V, Cr, Mn, Fe, Co, Ni, Cu, Zn, Ga, Ge, As, Se, Br, Kr, Rb, Sr, Y, Zr, Nd, Mo, Tc; calculated proton and neutron separation energies for normal and lambda hypernuclei using a generalized mass formula.

doi: 10.1088/0954-3899/35/6/065101
Citations: PlumX Metrics


2007CH36      Phys.Rev. C 75, 047306 (2007)

P.R.Chowdhury, D.N.Basu, C.Samanta

α decay chains from element 113

RADIOACTIVITY 278,283,284Nh, 274,279,280Rg, 270,275,276Mt, 266,272Bh(α); calculated T1/2. Density-dependent effective nucleon-nucleon interaction.

doi: 10.1103/PhysRevC.75.047306
Citations: PlumX Metrics


2007SA49      Nucl.Phys. A789, 142 (2007)

C.Samanta, P.R.Chowdhury, D.N.Basu

Predictions of alpha decay half lives of heavy and superheavy elements

RADIOACTIVITY 271Sg, 266,271Bh, 275Hs, 270,275,276Mt, 279Ds, 274,279,280Rg, 283,285Cn, 278,283,284Nh, 286,287,288,289Fl, 287,288Mc, 290,291,292,293Lv, 294Og(α); calculated T1/2 by calculating QM tunneling probabilities in a WKB framework. Compared results to available data.

doi: 10.1016/j.nuclphysa.2007.04.001
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2007SA58      J.Phys.Soc.Jpn. 76, 124201 (2007)

C.Samanta, D.N.Basu, P.Roy Chowdhury

Quantum Tunneling in 277112 and Its α-Decay Chain

RADIOACTIVITY 257No, 261Rf, 265Sg, 269Hs, 273Ds, 277Cn(α); calculated T1/2 in WKB framework using DDM3Y interaction, Q-values from the mass formula of Muntian-Hofmann-Patyk-Sobiczeski. Comparisons with experimental data.

doi: 10.1143/JPSJ.76.124201
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2006AD19      Phys.Rev. C 74, 024602 (2006)

S.Adhikari, C.Samanta, C.Basu, B.J.Roy, S.Ray, A.Srivastava, K.Ramachandran, V.Tripathi, K.Mahata, V.Jha, P.Shukla, S.Rathi, M.Biswas, P.R.Chowdhury, A.Chatterjee, S.Kailas

Reaction mechanisms with loosely bound nuclei 7Li+6Li at forward angles in the incident energy range 14-20 MeV

NUCLEAR REACTIONS 6Li(7Li, pX), (7Li, dX), (7Li, tX), (7Li, αX), E=14-20 MeV; measured light charged particle yields, spectra, σ(E, θ); deduced reaction mechanism features. Comparison with model predictions.

doi: 10.1103/PhysRevC.74.024602
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6047.


2006BA68      Acta Phys.Pol. B37, 2869 (2006)

D.N.Basu, P.R.Chowdhury, C.Samanta

Equation of state for isospin asymmetric nuclear matter using Lane potential


2006CH04      Phys.Rev. C 73, 014612 (2006)

P.R.Chowdhury, C.Samanta, D.N.Basu

α decay half-lives of new superheavy elements

RADIOACTIVITY 274,276,278,280,282,284,286,288,290,292Rf, 271,278,280,282,284,286,288,290,292,294Sg, 275,282,284,286,288,290,292,294,296Hs, 279,286,288,290,292,294,296,298Ds, 283,285,288,290,292,294,296,298,300Cn, 286,287,288,289,290,292,294,296,298,300,302Fl, 284,286,288,290,291,292,293,294,296,298,300,302,304Lv, 288,290,292,294,296,298,300,302,304Og, 292,294,296,298,300,302,304,306120(α); calculated Qα, T1/2. Double-folding model, comparison with data and previous calculations.

doi: 10.1103/PhysRevC.73.014612
Citations: PlumX Metrics


2006SA05      J.Phys.(London) G32, 363 (2006)

C.Samanta, P.R.Chowdhury, D.N.Basu

Generalized mass formula for non-strange and hypernuclei with SU(6) symmetry breaking

NUCLEAR STRUCTURE A=4-210; calculated hyperon binding energies. Generalized mass formula, spin-flavor SU(6) symmetry breaking.

doi: 10.1088/0954-3899/32/3/010
Citations: PlumX Metrics


2006WA18      Phys.Rev. C 74, 014605 (2006)

R.E.Warner, F.Carstoiu, J.A.Brown, F.D.Becchetti, D.A.Roberts, B.Davids, A.Galonsky, R.M.Ronningen, M.Steiner, M.Horoi, J.J.Kolata, A.Nadasen, C.Samanta, J.Schwarzenberg, K.Subotic

Reaction and proton-removal cross sections of 6Li, 7Be, 10B, 9, 10, 11C, 12N, 13, 15O, and 17Ne on Si at 15 to 53 MeV/nucleon

NUCLEAR REACTIONS Si(6Li, X), (7Be, X), (10B, X), (9C, X), (10C, X), (11C, X), (12N, X), (13O, X), (15O, X), (17Ne, X), E=15-53 MeV/nucleon; measured reaction and proton-removal σ. 6Li, 7Be, 10B, 9,10,11C, 12N, 13,15O, 17Ne deduced radii. Comparison with Glauber model predictions.

doi: 10.1103/PhysRevC.74.014605
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1445.


2005AD35      Eur.Phys.J. A 25, Supplement 1, 299 (2005)

S.Adhikari, C.Samanta, C.Basu, S.Ray, A.Chatterjee, S.Kailas

Entrance channel dependence in compound nuclear reactions with loosely bound nuclei

NUCLEAR REACTIONS 6Li(6Li, αX), (7Li, αX), E=14-20 MeV; measured α-spectra. 12C(n, α), E=72.8 MeV; 28Si(6Li, α), E=36 MeV; analyzed α-spectra. Statistical model calculations. Target-projectile symmetry discussed.

doi: 10.1140/epjad/i2005-06-066-4
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6009.


2005BA97      Phys.Rev. C 72, 051601 (2005)

D.N.Basu, P.R.Chowdhury, C.Samanta

Folding model analysis of proton radioactivity of spherical proton emitters

RADIOACTIVITY 105Sb, 145,147Tm, 150,151Lu, 155,156,157Ta, 160,161Re, 164,165,166,167Ir, 171Au, 177Tl, 185Bi(p); calculated proton decay T1/2 for ground and isomeric states. Folding model, global proton optical potential, comparison with data.

doi: 10.1103/PhysRevC.72.051601
Citations: PlumX Metrics


2005KA49      Eur.Phys.J. A 25, Supplement 1, 261 (2005)

R.Kanungo, M.Chiba, B.Abu-Ibrahim, S.Adhikari, D.Q.Fang, N.Iwasa, K.Kimura, K.Maeda, S.Nishimura, T.Ohnishi, A.Ozawa, C.Samanta, T.Suda, T.Suzuki, Q.Wang, C.Wu, Y.Yamaguchi, K.Yamada, A.Yoshida, T.Zheng, I.Tanihata

A new view to the structure of 19C

NUCLEAR REACTIONS Be(19C, 18CX), (19C, 17CX), E not given; measured longitudinal momentum distributions; deduced role of neutron evaporation. Comparison with Glauber model calculations.

doi: 10.1140/epjad/i2005-06-183-0
Citations: PlumX Metrics


2005KA51      Eur.Phys.J. A 25, Supplement 1, 327 (2005)

R.Kanungo, M.Chiba, B.Abu-Ibrahim, S.Adhikari, D.Q.Fang, N.Iwasa, K.Kimura, K.Maeda, S.Nishimura, T.Ohnishi, A.Ozawa, C.Samanta, T.Suda, T.Suzuki, Q.Wang, C.Wu, Y.Yamaguchi, K.Yamada, A.Yoshida, T.Zheng, I.Tanihata

Observation of a two-proton halo in 17Ne

NUCLEAR REACTIONS Be(17Ne, 15OX), E=64 MeV/nucleon; measured fragments longitudinal momentum distributions, interaction σ. 17Ne deduced two-proton halo features. Few-body Glauber model analysis.

doi: 10.1140/epjad/i2005-06-184-y
Citations: PlumX Metrics


2004AD29      Int.J.Mod.Phys. E13, 987 (2004)

S.Adhikari, C.Samanta

Systematic study of shell effect near drip-lines

NUCLEAR STRUCTURE Z=4-98; analyzed binding energies, particle separation energies; deduced shell effects. Modified Bethe-Weiszacker formula.

doi: 10.1142/S0218301304002570
Citations: PlumX Metrics


2004CH43      Nucl.Phys. A741, 29 (2004)

M.Chiba, R.Kanungo, B.Abu-Ibrahim, S.Adhikari, D.Q.Fang, N.Iwasa, K.Kimura, K.Maeda, S.Nishimura, T.Ohnishi, A.Ozawa, C.Samanta, T.Suda, T.Suzuki, I.Tanihata, Q.Wang, C.Wu, Y.Yamaguchi, K.Yamada, A.Yoshida, T.Zheng

Neutron removal studies on 19C

NUCLEAR REACTIONS Be(19C, 18CX), (19C, 17CX), E=64 MeV/nucleon; measured one- and two-neutron removal σ, longitudinal momentum distributions. Comparison with previous results.

doi: 10.1016/j.nuclphysa.2004.06.009
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1906.


2004JE07      Nucl.Phys. A739, 57 (2004)

H.Jeppesen, R.Kanungo, B.Abu-Ibrahim, S.Adhikari, M.Chiba, D.Fang, N.Iwasa, K.Kimura, K.Maeda, S.Nishimura, T.Ohnishi, A.Ozawa, C.Samanta, T.Suda, T.Suzuki, I.Tanihata, Q.Wang, C.Wu, Y.Yamaguchi, K.Yamada, A.Yoshida, T.Zheng

One- and two-proton removal from 15O

NUCLEAR REACTIONS Be(15O, 14NX), (15O, 13CX), E=56 MeV/nucleon; measured parallel momentum distributions. 15O deduced valence proton configuration. 17Ne deduced halo features.

doi: 10.1016/j.nuclphysa.2004.03.145
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1902.


2004SA33      Nucl.Phys. A738, 491 (2004)

C.Samanta, S.Adhikari

Shell effect in Pb isotopes near the proton drip line

NUCLEAR STRUCTURE Pb; analyzed masses, proton separations energies, shell effects.

doi: 10.1016/j.nuclphysa.2004.04.094
Citations: PlumX Metrics


2004SA50      Acta Phys.Hung.N.S. 19, 161 (2004)

C.Samanta

A New Mass Formula and New Neutron and Proton Magic Numbers in Light Nuclei

NUCLEAR STRUCTURE 5,6,7,8,9,10,11,12,13,14Be; calculated binding energies. Z=64-92; calculated proton separation energies. Comparisons with data.

doi: 10.1556/APH.19.2004.1-2.25
Citations: PlumX Metrics


2003KA43      Phys.Lett. B 571, 21 (2003)

R.Kanungo, M.Chiba, S.Adhikari, D.Fang, N.Iwasa, K.Kimura, K.Maeda, S.Nishimura, Y.Ogawa, T.Ohnishi, A.Ozawa, C.Samanta, T.Suda, T.Suzuki, Q.Wang, C.Wu, Y.Yamaguchi, K.Yamada, A.Yoshida, T.Zheng, I.Tanihata

Possibility of a two-proton halo in 17Ne

NUCLEAR REACTIONS 9Be(17Ne, X), E=66 MeV/nucleon; measured particle spectra, longitudinal momentum distribution, two-proton removal σ. 17Ne deduced two-proton halo features.

doi: 10.1016/j.physletb.2003.07.050
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1818.


2002GU02      J.Phys.(London) G28, 85 (2002)

D.Gupta, C.Samanta

Inelastic Scattering of Protons from 6, 8He and 7, 11Li in a Folding Model Approach

NUCLEAR REACTIONS 6,8He, 7,11Li(p, p), (p, p'), E ≈ 40-70 MeV; calculated σ(θ). Folding model, comparisons with data.

doi: 10.1088/0954-3899/28/1/306
Citations: PlumX Metrics


2002KA20      Phys.Rev.Lett. 88, 142502 (2002); Comment Phys.Rev.Lett. 90, 159201 (2003)

R.Kanungo, M.Chiba, N.Iwasa, S.Nishimura, A.Ozawa, C.Samanta, T.Suda, T.Suzuki, T.Yamaguchi, T.Zheng, I.Tanihata

Experimental Evidence of Core Modification in the Near Drip-Line Nucleus 23O

NUCLEAR REACTIONS C(23O, X), E=72 MeV/nucleon; measured one- and two-neutron removal σ, projectile-like fragments longitudinal momentum distributions. 23O deduced halo configuration, core modification.

doi: 10.1103/PhysRevLett.88.142502
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1779.


2002SA08      Phys.Rev. C65, 037301 (2002); Comment Phys.Rev. C 69, 049803 (2004)

C.Samanta, S.Adhikari

Extension of the Bethe-Weizsacker Mass Formula to Light Nuclei and Some New Shell Closures

NUCLEAR STRUCTURE C, Li, Bi; calculated binding energy per nucleon. Z=4-17; calculated one-neutron separation energies. 26O, 32Ne, 35Na, 38Mg, 41Al; calculated one- and two-neutron separation energies. New shell closures discussed.

doi: 10.1103/PhysRevC.65.037301
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2001GU09      Nucl.Phys. A683, 3 (2001)

D.Gupta, C.Samanta, A.Chatterjee, S.Kailas, B.J.Roy, K.Mahata, A.Shrivastava

Measurement of 42 MeV 7Li Projectile Breakup on 208Pb Target Near Grazing Incidence

NUCLEAR REACTIONS 208Pb(7Li, 7Li), E=42 MeV; measured σ(θ). 208Pb(7Li, X), (7Li, tα), E=42 MeV; measured elastic, direct, and sequential breakup particle spectra, σ(E, θ); deduced reaction mechanism features. 197Au(7Li, tα), E=54 MeV; 208Pb(7Li, tα), E=63 MeV; analyzed σ(E, θ).

doi: 10.1016/S0375-9474(00)00452-8
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0417.


2001GU32      Pramana 57, 209 (2001)

D.Gupta, C.Samanta, R.Kanungo, P.Basu, S.Roy, S.Kailas, A.Chatterjee, B.J.Roy, K.Mahata, A.Samant, A.Shrivastava

Breakup of 42 MeV 7Li Projectiles in the Fields of 12C and 197Au Nuclei

NUCLEAR REACTIONS 12C, 197Au(7Li, tα), E=42 MeV; measured Eα, triton spectra, σ(E, θ). Comparison with Serber model predictions.

doi: 10.1007/s12043-001-0177-7
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6112.


2001SA79      Pramana 57, 519 (2001)

C.Samanta

Physics with Loosely Bound Nuclei

NUCLEAR REACTIONS 4,6,8He, 6,7,9,11Li(p, p), (p, p'), E=25-75 MeV; analyzed σ(θ); deduced halo and resonance features. Folding model.

doi: 10.1007/s12043-001-0058-0
Citations: PlumX Metrics


2000GU17      J.Phys.(London) G26, L81 (2000)

D.Gupta, C.Samanta, A.Chatterjee, K.Rusek, Y.Hirabayashi

Channel Coupling Effects in Resonant Breakup of 42 MeV 7Li with 58Ni Target

NUCLEAR REACTIONS 58Ni(7Li, 7Li'), E=42 MeV; measured σ(θ) for elastic scattering and sequential α + t breakup of projectile. Comparison with coupled channel calculations.

doi: 10.1088/0954-3899/26/6/102
Citations: PlumX Metrics


2000GU19      Nucl.Phys. A674, 77 (2000)

D.Gupta, C.Samanta, R.Kanungo

Consistent Analysis of Proton Elastic Scattering from 4, 6, 8He and 6, 7, 9, 11Li in the Energy Range of 25-75 AMeV

NUCLEAR REACTIONS 4,6,8He, 6,7,9,11Li(p, p), E=25-75 MeV; analyzed σ(θ); deduced renormalization factors, channel coupling effects. Folding model, momentum-dependent interaction.

doi: 10.1016/S0375-9474(00)00159-7
Citations: PlumX Metrics


2000GU21      Acta Phys.Pol. B31, 471 (2000)

D.Gupta, C.Samanta, R.Kanungo

Effect of Smeared 4He-Core in 6He + p Elastic Scattering

NUCLEAR REACTIONS 4,6He(p, p), E=40-45 MeV; analyzed σ(θ); deduced possible role of smeared core vs halo structure.


2000SC11      Eur.Phys.J. A 7, 367 (2000)

K.Schwarz, C.Samanta, M.Fujiwara, H.Rebel, R.De Leo, N.Matsuoka, H.Utsunomiya, H.Akimune, I.Daito, H.Fujimura, F.Ihara, K.Ishibashi, Y.Maeda, T.Yamanaka, H.Yoshida, A.Okihana, T.Yoshimura, P.K.J.van Aarle, W.A.T.Uijen, M.Ito, Y.Sakuragi

Reaction Mechanism of 6Li Scattering at 600 MeV

NUCLEAR REACTIONS 12C, 58Ni, 90Zr, 208Pb(6Li, 6Li), (6Li, dα), E= 600 MeV; measured elastic and breakup σ(θ), particle spectra. Comparison with theoretical calculations.

doi: 10.1007/PL00013619
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1725.


1999GU02      Nucl.Phys. A646, 161 (1999)

D.Gupta, C.Samanta, R.Kanungo, M.K.Sharan, S.Kailas, A.Chatterjee, K.Mahata, A.Shrivastava

Measurement of 42 MeV 7Li Projectile Breakup on 58Ni Target Beyond Grazing Incidence

NUCLEAR REACTIONS 58Ni(7Li, 7Li), E=42 MeV; measured σ(θ). 58Ni(7Li, X), E=42 MeV; measured particle spectra. 58Ni(7Li, tα), E=42 MeV; measured Eα, Et, σ(θ(α), θ(t), Eα); deduced sequential breakup contribution.

doi: 10.1016/S0375-9474(98)00635-6
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0441.


1999KA68      Prog.Theor.Phys.(Kyoto) 102, 1133 (1999)

R.Kanungo, I.Tanihata, C.Samanta

Soft Dipole Resonance in 11Li

NUCLEAR REACTIONS 1H(11Li, 11Li), (11Li, X), E=68 MeV/nucleon; analyzed σ(E, θ). 11Li deduced soft dipole resonance. Microscopic approach.

doi: 10.1143/PTP.102.1133
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1998EJ03      Phys.Lett. 433B, 257 (1998)

H.Ejiri, H.Akimune, Y.Arimoto, I.Daito, H.Fujimura, Y.Fujita, M.Fujiwara, K.Fushimi, M.B.Greenfield, M.N.Harakeh, F.Ihara, T.Inomata, K.Ishibashi, J.Janecke, H.Kohri, S.Nakayama, C.Samanta, A.Tamii, M.Tanaka, H.Toyokawa, M.Yosoi

Spin-Isospin Responses of 71Ga for Solar Neutrinos Studied by 71Ga(3He, tγ)71Ge Reaction

NUCLEAR REACTIONS 71Ga(3He, t), E=450 MeV; measured Eγ, Iγ, forward-angle triton spectra, tγ-coin. 71Ge deduced γ-decay branching from levels above neutron threshold. Implications for solar neutrino absorption rates.

doi: 10.1016/S0370-2693(98)00673-X
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1998KA33      J.Phys.(London) G24, 1611 (1998)

R.Kanungo, C.Samanta

Is the 1.3 MeV Excited State of 11Li a Signature of Pygmy Resonance ?

NUCLEAR REACTIONS 11Li(p, p'), E=68 MeV; analyzed data. 11Li deduced pygmy resonance.

doi: 10.1088/0954-3899/24/8/040
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1998WA16      Nucl.Phys. A635, 292 (1998)

R.E.Warner, H.Thirumurthy, J.Woodroffe, F.D.Becchetti, J.A.Brown, B.S.Davids, A.Galonsky, J.J.Kolata, J.J.Kruse, M.Y.Lee, A.Nadasen, T.W.O'Donnell, D.A.Roberts, R.M.Ronningen, C.Samanta, P.Schwandt, J.von Schwarzenberg, M.Steiner, K.Subotic, J.Wang, J.A.Zimmerman

Reaction Cross Sections in Si of Light Proton-Halo Candidates 12N and 17Ne

NUCLEAR REACTIONS Si(12N, X), (15O, X), (17Ne, X), E=29-53 MeV/nucleon; measured total reaction σ, charge-removal σ; deduced dependence on proton separation energy. Radioactive beams, Glauber model, proton-halo nuclei.

doi: 10.1016/S0375-9474(98)00163-8
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1998YO09      Nucl.Phys. A641, 3 (1998)

T.Yoshimura, A.Okihana, R.E.Warner, N.S.Chant, P.G.Roos, C.Samanta, S.Kakigi, N.Koori, M.Fujiwara, N.Matsuoka, K.Tamura, E.Kubo, K.Ushiro

Alpha Spectroscopic Factors for 6Li, 7Li, 9Be and 12C from the (p(pol), pα) Reaction at 296 MeV

NUCLEAR REACTIONS 6,7Li, 9Be, 12C(polarized p, pα), E=296 MeV; measured σ(θ(p), θ(α), Ep), Ay; deduced alpha spectroscopic factor. Projected energy spectrum, analyzing power distributions, quasifree scattering, distorted wave impulse approximation.

doi: 10.1016/S0375-9474(98)00432-1
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1997KA19      Nucl.Phys. A617, 265 (1997)

R.Kanungo, C.Samanta

Halo Structure of 11Li in Proton Scattering: A folding model description with isospin, density and momentum dependent effective interaction

NUCLEAR REACTIONS 11Li(p, p), (p, p'), E=62-75 MeV; analyzed σ(θ); deduced model parameters. 11Li deduced dipole excitation related features. Single folding model, isospin, density, momentum dependent finite range effective interactions.

doi: 10.1016/S0375-9474(97)00010-9
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1997SA57      J.Phys.(London) G23, 1697 (1997)

C.Samanta, Y.Sakuragi, M.Ito, M.Fujiwara

Energy Dependence of the 6Li-Nucleus Interactions at Intermediate Energies

NUCLEAR REACTIONS 12C, 28Si, 58Ni, 120Sn, 208Pb(6Li, 6Li)E=20, 100 MeV/nucleon; calculated σ(θ); deduced projectile breakup channel energy dependence. Coupled channels calculations, energy, density dependent interaction. Other models compared.

doi: 10.1088/0954-3899/23/11/017
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1997SA69      Prog.Theor.Phys.(Kyoto) 98, 521 (1997)

Y.Sakuragi, M.Ito, Y.Hirabayashi, C.Samanta

Breakup Effect on the 6Li Elastic Scattering from 28Si at E/A = 35 and 53 MeV

NUCLEAR REACTIONS 28Si(6Li, 6Li), E=35, 53 MeV/nucleon; analyzed σ(θ); deduced projectile breakup channel role. Double-folding model interactions.

doi: 10.1143/PTP.98.521
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1996KA11      Nucl.Phys. A599, 579 (1996)

R.Kanungo, T.Sinha, C.Samanta, S.Roy, A.Chatterjee, B.J.Roy, S.Ray

Wide-Angle Measurement of 48 MeV 6Li Projectile Fragmentation on 197Au

NUCLEAR REACTIONS 197Au(6Li, 6Li), (6Li, α), (6Li, d), (6Li, dα), E=48 MeV; measured σ(θ). DWBA analysis, breakup.

doi: 10.1016/0375-9474(95)00480-7
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1996SA10      Phys.Rev. C53, 2287 (1996)

C.Samanta, S.Mukherjee, R.Kanungo, D.N.Basu

Deuteron Breakup at Extreme Forward Angles: Failure of a pure Coulomb dissociation description

NUCLEAR REACTIONS 12C, 40Ca, 208Pb(d, np), E=56 MeV; analyzed σ(θp, θn, Ep); deduced reaction mechanism related features.

doi: 10.1103/PhysRevC.53.2287
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1996SI13      Z.Phys. A355, 397 (1996)

T.Sinha, R.Kanungo, C.Samanta, S.Ghosh, P.Basu, H.Rebel

Coupling Effects of Resonant and Discretized Non-Resonant Continuum States in 4He + 6Li Scattering at 10 MeV/A

NUCLEAR REACTIONS 6Li(α, α'), (α, α), E=40 MeV; analyzed σ(θ); deduced nonresonant continuum states coupling strengths related features. Coupled-channels approach.

doi: 10.1007/s002180050128
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1995KA03      Nucl.Phys. A581, 294 (1995)

R.Kanungo, C.Samanta, S.Roy, S.K.Samaddar

Analysing Power Puzzle of p + 6Li Scattering: Consistent analysis with density and momentum dependent finite range effective interaction

NUCLEAR REACTIONS 6Li(polarized p, p), (polarized p, p'), E=10-136 MeV; analyzed σ(θ), analyzing power vs θ. 6Li(e, e'), (e, e), E not given; analyzed charge, transition density data; deduced density distributions. Single folding model, density, momentum dependent finite range effective interaction.

doi: 10.1016/0375-9474(94)00444-R
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1995KA07      Z.Phys. A351, 9 (1995)

R.Kanungo, M.Lahiri, C.Samanta, H.Rebel

Continuum-Continuum Coupling with Discretized 6Li → α + d Breakup Continuum Data

NUCLEAR REACTIONS 6Li(α, α'), (α, α), E=50 MeV; 6Li(p, p), (p, p'), E=65 MeV; analyzed σ(θ); deduced minimal continuum-continuum coupling.

doi: 10.1007/BF01292779
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1995KA43      Int.J.Mod.Phys. E4, 827 (1995)

R.Kanungo, M.Lahiri, C.Samanta, H.Rebel

Studies of Continuum Coupling Effects in 6Li(α, α') and 6Li(p, p') Excitation

NUCLEAR REACTIONS 6Li(p, p'), E=65 MeV; 6Li(α, α'), E=50 MeV; analyzed σ(θ); deduced marginal coupling due to multi-step processes. Realistic coupled-channels approach.

doi: 10.1142/S0218301395000298
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1995SA39      Phys.Lett. 352B, 197 (1995)

C.Samanta, R.Kanungo, S.Mukherjee, D.N.Basu

Coulomb-Nuclear Interference in 56 MeV Deuteron Breakup at Extreme Forward Angle

NUCLEAR REACTIONS 12C(d, np), E=56 MeV; analyzed σ(θ), σ(θp, θn, Ep); deduced Coulomb-nuclear interference role, optical potential features. Prior form DWBA.

doi: 10.1016/0370-2693(95)00515-M
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1994SA32      Phys.Rev. C50, 1226 (1994)

C.Samanta, T.Sinha, S.Ghosh, S.Ray, S.R.Banerjee

4He Induced 6Li → α + d Target Breakup in the Region of Small Relative Fragment Energies

NUCLEAR REACTIONS 6Li(α, α'), E=40 MeV; measured continuum σ(Eα, θα); deduced onset of Coulomb dissociation, 6Li breakup critical momentum transfer value features.

doi: 10.1103/PhysRevC.50.1226
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1993MA41      Phys.Rev. C48, 2093 (1993)

M.M.Majumdar, J.N.De, C.Samanta, S.K.Samaddar

Role of Nuclear Compressibility on the Fission Path

NUCLEAR STRUCTURE 238U, 208Pb; calculated equilibrium density along fission path, deformation energy, volume, Coulomb, surface contributions; deduced nuclear compressibility role. Semi-macroscopic framework.

doi: 10.1103/PhysRevC.48.2093
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1993SA10      Phys.Rev. C47, 1313 (1993)

C.Samanta, M.Lahiri, S.Roy, S.Ray, S.R.Banerjee

Distored-Wave Analysis of Proton Scattering from 6Li Near the α-d Breakup Threshold

NUCLEAR REACTIONS 6Li(p, p'), E=65 MeV; analyzed σ(θp, Ep) data; deduced breakup fragment recombination role. DWIA, DWBA analyses.

doi: 10.1103/PhysRevC.47.1313
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1993SI06      Phys.Rev. C47, 2994 (1993)

T.Sinha, S.Roy, C.Samanta

3He Scattering from 6Li: A semimicroscopic approach

NUCLEAR REACTIONS 6Li(3He, 3He), E=30-72 MeV; calculated σ(θ); deduced model parameters. Microscopic potential, semi-microscopic approach.

doi: 10.1103/PhysRevC.47.2994
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1993SI09      Phys.Rev. C48, 785 (1993)

T.Sinha, S.Roy, C.Samanta

Double-Folding Model Potential for 6Li Scattering with 4He: Absence of anomalous reduction factor

NUCLEAR REACTIONS 6Li(α, α), (α, X), E=36.6-166 MeV; analyzed σ(θ); deduced no anomalous reduction factor. Double-folding model, microscopic potential, single nucleon exchange term.

doi: 10.1103/PhysRevC.48.785
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1992SA01      Phys.Rev. C45, 1757 (1992)

C.Samanta, S.Ghosh, M.Lahiri, S.Ray, S.R.Banerjee

Alpha-Particle Scattering from 6Li Near the α-d Breakup Threshold

NUCLEAR REACTIONS 6Li(α, α'), (α, α), E=50 MeV; measured σ(θ), σ(θα, Eα); deduced breakup cluster recombination role in exit channel. DWBA analysis.

doi: 10.1103/PhysRevC.45.1757
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1990BA17      Nucl.Phys. A511, 1 (1990)

D.Bandyopadhyay, C.Samanta, S.K.Samaddar, J.N.De

Thermostatic Properties of Finite and Infinite Nuclear Systems

NUCLEAR STRUCTURE A=50-200; calculated limiting temperature vs mass number.

doi: 10.1016/0375-9474(90)90024-G
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1990MU04      J.Phys.(London) G16, L107 (1990)

P.Mukherjee, P.Sen, I.Mukherjee, C.Samanta

Evidence of New High Spin States Excited in the 209Bi(α, 4n)209At Reaction

NUCLEAR REACTIONS 209Bi(α, 4n), E=52 MeV; measured Eγ, Iγ, γγ-coin. 209At deduced levels, J, π, γ-multipolarity, γ-branching.

doi: 10.1088/0954-3899/16/7/002
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1989DA04      Phys.Rev. C39, 1281 (1989)

S.K.Datta, S.Ray, H.Majumdar, S.K.Ghosh, C.Samanta, S.Ray, P.Dasgupta, S.N.Chintalapudi, S.R.Banerjee

Neutron Transition Multipole Moment for 88Sr(α, α')88Sr(*)(2+, 1.84 MeV)

NUCLEAR REACTIONS 88Sr(α, α'), (α, α), E=50 MeV; measured σ(θ), σ(Eα); deduced model, vibrational parameters. 88Sr level deduced neutron transition multipole moment. Microscopic DWBA analysis.

doi: 10.1103/PhysRevC.39.1281
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1989JE01      Z.Phys. A332, 317 (1989)

H.Jelitto, J.Buschmann, V.Corcalciuc, H.J.Gils, N.Heide, J.Kiener, H.Rebel, C.Samanta, S.Zagromski

Inclusive Measurements of the Break-Up of 156 MeV 6Li-Ions at Extreme Forward Angles

NUCLEAR REACTIONS 12C, 208Pb(6Li, αX), (6Li, dX), E=156 MeV; measured σ(θα), σ(θd), inclusive reaction σ(θα, Eα), σ(θd, Ed); deduced reaction, projectile breakup mechanisms.


1989SA59      Phys.Lett. B 217, 381 (1989)

C.Samanta, D.Bandyopadhyay, J.N.De

Incompressibility of asymmetric nuclear matter

doi: 10.1016/0370-2693(89)90064-6
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1987MU14      Phys.Rev. C36, 1197 (1987)

P.Mukherjee, I.Mukherjee, P.Sen, C.Samanta

Angular Momentum Saturation in the 209Bi(α, 2n) Reaction

NUCLEAR REACTIONS 209Bi(α, 2n), E=34-52 MeV; measured Eγ, Iγ; deduced residual nucleus isomer yields, evaporation residue average angular momentum.

doi: 10.1103/PhysRevC.36.1197
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1987MU17      Phys.Rev. C36, 2618 (1987)

P.Mukherjee, C.Samanta, I.Mukherjee

3s1/2 Spectroscopic Strength Distribution in 207Tl and 205Tl

NUCLEAR STRUCTURE 205,207Tl; calculated proton hole state fragmentation, spectroscopic strengths.

doi: 10.1103/PhysRevC.36.2618
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1987SA01      Phys.Rev. C35, 333 (1987)

C.Samanta, N.S.Chant, P.G.Roos, A.Nadasen, A.A.Cowley

16O(α, αp) and 40Ca(α, αp) Reactions at 139.2 MeV Incident Energy

NUCLEAR REACTIONS 16O, 40Ca(α, pα), E=139.2 MeV; measured σ(θα, Eα, θp). 39K, 15N levels deduced spectroscopic factors. ΔE-E telescopes. DWIA calculations.

doi: 10.1103/PhysRevC.35.333
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1986MU17      Nucl.Instrum.Methods Phys.Res. A251, 191 (1986)

P.Mukherjee, P.Sen, I.Mukherjee, C.Samanta

On-Line Neutron Response of a Ge-NaI(Tl) Anti-Compton Spectrometer

NUCLEAR REACTIONS 197Au, 209Bi(α, xnγ), E=52 MeV; measured Eγ; deduced residual γ-emitting source, detector neutron response. Ge-NaI(Tl) anti-Compton spectrometer.

doi: 10.1016/0168-9002(86)91167-8
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1986SA24      Phys.Rev. C34, 1610 (1986)

C.Samanta, N.S.Chant, P.G.Roos, A.Nadasen, J.Wesick, A.A.Cowley

Tests of the Factorized Distorted Wave Impluse Approximation for (p, 2p) Reactions

NUCLEAR REACTIONS 40Ca, 16O(p, 2p), E=76.1, 101.3 MeV; measured σ(θ1, θ2, Ep1). 39K, 15N levels deduced L, spectroscopic factors. ΔE-E telescopes. DWIA analysis.

doi: 10.1103/PhysRevC.34.1610
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1985SA34      Phys.Rev. C32, 2217 (1985)

C.Samanta, I.Mukherjee, P.Mukherjee

Structure of High-Spin Proton States in 208Pb

NUCLEAR REACTIONS 208Pb(α, t), E not given; analyzed data; deduced spectroscopic strength distributions for 2g9/2, 1i11/2, 1i13/2, and 1j15/2 proton states in 209Bi. Particle core vibration model.

doi: 10.1103/PhysRevC.32.2217
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1983MU17      Phys.Rev. C28, 1396 (1983)

P.Mukherjee, R.Bhattacharya, C.Samanta

Effect of Core Polarization on the Charge Distribution in 208Pb

NUCLEAR STRUCTURE 208Pb; calculated charge distribution Fourier-Bessel expansion coefficient potential dependence; deduced core polarization effect. Different potentials.

doi: 10.1103/PhysRevC.28.1396
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1982SA24      Phys.Rev. C26, 1379 (1982)

C.Samanta, N.S.Chant, P.G.Roos, A.Nadasen, A.A.Cowley

Discrepancy between Proton- and Alpha-Induced Cluster Knockout Reactions on 16O

NUCLEAR REACTIONS 16O(p, pd), (p, pt), E=101.3 MeV; 16O(α, dα), (α, tα), (α, 3Heα), E=139.2 MeV; measured σ(E1, E2, θ1, θ2). 14,13N, 13C levels deduced L, S. DWIA analysis.

doi: 10.1103/PhysRevC.26.1379
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1981NA03      Phys.Rev. C23, 2353 (1981)

A.Nadasen, P.G.Roos, N.S.Chant, A.A.Cowley, C.Samanta, J.Wesick

40Ca(p, pα)36Ar Reaction in a Noncoplanar Geometry

NUCLEAR REACTIONS 40Ca(p, pα), E=101.3 MeV; measured σ(θp, θα, Ep). 40Ca level deduced Sα. DWIA analysis.

doi: 10.1103/PhysRevC.23.2353
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1980CO19      Phys.Rev.Lett. 45, 1930 (1980)

A.A.Cowley, C.C.Chang, H.D.Holmgren, J.D.Silk, D.L.Hendrie, R.W.Koontz, P.G.Roos, C.Samanta, J.R.Wu

Energy Dissipation Process for 100-MeV Protons and the Nucleon-Nucleon Interactions in Nuclei

NUCLEAR REACTIONS 58Ni(p, 2p), E=100 MeV; measured pp-coin, σ(Ep1, Ep2, θ1, θ2); deduced reaction mechanism, energy dissipation process. DWIA analysis, quasifree scattering.

doi: 10.1103/PhysRevLett.45.1930
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1980NA09      Phys.Rev. C22, 1394 (1980)

A.Nadasen, N.S.Chant, P.G.Roos, T.A.Carey, R.Cowen, C.Samanta, J.Wesick

Non-Coplanar (p, pα) and (p, d3He) Reactions on 9Be at 101.5 MeV

NUCLEAR REACTIONS 9Be(p, pα) and 9Be(p, d3He), E(lab)=101.5 MeV; measured σ(E1, E2, θ1, θ2); 9Be level deduced Sα. Noncoplanar geometry. DWIA analysis.

doi: 10.1103/PhysRevC.22.1394
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