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NSR database version of April 11, 2024.

Search: Author = D.Pocanic

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2019BR14      Hyperfine Interactions 240, 1 (2019)

L.J.Broussard, S.Baessler, T.L.Bailey, N.Birge, J.D.Bowman, C.B.Crawford, C.Cude-Woods, D.E.Fellers, N.Fomin, E.Frlez, M.T.W.Gericke, L.Hayen, A.P.Jezghani, H.Li, N.Macsai, M.F.Makela, R.R.Mammei, D.Mathews, P.L.McGaughey, P.E.Mueller, D.Pocanic, C.A.Royse, A.Salas-Bacci, S.K.L.Sjue, J.C.Ramsey, N.Severijns, E.C.Smith, J.Wexler, R.A.Whitehead, A.R.Young, B.A.Zeck

Using Nab to determine correlations in unpolarized neutron decay

RADIOACTIVITY ⁴⁵Ca(β^-); measured decay products, Eβ, Iβ; deduced sensitivity for the ratio of the weak axial-vector and vector coupling constants.

doi: 10.1007/s10751-018-1538-7
Citations: PlumX Metrics

2010PO11      Nucl.Phys. A844, 26c (2010)

D.Pocanic, and the PIBETA Collaboration

Pion, muon decays and weak interaction symmetries

doi: 10.1016/j.nuclphysa.2010.05.009
Citations: PlumX Metrics

2005WI18      J.Res.Natl.Inst.Stand.Technol. 110, 389 (2005)

W.S.Wilburn, J.D.Bowman, G.S.Mitchell, J.M.O'Donnell, S.I.Penttila, P.-N.Seo, J.R.Calarco, F.W.Hersmann, T.E.Chupp, T.V.Cianciolo, K.P.Rykaczewski, G.R.Young, R.T.De Souza, W.M.Snow, D.Desai, G.L.Greene, R.K.Grzywacz, E.Frlez, D.Pocanic, T.R.Gentile, V.Gudkov, G.L.Jones

Measurement of Neutron Decay Parameters-The abBA Experiment

doi: 10.6028/jres.110.058
Citations: PlumX Metrics

1999AN43      Phys.Lett. 463B, 339 (1999)

P.L.Anthony, R.G.Arnold, T.Averett, H.R.Band, M.C.Berisso, H.Borel, P.E.Bosted, S.L.Bultmann, M.Buenerd, T.Chupp, S.Churchwell, G.R.Court, D.Crabb, D.Day, P.Decowski, P.DePietro, R.Erbacher, R.Erickson, A.Feltham, H.Fonvieille, E.Frlez, R.Gearhart, V.Ghazikhanian, J.Gomez, K.A.Griffioen, C.Harris, M.A.Houlden, E.W.Hughes, C.E.Hyde-Wright, G.Igo, S.Incerti, J.Jensen, J.R.Johnson, P.M.King, Yu.G.Kolomensky, S.E.Kuhn, R.Lindgren, R.M.Lombard-Nelsen, J.Marroncle, J.McCarthy, P.McKee, W.Meyer, G.Mitchell, J.Mitchell, M.Olson, S.Penttila, G.Peterson, G.G.Petratos, R.Pitthan, D.Pocanic, R.Prepost, C.Prescott, L.M.Qin, B.A.Raue, D.Reyna, L.S.Rochester, S.Rock, O.A.Rondon-Aramayo, F.Sabatie, I.Sick, T.Smith, L.Sorrell, F.Staley, S.St.Lorant, L.M.Stuart, Z.Szalata, Y.Terrien, A.Tobias, L.Todor, T.Toole, S.Trentalange, D.Walz, R.C.Welsh, F.R.Wesselmann, T.R.Wright, C.C.Young, M.Zeier, H.Zhu, B.Zihlmann

Measurement of the Deuteron Spin Structure Function g₁^d(x) for 1 (GeV/c)² < Q² < 40 (GeV/c)²

NUCLEAR REACTIONS ²H, ⁶Li(polarized e, e'X), E=48.3 GeV; measured electrons σ(θ), longitudinal asymmetries. ²H deduced spin structure function.

doi: 10.1016/S0370-2693(99)00940-5
Citations: PlumX Metrics

1998FR07      Phys.Rev. C57, 3144 (1998)

E.Frlez, D.Pocanic, K.A.Assamagan, J.P.Chen, K.J.Keeter, R.M.Marshall, R.C.Minehart, L.C.Smith, G.E.Dodge, S.S.Hanna, B.H.King, J.N.Knudson

Differential Cross Sections for Pion Charge Exchange on the Proton at 27.5 MeV

NUCLEAR REACTIONS ¹H(π^-, π⁰), E=27.5 MeV; measured σ(θ).

doi: 10.1103/PhysRevC.57.3144
Citations: PlumX Metrics

1998HA24      Nucl.Instrum.Methods Phys.Res. A401, 345 (1998)

S.S.Hanna, C.J.Martoff, D.Pocanic, K.Wang, R.C.Byrd, C.C.Foster, I.J.van Heerden

A Monochromatic Neutron Facility for (n, p) Reactions

NUCLEAR REACTIONS ⁶Li, ¹³C(n, p), E=118 MeV; measured proton spectra.

doi: 10.1016/S0168-9002(97)00985-6
Citations: PlumX Metrics

1998PO01      Nucl.Phys. A629, 201c (1998)

D.Pocanic, E.Frlez

π-N Charge Exchange and π⁺-π⁰ Scattering at Low Energies

NUCLEAR REACTIONS ¹H(π^-, π⁰), E=27.5 MeV; measured σ(θ); ¹H(π⁺, π⁺π⁰), E=260 MeV; measured σ; deduced chiral symmetry breaking related features.

doi: 10.1016/S0375-9474(97)00687-8
Citations: PlumX Metrics

1996AB02      Phys.Rev.Lett. 76, 587 (1996)

K.Abe, T.Akagi, P.L.Anthony, R.Antonov, R.G.Arnold, T.Averett, H.R.Band, J.M.Bauer, H.Borel, P.E.Bosted, V.Breton, J.Button-Shafer, J.P.Chen, T.E.Chupp, J.Clendenin, C.Comptour, K.P.Coulter, G.Court, D.Crabb, M.Daoudi, D.Day, F.S.Dietrich, J.Dunne, H.Dutz, R.Erbacher, J.Fellbaum, A.Feltham, H.Fonvieille, E.Frlez, D.Garvey, R.Gearhart, J.Gomez, P.Grenier, K.A.Griffioen, S.Hoibraten, E.W.Hughes, C.Hyde-Wright, J.R.Johnson, D.Kawall, A.Klein, S.E.Kuhn, M.Kuriki, R.Lindgren, T.J.Liu, R.M.Lombard-Nelsen, J.Marroncle, T.Maruyama, X.K.Maruyama, J.McCarthy, W.Meyer, Z.-E.Meziani, R.Minehart, J.Mitchell, J.Morgenstern, G.G.Petratos, R.Pitthan, D.Pocanic, C.Prescott, R.Prepost, P.Raines, B.Raue, D.Reyna, A.Rijllart, Y.Roblin, L.S.Rochester, S.E.Rock, O.A.Rondon, I.Sick, L.C.Smith, T.B.Smith, M.Spengos, F.Staley, P.Steiner, S.St.Lorant, L.M.Stuart, F.Suekane, Z.M.Szalata, H.Tang, Y.Terrien, T.Usher, D.Walz, J.L.White, K.Witte, C.C.Young, B.Youngman, H.Yuta, G.Zapalac, B.Zihlmann, D.Zimmermann, and the E143 Collaboration

Measurements of the Proton and Deuteron Spin Structure Function g₂ and Asymmetry A₂

NUCLEAR STRUCTURE ^1,2H; analyzed data; deduced spin structure function, asymmetry data. Polarized ammonia targets, (polarized e, e') reaction.

NUCLEAR REACTIONS ^1,2H(polarized e, e'), E=29.1 GeV; measured spin asymmetries. ^1,2H deduced spin structure functions. Polarized ammonia targets.

doi: 10.1103/PhysRevLett.76.587
Citations: PlumX Metrics

1996MA58      Phys.Rev. C54, 2767 (1996)

C.J.Martoff, S.S.Hanna, D.Pocanic, K.Wang, W.J.Cummings, R.C.Byrd, C.C.Foster

Reaction ¹³C(n, p)¹³B at 118 MeV

NUCLEAR REACTIONS ¹³C(n, p), E=118 MeV; measured σ(θ), proton spectra; deduced nucleon-nucleon interaction spin-isospin component central part volume integral, (n, p), (p, n) reaction σ universal proportionality energy dependence.

doi: 10.1103/PhysRevC.54.2767
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13951.

1996WA06      Phys.Rev. C53, 1718 (1996)

K.Wang, C.J.Martoff, D.Pocanic, S.S.Hanna, F.P.Brady, J.L.Romero, C.M.Castaneda, J.R.Drummond, B.McEachern, D.S.Sorenson

Reaction ¹³C(n, p)¹³B at 65 MeV

NUCLEAR REACTIONS ¹³C(n, p), E=65 MeV; measured spectra, σ(θ); deduced v(c)(στ). ¹³B levels deduced spin-dipole transition role, possible analog resonance.

doi: 10.1103/PhysRevC.53.1718
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13633.

1995AB02      Phys.Rev.Lett. 74, 346 (1995)

K.Abe, T.Akagi, P.L.Anthony, R.Antonov, R.G.Arnold, T.Averett, H.R.Band, J.M.Bauer, H.Borel, P.E.Bosted, V.Breton, J.Button-Shafer, J.P.Chen, T.E.Chupp, J.Clendenin, C.Comptour, K.P.Coulter, G.Court, D.Crabb, M.Daoudi, D.Day, F.S.Dietrich, J.Dunne, H.Dutz, R.Erbacher, J.Fellbaum, A.Feltham, H.Fonvieille, E.Frlez, D.Garvey, R.Gearhart, J.Gomez, P.Grenier, K.A.Griffioen, S.Hoibraten, E.W.Hughes, C.Hyde-Wright, J.R.Johnson, D.Kawall, A.Klein, S.E.Kuhn, M.Kuriki, R.Lindgren, T.J.Liu, R.M.Lombard-Nelsen, J.Marroncle, T.Maruyama, X.K.Maruyama, J.McCarthy, W.Meyer, Z.-E.Meziani, R.Minehart, J.Mitchell, J.Morgenstern, G.G.Petratos, R.Pitthan, D.Pocanic, C.Prescott, R.Prepost, P.Raines, B.Raue, D.Reyna, A.Rijllart, Y.Roblin, L.S.Rochester, S.E.Rock, O.A.Rondon, I.Sick, L.C.Smith, T.B.Smith, M.Spengos, F.Staley, P.Steiner, S.St.Lorant, L.M.Stuart, F.Suekane, Z.M.Szalata, H.Tang, Y.Terrien, T.Usher, D.Walz, J.L.White, K.Witte, C.C.Young, B.Youngman, H.Yuta, G.Zapalac, B.Zihlmann, D.Zimmermann, and the E143 Collaboration

Precision Measurement of the Proton Spin Structure Function g₁(p)

NUCLEAR REACTIONS ¹H(polarized e, e'), E=9.7-29.1 GeV; measured asymmetry. ¹H deduced spin structure function g₁(p). Polarized ¹⁵NH₃ target.

doi: 10.1103/PhysRevLett.74.346
Citations: PlumX Metrics

1994KN01      Phys.Rev. C50, 909 (1994)

J.N.Knudson, J.D.Bowman, S.I.Penttila, J.R.Comfort, J.Tinsley, B.G.Ritchie, J.Gorgen, D.Mathis, S.S.Hanna, B.King, D.Pocanic, R.A.Loveman, L.S.Fritz, N.S.Dixon

Neutron Deformation in ¹⁶⁵Ho

NUCLEAR REACTIONS ¹⁶⁵Ho(π⁺, π⁰), E=165 MeV; measured σ(E, θ), oriented, unoriented nuclei; deduced asymmetry vs θ. ¹⁶⁵Ho deduced neutron distribution deformation features.

doi: 10.1103/PhysRevC.50.909
Citations: PlumX Metrics

1994PO01      Phys.Rev.Lett. 72, 1156 (1994)

D.Pocanic, E.Frlez, K.A.Assamagan, J.P.Chen, K.J.Keeter, R.M.Marshall, R.C.Minehart, L.C.Smith, G.E.Dodge, S.S.Hanna, B.H.King, J.N.Knudson

Reaction π⁺p → π⁺π⁰p Near Threshold and Chiral Symmetry Breaking

NUCLEAR REACTIONS ¹H(π⁺, π⁺π⁰), E=190-260 MeV; measured invariant mass spectra, π⁰π⁺-, π⁰p-coin; deduced total σ(E).

doi: 10.1103/PhysRevLett.72.1156
Citations: PlumX Metrics

1991KN01      Phys.Rev.Lett. 66, 1026 (1991)

J.N.Knudson, J.D.Bowman, S.I.Penttila, J.R.Comfort, B.G.Ritchie, J.Gorgen, D.Mathis, J.Tinsley, S.S.Hanna, B.King, D.Pocanic, R.A.Loveman, L.S.Fritz, N.S.Dixon

Neutron Deformation in ¹⁶⁵Ho

NUCLEAR REACTIONS ¹⁶⁵Ho(π⁺, π⁰), E=165 MeV; measured σ(E(π⁰)), orientation asymmetries. ¹⁶⁵Ho deduced neutral, charge quadrupole deformation ratio. Aligned, unaligned targets.

doi: 10.1103/PhysRevLett.66.1026
Citations: PlumX Metrics

1991MA02      Phys.Rev. C43, 1106 (1991)

C.J.Martoff, W.J.Cummings, D.Pocanic, S.S.Hanna, H.Ullrich, M.Furic, T.Petkovic, T.Kozlowski, J.P.Perroud

Nucleon Pairing in μ^- Capture by ⁴⁰Ca

NUCLEAR REACTIONS Ca(μ^-, p), (μ^-, n), E at rest; measured nucleon spectra; deduced correlated pair capture role.

doi: 10.1103/PhysRevC.43.1106
Citations: PlumX Metrics

1988WA24      Phys.Rev. C38, 2478 (1988)

K.Wang, C.J.Martoff, D.Pocanic, W.J.Cummings, S.S.Hanna, R.C.Byrd, C.C.Foster

Reaction ⁶Li(n, p)⁶He at 118 MeV

NUCLEAR REACTIONS ⁶Li(n, p), E=118 MeV; measured σ(θ); deduced Gamow-Teller resonance, sum rule. DWBA analyses. Intrinsic germanium detectors, enriched target.

doi: 10.1103/PhysRevC.38.2478
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13152.

1987BI03      Nucl.Phys. A463, 731 (1987)

B.Bilwes, R.Bilwes, J.Diaz, J.L.Ferrero, D.Pocanic, L.Stuttge

Intermediate Structure in the ²⁸Si + ³²S System

NUCLEAR REACTIONS, ICPND ²⁸Si(³²S, ³²S), (³²S, ³⁶Ar), E=42-48.1 MeV; measured σ(θ), σ(E); deduced deviation, correlation functions. Optical-model calculations. Enriched targets.

doi: 10.1016/0375-9474(87)90640-3
Citations: PlumX Metrics

1987KN02      Phys.Rev. C35, 1382 (1987)

J.N.Knudson, J.R.Comfort, R.A.Gianelli, B.G.Ritchie, D.Rothenberger, D.Pocanic, S.S.Hanna, J.D.Bowman, H.W.Baer, A.G.Bergmann, P.A.Heusi, F.Irom, C.J.Seftor, S.Hoibraten, R.A.Loveman, S.H.Rokni, H.Crannell, D.I.Sober, W.J.Fickinger, H.Marshak

Excitation of the Isobaric Analog State of ¹⁶⁵Ho Pion Single-Charge Exchange

NUCLEAR REACTIONS ¹⁶⁵Ho(π⁺, π⁰), E=98, 163.2, 228.3 MeV; measured π⁰ yield, θ=4°-6°. ¹²⁰Sn(π⁺, π⁰), E=98-165 MeV; analyzed data; deduced reaction systematics vs mass. ¹⁶⁵Er deduced IAS excitation σ.

doi: 10.1103/PhysRevC.35.1382
Citations: PlumX Metrics

1987PO18      Can.J.Phys. 65, 687 (1987)

D.Pocanic, K.Wang, C.J.Martoff, S.S.Hanna, R.C.Byrd, C.C.Foster, D.L.Friesel, J.Rapaport

First (n, p) Measurements with the Indiana University Cyclotron Facility

NUCLEAR REACTIONS ⁶Li(n, p), E=118 MeV; measured σ(Ep), σ(θp).

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13152.

1986CI06      Nucl.Phys. A459, 438 (1986)

N.Cindro, D.Pocanic, D.M.Drake, J.D.Moses, J.C.Peng, N.Stein, J.W.Sunier

Elastic Scattering of ²⁸Si on ²⁴Mg and ²⁶Mg

NUCLEAR REACTIONS ^26,24Mg(²⁸Si, ²⁸Si), E=74.5-83 MeV; ²⁴Mg(²⁸Si, ²⁴Mg), (²⁸Si, ²⁶Mg), E=83 MeV; measured σ(θ), σ(E); deduced intermediate structure.

doi: 10.1016/0375-9474(86)90144-2
Citations: PlumX Metrics

1986MA16      Czech.J.Phys. B36, 378 (1986)

C.J.Martoff, D.Pocanic, L.W.Whitlow, S.S.Hanna, H.Ullrich, S.Cierjacks, M.Furic, T.Petkovic, H.J.Weyer

Search for Emission of Nucleons and Nucleon Pairs following Muon Capture in Selected Light Nuclei

NUCLEAR REACTIONS ¹²C, ¹⁶O, ²⁷Al(μ^-, p), E at rest; measured proton spectra.

doi: 10.1007/BF01597841
Citations: PlumX Metrics

1985PO01      Nucl.Phys. A433, 531 (1985)

D.Pocanic, N.Cindro

Extension of the Orbiting-Cluster Concept to fp Shell Systems

NUCLEAR STRUCTURE A=22-72; analyzed heavy ion reaction data; deduced composite system parameters. Orbiting cluster model.

NUCLEAR REACTIONS ²⁸Si, ¹²C(¹²C, X), ²⁴Mg(¹⁶O, X), (²⁸Si, X), E not given; calculated composite system densities along bands.

doi: 10.1016/0375-9474(85)90280-5
Citations: PlumX Metrics

1985PO16      Nucl.Phys. A444, 303 (1985)

D.Pocanic, R.Caplar, G.Vourvopoulos, X.Aslanoglou

Search for Intermediate Structure in ³⁶Ar via the ²⁴Mg(¹²C, α)³²S Reaction

NUCLEAR REACTIONS ²⁴Mg(¹²C, α), E=11.9-19.4 MeV; measured σ(E, θ). ³²S deduced angular momenta, deviation, correlation functions. Hauser-Feshbach calculations. Enriched targets.

doi: 10.1016/0375-9474(85)90352-5
Citations: PlumX Metrics

1984PO15      Phys.Rev. C30, 1520 (1984)

D.Pocanic, K.Van Bibber, J.S.Dunham, W.A.Seale, F.Sperisen, S.S.Hanna

Intermediate Structure in the ¹⁶O + ¹⁶O System

NUCLEAR REACTIONS ¹⁶O(¹⁶O, α), E=20-44 MeV; measured σ(θ) vs E; deduced optical model parameters. ³²S deduced intermediate structure, resonance J, π. Statistical, Hauser-Feshbach analyses.

doi: 10.1103/PhysRevC.30.1520
Citations: PlumX Metrics

1983CA23      Z.Phys. A313, 227 (1983)

R.Caplar, I.Udovicic, E.Holub, D.Pocanic, N.Cindro

Isotopic Effects in the (n, p) Reaction Cross Section on Heavy Targets and the Statistical Preequilibrium Model

NUCLEAR REACTIONS ^{122,124,126,128,130}Te(n, p), E=14.6 MeV; ^{128,130,131,132,134}Xe(n, p), E=14.4 MeV; ^{180,182,183,184,186}W, ^{188,189,190,192}Os(n, p), E=14.7 MeV; calculated σ; deduced proton, neutron separation energy role. Statistical preequilibrium model.

1981CA16      Fizika(Zagreb) 13, Suppl.No.1, 37 (1981)

R.Caplar, G.Vourvopoulos, X.Aslanoglou, D.Pocanic

Search for Intermediate Structure in ³⁶Ar above the Coulomb Barrier via the ²⁴Mg(¹²C, α)³²S Reaction

NUCLEAR REACTIONS ²⁴Mg(¹²C, α), E(cm)=11.9-16.1 MeV; measured σ(E); deduced spin selectivity. ³⁶Ar deduced no definitive intermediate resonances. Statistical analysis.

1981DR01      Phys.Lett. B98, 36 (1981)

D.M.Drake, M.Cates, N.Cindro, D.Pocanic, E.Holub

Gross Structure and Resonant Behaviour of ¹⁴C + ¹⁴C Elastic Scattering

NUCLEAR REACTIONS ¹⁴C(¹⁴C, ¹⁴C), E=23.4-58.4 MeV; measured σ(θ, E); deduced gross structure, resonant behavior. Optial model analysis.

doi: 10.1016/0370-2693(81)90362-2
Citations: PlumX Metrics

1981PO05      J.Phys.(London) G7, 389 (1981)

D.Pocanic, G.Vourvopoulos, X.Aslanoglou, E.Holub

Possible Evidence for the Existence of Intermediate Resonant Structure in the ⁹Be + ¹³C Heavy-Ion System

NUCLEAR REACTIONS ¹³C(⁹Be, α), E=8-22.75; measured σ(E, θ). ²²Ne deduced possible intermediate resonances. Statistical analysis.

doi: 10.1088/0305-4616/7/3/014
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2155.

1981PO16      Fizika(Zagreb) 13, Suppl.No.1, 35 (1981)

D.Pocanic, K.Van Bibber, W.A.Seale, J.Dunham, J.L.Thornton, S.S.Hanna

Intermediate Structure in the ¹⁶O + ¹⁶O System Observed via the α Exit Channel

NUCLEAR REACTIONS ¹⁶O(¹⁶O, α), E ≈ 20-45 MeV; measured σ(θ, E). ³²S deduced intermediate structure. Correlation, deviation function analysis.

1980CI02      J.Phys.(London) G6, 359 (1980)

N.Cindro, D.Pocanic

Resonances in Heavy-Ion Reactions as Orbiting-Cluster Phenomena

NUCLEAR REACTIONS ¹²C(¹²C, X), E(cm) ≈ 4-20 MeV; ¹²C(¹⁶O, X), E(cm) ≈ 12-21 MeV; ¹²C(¹⁸O, X), E(cm) ≈ 10-25 MeV; ²⁴Mg(¹²C, X), E=27.5-35.5 MeV; ¹²C(²⁸Si, X), E(cm) ≈ 18-35 MeV; ¹⁶O(²⁸Si, X), E(cm)=17-37 MeV; calculated molecular resonances. ²⁴Mg, ^28,30Si, ³⁶Ar, ⁴⁰Ca, ⁴⁴Ti deduced moments of inertia, level densities. Molecular resonance window model.

doi: 10.1088/0305-4616/6/3/011
Citations: PlumX Metrics

1980CI05      J.Phys.(London) G6, 885 (1980)

N.Cindro, D.Pocanic

On the Nature of Heavy-Ion Resonances in the ⁴⁰Ca Composite System

NUCLEAR REACTIONS ²⁸Si(¹²C, ¹²C), (¹²C, ¹⁶O), ²⁴Mg(¹⁶O, ¹⁶O), (¹⁶O, ¹²C), E not given; analyzed σ. ⁴⁰Ca resonances deduced character. Orbiting cluster model, molecular resonance window concept.

doi: 10.1088/0305-4616/6/7/011
Citations: PlumX Metrics

1980HO23      Z.Phys. A296, 341 (1980)

E.Holub, D.Pocanic, R.Caplar, N.Cindro

A Consistent Study of Precompound and Compound-Nucleus Emission Mechanisms in Neutron-Induced Reactions

NUCLEAR REACTIONS ⁴⁵Sc, ⁵⁵Mn, ⁵⁶Fe, ⁵⁹Co, ⁸⁹Y, ⁹³Nb, ¹⁰³Rh, ¹⁶⁹Tm, ¹⁷⁵Lu, ¹⁸¹Ta, ¹⁹⁷Au, ²⁰⁹Bi(n, n'), (n, p), (n, 2n), (n, 3n), E=4-24 MeV; calculated σ(E); deduced exciton model parameter K. Weisskopf-Ewing evaporation, precompound exciton models.

doi: 10.1007/BF01438529
Citations: PlumX Metrics

1979PO02      J.Phys.(London) G5, L25 (1979)

D.Pocanic, N.Cindro

A Semiempirical Prediction of Resonances in Heavy-Ion Reactions for s-d Shell Nuclei

NUCLEAR REACTIONS ¹²C(¹²C, X), ¹²C(¹⁶O, X), ¹²C(¹⁸O, X), E not given; predicted resonances in ²⁴Mg, ²⁸Si, ³⁰Si based on spreading width estimates via level density calculation.

doi: 10.1088/0305-4616/5/2/002
Citations: PlumX Metrics

1978PO07      Fizika, Suppl. 10, 3 (1978)

D.Pocanic, N.Cindro

A Semiempirical Prediction of the Occurrence of Resonances in Heavy Ion Reactions

NUCLEAR REACTIONS ¹²C(¹²C, X), (¹⁶O, X), ¹²C(¹⁴N, X), ¹⁶O(¹⁶O, X), E not given; calculated constant density lines in energy vs J(J+1) plane. ²⁴Mg, ²⁶Al, ²⁸Si, ³²S deduced conditions for resonance excitation in HI reactions.