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NSR database version of April 11, 2024.

Search: Author = H.Schelin

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2013DE15      Eur.Phys.J. A 49, 51 (2013)

V.V.Denyak, V.M.Khvastunov, S.A.Paschuk, H.R.Schelin

Mass dependence of azimuthal asymmetry in the fission of ²³²Th and ^{233, 235, 236, 238}U by polarized photons

NUCLEAR REACTIONS ²³²Th(polarized γ, F), E=9.3 MeV;^{233,235,236,238}U(polarized γ, F), E=7.9 MeV; measured bremsstrahlung induced fission products; deduced mass distributions, asymmetry.

doi: 10.1140/epja/i2013-13051-6
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG4069.

2013IZ01      Phys.Rev. C 88, 065808 (2013)

R.Izsak, A.Horvath, A.Kiss, Z.Seres, A.Galonsky, C.A.Bertulani, Zs.Fulop, T.Baumann, D.Bazin, K.Ieki, C.Bordeanu, N.Carlin, M.Csanad, F.Deak, P.DeYoung, N.Frank, T.Fukuchi, A.Gade, D.Galaviz, C.R.Hoffman, W.A.Peters, H.Schelin, M.Thoennessen, G.I.Veres

Determining the ⁷Li(n, γ) cross section via Coulomb dissociation of ⁸Li

NUCLEAR REACTIONS C, Pb(⁸Li, n), [⁸Li secondary beam from ⁹Be(¹⁸O, X), E=120 MeV/nucleon primary reaction], E=69.5 MeV/nucleon; ⁸Li(γ, n)⁷Li, [γ from ⁸Li beam impinging on C and Pb targets], E(⁸Li)=69.5 MeV/nucleon; measured TOF, position and angle of ⁸Li particles, neutron spectra from Coulomb dissociation of ⁸Li, E(n), I(n) using MONA neutron detector array at NSCL-MSU cyclotron facility; reconstructed neutron ⁷Li energy spectra and momentum vectors; deduced σ(E) for ⁷Li(n, γ)⁸Li reaction. Surrogate method. Comparison of σ with previous experimental results, and with low-energy effective field theory calculations.

doi: 10.1103/PhysRevC.88.065808
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14378.

2010DE09      Phys.Atomic Nuclei 73, 395 (2010); Yad.Fiz. 73, 419 (2010)

V.V.Denyak, V.M.Khvastunov, S.A.Paschuk, H.R.Schelin, A.A.Khomich, N.G.Shevchenko

Excitation of Discrete Levels of ⁶³Cu and ⁶⁵Cu Nuclei in (e, e') Reactions

NUCLEAR REACTIONS ^63,65Cu(e, e'), E=120, 150, 225 MeV; measured Ee, Ie; ^63,65Cu deduced level energies, multipolarities, B(E1), B(E2), B(E3).

doi: 10.1134/S1063778810030014
Citations: PlumX Metrics
Data from this article have been entered in the XUNDL database. For more information, click here.

2006HO14      Eur.Phys.J. A 27, Supplement 1, 217 (2006)

A.Horvath, K.Ieki, A.Kiss, A.Galonsky, M.Thoennessen, T.Baumann, D.Bazin, C.A.Bertulani, C.Bordeanu, N.Carlin, M.Csanad, F.Deak, P.DeYoung, N.Frank, T.Fukuchi, Zs.Fulop, A.Gade, D.Galaviz, C.Hoffman, R.Izsak, W.A.Peters, H.Schelin, A.Schiller, R.Sugo, Z.Seres, G.I.Veres

Can the neutron-capture cross sections be measured with Coulomb dissociation?

NUCLEAR REACTIONS C, Pb(⁸Li, n⁷Li), E=41 MeV/nucleon; measured particle spectra, angular distributions; deduced nuclear and Coulomb contributions.

doi: 10.1140/epja/i2006-08-033-6
Citations: PlumX Metrics

2004DE25      Yad.Fiz. 67, 906 (2004); Phys.Atomic Nuclei 67, 882 (2004)

V.V.Denyak, V.M.Khvastunov, V.P.Likhachev, A.A.Nemashkalo, S.P.Paschuk, H.R.Schelin

Excitation of Discrete Levels in ⁵⁴Fe and ⁵⁶Fe Nuclei by Means of (e, e') Reactions

NUCLEAR REACTIONS ^54,56Fe(e, e'), E=226 MeV; measured σ(E, θ). ^54,56Fe deduced level energies, multipolarities.

doi: 10.1134/1.1755380
Citations: PlumX Metrics

2004LI78      Braz.J.Phys. 34, 753 (2004)

V.P.Likhachev, J.D.T.Arruda-Neto, M.T.F.da Cruz, H.Dias, S.B.Duarte, W.R.Carvalho, Jr., M.S.Hussein, A.C.S.Lima, L.F.R.Macedo, J.Mesa, S.A.Pashchuk, T.E.Rodrigues, G.Silva, H.R.Schelin, O.A.P.Tavares

Residual Nucleus Excitation Energy in (e, e'p)- Reaction

doi: 10.1590/S0103-97332004000500012
Citations: PlumX Metrics

2003HO22      Nucl.Phys. A719, 9c (2003)

A.Horvath, A.Galonsky, N.Carlin, F.Deak, T.Gomi, V.Guimaraes, Y.Higurashi, K.Hiroshi, K.Ieki, Y.Iwata, A.Kiss, J.Kolata, T.Rauscher, H.Schelin, J.von Schwarzenberg, Z.Seres, S.Takeuchi, S.Typel, R.Warner, J.Weiner

Measurements of astrophysical neutron capture cross sections via the inverse reaction

NUCLEAR REACTIONS C, Al, Cu, Sn, Pb(¹⁵C, nX), E=35 MeV/nucleon; C, Al, Cu, Sn, Pb(⁹Li, nX), E=40 MeV/nucleon; measured neutron spectra, (fragment)(neutron)-coin, dissociation yields. ⁸Li, ¹⁴C(n, γ), E=low; deduced astrophysical reaction rates.

doi: 10.1016/S0375-9474(03)00951-5
Citations: PlumX Metrics

2003KO07      Phys.Rev. C 67, 015806 (2003)

H.Kobayashi, K.Ieki, A.Horvath, A.Galonsky, N.Carlin, F.Deak, T.Gomi, V.Guimaraes, Y.Higurashi, Y.Iwata, A.Kiss, J.J.Kolata, T.Rauscher, H.Schelin, Z.Seres, R.Warner

Astrophysical reaction rate for the ⁸Li(n, γ)⁹Li reaction

NUCLEAR REACTIONS Pb(⁹Li, n⁸Li), E=39.7 MeV/nucleon; measured neutron and lithium spectra. ⁸Li(n, γ), E not given; deduced σ, astrophysical reaction rate upper limits. Comparison with previous results.

doi: 10.1103/PhysRevC.67.015806
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2003LI25      Phys.Rev. C 68, 014615 (2003)

V.P.Likhachev, J.D.T.Arruda-Neto, W.R.Carvalho, Jr., A.Deppman, I.G.Evseev, F.Garcia, M.S.Hussein, L.F.R.Macedo, A.Margaryan, J.Mesa, V.O.Nesterenko, O.Rodriguez, S.A.Pashchuk, H.R.Schelin, M.S.Vaudeluci

Inclusive quasifree electrofission cross section for ²³⁸U

NUCLEAR STRUCTURE ^237,238U, ²³⁷Pa; calculated fissility vs excitation energy.

NUCLEAR REACTIONS ²³⁸U(e, e'p), (e, e'), E=300 MeV; calculated σ(E, θ). ²³⁸U(e, F), E=100-250 MeV; measured fission σ; deduced reaction mechanism features.

doi: 10.1103/PhysRevC.68.014615
Citations: PlumX Metrics

2002WA04      Phys.Rev. C65, 034306 (2002)

J.Wang, A.Galonsky, J.J.Kruse, E.Tryggestad, R.H.White-Stevens, P.D.Zecher, Y.Iwata, K.Ieki, A.Horvath, F.Deak, A.Kiss, Z.Seres, J.J.Kolata, J.von Schwarzenberg, R.E.Warner, H.Schelin

Dissociation of ⁶He

NUCLEAR REACTIONS C, Al, Cu, Sn, Pb, U(⁶He, 2nα), (⁶He, αX), E=23.9 MeV/nucleon; measured Eα, En, nα-coin, parallel momentum distributions, angular correlations, two-neutron removal σ; deduced Coulomb contribution, other reaction mechanism features. ⁶He deduced halo neutron correlations. Comparisons with model predictions.

doi: 10.1103/PhysRevC.65.034306
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0867.

2000IW05      Phys.Rev. C62, 064311 (2000)

Y.Iwata, K.Ieki, A.Galonsky, J.J.Kruse, J.Wang, R.H.White-Stevens, E.Tryggestad, P.D.Zecher, F.Deak, A.Horvath, A.Kiss, Z.Seres, J.J.Kolata, J.von Schwarzenberg, R.E.Warner, H.Schelin

Dissociation of ⁸He

NUCLEAR REACTIONS Al(⁸He, n⁶He), Sn, Pb(⁸He, 2n⁶He), E=24 MeV/nucleon; measured invariant mass spectra, relative momentum distributions; deduced sequential decay contribution, dipole strength function, sum rules. ⁸He deduced excited state J, π, Γ. Secondary beam from ¹⁶O fragmentation.

doi: 10.1103/PhysRevC.62.064311
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1999HE45      Nucl.Sci.Eng. 132, 1 (1999)

L.Heilbronn, R.S.Cary, M.Cronqvist, F.Deak, K.Frankel, A.Galonsky, K.Holabird, A.Horvath, A.Kiss, J.Kruse, R.M.Ronningen, H.Schelin, Z.Seres, C.E.Stronach, J.Wang, P.Zecher, C.Zeitlin

Neutron yields from 155 MeV/Nucleon Carbon and Helium Stopping in Aluminum

NUCLEAR REACTIONS ²⁷Al(α, X), (¹²C, X), E=155 MeV/nucleon; measured reaction products, En, In; deduced yields, number of neutrons per interaction.

doi: 10.13182/nse98-41
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1051.

1998ZE01      Phys.Rev. C57, 959 (1998)

P.D.Zecher, A.Galonsky, S.J.Gaff, J.J.Kruse, G.Kunde, E.Tryggestad, J.Wang, R.E.Warner, D.J.Morrissey, K.Ieki, Y.Iwata, F.Deak, A.Horvath, A.Kiss, Z.Seres, J.J.Kolata, J.von Schwarzenberg, H.Schelin

Measurement of the ⁸Li(n, γ)⁹Li Cross Section at Astrophysical Energies by Reverse Kinematics

NUCLEAR REACTIONS U, Pb(⁹Li, n⁸Li), E=30 MeV/nucleon; measured σ. ⁸Li(n, γ), E=0.25, 0.75 MeV; deduced σ upper limit. Astrophysical implications discussed. Radioactive beam.

doi: 10.1103/PhysRevC.57.959
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13692.

1997DE58      Acta Phys.Hung.N.S. 5, 13 (1997)

F.Deak, A.Horvath, A.Kiss, Z.Seres, A.Galonsky, H.Hama, L.Heilbronn, D.W.Sackett, H.R.Schelin

Production Rates of Excited Fragment Isotopes from the ³⁶Ar + Ag Reaction at 35 MeV/nucleon

NUCLEAR REACTIONS Ag(³⁶Ar, X), E=35 MeV/nucleon; measured Z=3-5 excited fragments σ(θ) vs kinetic energy; deduced total production of neutron unbound states. Thermal model.

1997LI15      Phys.Rev. C56, 250 (1997)

I.Licot, N.Added, N.Carlin, G.M.Crawley, S.Danczyk, J.Finck, D.Hirata, H.Laurent, D.J.Morrissey, M.M.de Moura, H.R.Schelin, J.Stasko, M.Steiner, A.A.P.Suaide, A.Szanto de Toledo, E.M.Szanto, M.Thoennessen, J.A.Winger

Reaction Cross Sections and Radii for f-p Shell Exotic Neutron-Rich Nuclei

NUCLEAR REACTIONS, ICPND Si(⁴¹Ar, X), (⁴²Ar, X), (⁴³Ar, X), (⁴⁴Ar, X), (⁴⁵Ar, X), (⁴⁶Ar, X), (⁴⁴K, X), (⁴⁵K, X), (⁴⁶K, X), (⁴⁷K, X), (⁴⁸K, X), (⁴⁹K, X), (⁴⁶Ca, X), (⁴⁷Ca, X), (⁴⁸Ca, X), (⁴⁹Ca, X), (⁵⁰Ca, X), (⁵¹Ca, X), (⁴⁹Sc, X), (⁵⁰Sc, X), (⁵¹Sc, X), (⁵²Sc, X), (⁵³Sc, X), E=52-69 MeV/nucleon; measured reaction σ. ^{41,42,43,44,45,46}Ar, ^{44,45,46,47,48,49}K, ^{46,47,48,49,50,51}Ca, ^{49,50,51,52,53}Sc deduced strong absorption radii, neutron separation energies. Comparison to Glauber model, RMF theory.

doi: 10.1103/PhysRevC.56.250
Citations: PlumX Metrics

1996GA08      Nucl.Phys. A599, 353c (1996)

A.Galonsky, J.J.Kruse, W.G.Lynch, D.J.Morrissey, N.Orr, J.Ottarson, D.Sackett, B.M.Sherrill, J.Wang, J.Winger, P.Zecher, K.Ieki, Y.Iwata, F.Deak, A.Horvath, A.Kiss, Z.Seres, J.J.Kolata, R.E.Warner, H.Schelin, D.L.Humphrey

Soft Dipole Resonance in Exotic Nuclei ( Question )

NUCLEAR REACTIONS Pb(¹¹Li, X), E=30 MeV/nucleon; measured projectile three-body breakup energy spectrum, three-particle momenta; deduced no soft dipole resonance. ¹¹Li deduced no dineutron. Virtual photon induced photodisintegration of ¹¹Li.

doi: 10.1016/0375-9474(96)00078-4
Citations: PlumX Metrics

1995DE24      Phys.Rev. C52, 219 (1995)

F.Deak, A.Horvath, A.Kiss, Z.Seres, A.Galonsky, C.K.Gelbke, H.Hama, L.Heilbronn, D.Krofcheck, W.G.Lynch, D.W.Sackett, H.R.Schelin, M.B.Tsang, J.Kasagi, T.Murakami

Internal Excitation of Intermediate Mass Fragments from Collisions of ³⁶Ar + Ag Nuclei at 35 MeV/nucleon

NUCLEAR REACTIONS Ag(³⁶Ar, X), E=35 MeV/nucleon; measured intermediate mass fragments (Li-Mg) population ratios.

doi: 10.1103/PhysRevC.52.219
Citations: PlumX Metrics

1994HO02      Phys.Rev. C49, 1012 (1994)

A.Horvath, F.Deak, A.Kiss, Z.Seres, A.Galonsky, C.K.Gelbke, H.Hama, L.Heilbronn, D.Krofcheck, W.G.Lynch, D.W.Sackett, H.R.Schelin, M.B.Tsang, J.Kasagi, T.Murakami

Fragment Isotope Spectra from the ³⁶Ar + Ag Reaction at 35 MeV/nucleon

NUCLEAR REACTIONS Ag(³⁶Ar, X), E=35 MeV/nucleon; measured inclusive fragment σ(E, θ); deduced total fragment production σ charge, mass dependence.

doi: 10.1103/PhysRevC.49.1012
Citations: PlumX Metrics

1993AN15      Phys.Rev. C48, R2154 (1993)

R.M.Anjos, N.Added, N.Carlin, L.Fante, Jr., M.C.S.Figueira, R.Matheus, H.R.Schelin, E.M.Szanto, C.Tenreiro, A.Szanto de Toledo, S.J.Sanders

Fission Decay of Very Light Nuclear Systems

NUCLEAR REACTIONS ^10,11B(¹⁶O, X), (¹⁷O, X), (¹⁸O, X), ⁹Be(¹⁹F, X), E < 5 MeV/nucleon; measured σ(fragment θ); deduced fusion followed by fission evidence.

doi: 10.1103/PhysRevC.48.R2154
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0407.

1993SC04      Nucl.Sci.Eng. 113, 184 (1993)

H.R.Schelin, A.Galonsky, C.K.Gelbke, H.Hama, L.Heilbronn, D.Krofcheck, W.G.Lynch, D.Sackett, M.B.Tsang, X.Yang, F.Deak, A.Horvath, A.Kiss, Z.Seres, J.Kasagi, T.Murakami

Neutron Production in Heavy-Ion Reactions at 35 and 50 MeV/Nucleon

NUCLEAR REACTIONS Ag(¹⁴N, xn), E=50 MeV/nucleon; measured neutron spectra. Moving source model analysis.

doi: 10.13182/NSE93-A24007
Citations: PlumX Metrics

1992ME06      Nucl.Sci.Eng. 111, 132 (1992)

A.C.Merchant, P.E.Hodgson, H.R.Schelin

The Interaction of 1- to 20-MeV Neutrons with ²³⁸U

NUCLEAR REACTIONS ²³⁸U(n, n), (n, n'), E=1-20 MeV; ²³⁸U(n, 2n), (n, 3n), E=threshold-20 MeV; analyzed σ(E), other data. Optical potential, dispersion relation approach.

doi: 10.13182/NSE92-A23929
Citations: PlumX Metrics

1991HE07      Phys.Rev. C43, 2318 (1991)

L.Heilbronn, A.Galonsky, C.K.Gelbke, W.G.Lynch, T.Murakami, D.Sackett, H.Schelin, M.B.Tsang, F.Deak, A.Kiss, Z.Seres, J.Kasagi, B.A.Remington

Production of Neutron-Unbound States in Intermediate-Mass Fragments from ¹⁴N + Ag Reactions at E/A = 35 MeV

NUCLEAR REACTIONS Ag(¹⁴N, nX), E=35 MeV/nucleon; measured γ(fragment)-coin, X=Li, Be, B, C isotopes; deduced source temperatures, amount of sequential feeding.

doi: 10.1103/PhysRevC.43.2318
Citations: PlumX Metrics

1991SA10      Phys.Rev. C44, 384 (1991)

D.Sackett, A.Galonsky, C.K.Gelbke, H.Hama, L.Heilbronn, D.Krofcheck, W.Lynch, H.R.Schelin, M.B.Tsang, X.Yang, F.Deak, A.Horvath, A.Kiss, Z.Seres, J.Kasagi, T.Murakami

Neutron Inclusive Measurements of ³⁶Ar + Ag Reactions at 35 MeV/Nucleon

NUCLEAR REACTIONS Ag(³⁶Ar, nX), E=35 MeV/nucleon; measured inclusive σ(θ, E); deduced neutron multiplicities, nuclear temperatures. Moving source fits.

doi: 10.1103/PhysRevC.44.384
Citations: PlumX Metrics

1990DE25      Phys.Rev. C42, 1029 (1990)

F.Deak, A.Kiss, Z.Seres, A.Galonsky, L.Heilbronn, H.R.Schelin

Light Fragments from ¹⁴N + Ag Collisions at 35 MeV/Nucleon

NUCLEAR REACTIONS Ag(¹⁴N, X), E=35 MeV/nucleon; measured σ(fragment θ, En, θn); deduced model parameters. Moving source model.

doi: 10.1103/PhysRevC.42.1029
Citations: PlumX Metrics

1989DE05      Phys.Rev. C39, 733 (1989)

F.Deak, A.Kiss, Z.Seres, A.Galonsky, C.K.Gelbke, L.Heilbronn, W.Lynch, T.Murakami, H.Schelin, M.B.Tsang, B.A.Remington, J.Kasagi

Dependence of ¹²B Excitation Energy on Its Kinetic Energy in the ¹⁴N + Ag Reaction at E/A = 35 MeV

NUCLEAR REACTIONS Ag(¹⁴N, ¹²BX), E=490 MeV; measured σ(θ) vs ejectile energy, n(¹¹B)-coin following ejectile breakup.

doi: 10.1103/PhysRevC.39.733
Citations: PlumX Metrics

1989SC08      Phys.Rev. C39, 1827 (1989)

H.R.Schelin, A.Galonsky, C.K.Gelbke, L.Heilbronn, W.G.Lynch, T.Murakami, M.B.Tsang, X.Yang, G.Zhang, B.A.Remington, F.Deak, A.Kiss, Z.Seres, J.Kasagi

Neutron Inclusive Measurements in ¹⁴N + Ag Reactions at 35 MeV/Nucleon

NUCLEAR REACTIONS Ag(¹⁴N, nX), E=35 MeV/nucleon; measured σ(θn, En); deduced angle integrated σ.

doi: 10.1103/PhysRevC.39.1827
Citations: PlumX Metrics

1987GA17      Phys.Lett. 197B, 511 (1987)

A.Galonsky, G.Caskey, L.Heilbronn, B.Remington, H.Schelin, F.Deak, A.Kiss, Z.Seres, J.Kasagi

Temperatures Determined from Neutron Emission in Nucleus-Nucleus Collisions

NUCLEAR REACTIONS ¹⁶⁵Ho(¹⁴N, xn), E=35 MeV/nucleon; measured σ(θn, En); deduced temperatures.

doi: 10.1016/0370-2693(87)91045-8
Citations: PlumX Metrics

1986HU06      Nucl.Phys. A458, 397 (1986)

M.S.Hussein, E.Farrelly-Pessoa, H.R.Schelin, R.A.Douglas

Isospin Mixing in Compound Nuclear Reactions: A study in the ¹¹B(p, n)¹¹C system at E(p) = 14.3 MeV

NUCLEAR REACTIONS ¹¹B(p, n), E=14.3 MeV; calculated σ(θ). ¹²C levels deduced isopsin purity. DWBA, Hauser-Feshbach calculations.

doi: 10.1016/0375-9474(86)90042-4
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0826.

1985SC08      Nucl.Sci.Eng. 89, 87 (1985)

H.R.Schelin, E.Farrelly Pessoa, W.R.Wylie, J.L.Cardoso, Jr., R.A.Douglas

The ^10,11B(p, n)^10,11C Reactions Between E(p) = 13.7 and 14.7 MeV

NUCLEAR REACTIONS ^10,11B(p, n), E=13.7-14.7 MeV; measured absolute σ(θ) vs E.

doi: 10.13182/NSE85-A17886
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0331.

1984SC04      Nucl.Phys. A414, 67 (1984)

H.R.Schelin, E.Farrelly Pessoa, W.R.Wylie, E.W.Cybulska, K.Nakayama, L.M.Fagundes, R.A.Douglas

The ¹²C(d, n)¹³N Reaction between E(d) = 7.0 and 13.0 MeV

NUCLEAR REACTIONS ¹²C(d, n), E=7, 9.1, 13 MeV; measured σ(En), σ(E), absolute σ(θ). ¹²C(d, n), E=10.6-13 MeV; measured σ(E). ¹³N levels deduced S. Hauser-Feshbach reduction factors. Tof. DWBA analysis.

doi: 10.1016/0375-9474(84)90497-4
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0806.

Note: The following list of authors and aliases matches the search parameter H.Schelin: , H.R.SCHELIN