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NSR database version of April 25, 2024.

Search: Author = H.C.Britt

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2003YO03      Phys.Rev. C 67, 024610 (2003)

W.Younes, H.C.Britt

Neutron-induced fission cross sections simulated from (t, pf) results

NUCLEAR REACTIONS ²³⁴U(t, pF), E=15, 18 MeV; analyzed fission probabilities; deduced parameters. ^235,235mU(n, F), E=0.1-2.5 MeV; calculated fission σ.

doi: 10.1103/PhysRevC.67.024610
Citations: PlumX Metrics

2003YO06      Phys.Rev. C 68, 034610 (2003)

W.Younes, H.C.Britt

Simulated neutron-induced fission cross sections for various Pu, U, and Th isotopes

NUCLEAR REACTIONS ^239,240,242Pu, ^{233,234,235,236,238}U, ^230,232Th(t, pF), E^* ≈ 4-9 MeV; analyzed fission probabilities. ^240,241,243Pu, ^{234,235,236,237,238}U, ^231,233Th(n, F), E ≈ 0.1-2.5 MeV; deduced fission σ. Comparison with previous results.

doi: 10.1103/PhysRevC.68.034610
Citations: PlumX Metrics

1997AH03      Phys.Rev. C55, 2604 (1997)

L.Ahle, Y.Akiba, D.Beavis, P.Beery, H.C.Britt, B.Budick, C.Chasman, Z.Chen, C.Y.Chi, Y.Y.Chu, V.Cianciolo, B.A.Cole, J.B.Costales, H.J.Crawford, J.B.Cumming, R.Debbe, J.Engelage, S.Y.Fung, M.Gonin, S.Gushue, H.Hamagaki, R.S.Hayano, S.Hayashi, S.Homma, H.Kaneko, J.Kang, S.Kaufman, W.L.Kehoe, K.Kurita, R.J.Ledoux, M.J.LeVine, Y.Miake, D.P.Morrison, R.J.Morse, B.Moskowitz, S.Nagamiya, M.N.Namboodiri, T.Nayak, J.Olness, C.G.Parsons, L.P.Remsberg, D.Roehrich, P.Rothschild, H.Sakurai, T.C.Sangster, R.Seto, K.Shigaki, R.Soltz, P.Stankus, S.G.Steadman, G.S.F.Stephans, T.Sung, Y.Tanaka, M.J.Tannenbaum, J.Thomas, S.Tonse, S.Ueno, J.H.van Dijk, F.Videbaek, O.Vossnack, V.Vutsadakis, F.Q.Wang, Y.Wang, H.E.Wegner, H.E.Wegner, D.S.Woodruff, Y.D.Wu, K.Yagi, X.Yang, D.Zachary, W.A.Zajc, and the E802 Collaboration

Baryon Emission at Target Rapidities in Si + Al, Cu, Au Collisions at 14.6A GeV/c and Au + Au Collisions at 11.7A GeV/c

NUCLEAR REACTIONS ²⁷Al, Cu, ¹⁹⁷Au(²⁸Si, X), E at 14.6 GeV/c/nucleon; ¹⁹⁷Au(¹⁹⁷Au, X), E at 11.7 GeV/c/nucleon; measured light charged particle momentum density distribution; deduced proton distributions at minimum bias target rapidities, pseudorapidity distributions shapes. Model comparison.

doi: 10.1103/PhysRevC.55.2604
Citations: PlumX Metrics

1997AK04      Phys.Rev. C56, 1544 (1997)

Y.Akiba, D.Beavis, P.Beery, H.C.Britt, B.Budick, C.Chasman, Z.Chen, C.Y.Chi, Y.Y.Chu, V.Cianciolo, B.A.Cole, J.B.Costales, H.J.Crawford, J.B.Cumming, R.Debbe, J.Engelage, S.Y.Fung, M.Gonin, S.Gushue, H.Hamagaki, O.Hansen, R.S.Hayano, S.Hayashi, S.Homma, H.Kaneko, J.Kang, S.Kaufman, W.L.Kehoe, K.Kurita, R.J.Ledoux, M.J.Levine, Y.Miake, D.P.Morrison, R.J.Morse, B.Moskowitz, S.Nagamiya, M.N.Namboodiri, T.K.Nayak, J.Olness, C.G.Parsons, L.P.Remsberg, D.Roehrich, P.Rothschild, H.Sakurai, T.C.Sangster, R.Seto, R.Soltz, P.Stankus, S.G.Steadman, G.S.F.Stephans, T.Sung, Y.Tanaka, M.J.Tannenbaum, J.Thomas, S.Tonse, J.H.Van Dijk, F.Videbaek, O.Vossnack, V.Vutsadakis, F.Q.Wang, Y.Wang, H.E.Wegner, D.S.Woodruff, Y.D.Wu, X.Yang, D.Zachary, W.A.Zajc

Two-Particle Rapidity Correlations from the Bose-Einstein Effect in Central ²⁸Si + Au Collisions at 14.6A GeV/c and Intermittency

NUCLEAR REACTIONS ¹⁹⁷Au(²⁸Si, X), E at 14.6 GeV/c/nucleon; measured two-pion correlation functions vs Q(inv), rapidity, pseudorapidity; deduced correlation length, Bose-Einstein effect role.

doi: 10.1103/PhysRevC.56.1544
Citations: PlumX Metrics

1996AK04      Phys.Rev.Lett. 76, 2021 (1996)

Y.Akiba, D.Beavis, P.Beery, H.C.Britt, B.Budick, C.Chasman, Z.Chen, C.Y.Chi, Y.Y.Chu, V.Cianciolo, B.A.Cole, J.B.Costales, H.J.Crawford, J.B.Cumming, R.Debbe, J.Engelage, S.Y.Fung, M.Gonin, S.Gushue, H.Hamagaki, O.Hansen, R.S.Hayano, S.Hayashi, S.Homma, H.Kaneko, J.Kang, S.Kaufman, W.L.Kehoe, K.Kurita, R.J.Ledoux, M.J.Levine, Y.Miake, D.P.Morrison, R.J.Morse, B.Moskowitz, S.Nagamiya, M.N.Namboodiri, T.K.Nayak, J.Olness, C.G.Parsons, L.P.Remsberg, D.Roehrich, P.Rothschild, H.Sakurai, T.C.Sangster, R.Seto, R.Soltz, P.Stankus, S.G.Steadman, G.S.F.Stephans, T.Sung, Y.Tanaka, M.J.Tannenbaum, J.Thomas, S.Tonse, J.H.Van Dijk, F.Videbaek, O.Vossnack, V.Vutsadakis, F.Q.Wang, Y.Wang, H.E.Wegner, D.S.Woodruff, Y.D.Wu, X.Yang, D.Zachary, W.A.Zajc, and the E-802 Collaboration

Production of φ Mesons in Central ²⁸Si + ¹⁹⁷Au Collisions at 14.6A GeV/c

NUCLEAR REACTIONS ¹⁹⁷Au(²⁸Si, X), E at 14.6 GeV/c/nucleon; measured invariant φ yield; deduced invariant transverse mass distribution width.

doi: 10.1103/PhysRevLett.76.2021
Citations: PlumX Metrics

1995SA04      Phys.Rev. C51, 1280 (1995)

T.C.Sangster, M.Begemann-Blaich, Th.Blaich, H.C.Britt, L.F.Hansen, M.N.Namboodiri, G.Peilert

Correlations of Intermediate Mass Fragments from Fe + Ta, Au, and Th Collisions

NUCLEAR REACTIONS ¹⁸²Ta, ¹⁹⁷Au, ²³²Th(Fe, X), E=50-100 MeV/nucleon; measured σ(θ) vs fragment Z, velocity; deduced fragmenting source extent. Quantum molecular dynamics approach.

doi: 10.1103/PhysRevC.51.1280
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1994PE20      J.Phys.(London) G20, L105 (1994)

G.Peilert, T.C.Sangster, M.N.Namboodiri, H.C.Britt

The Multifragmentation Freeze-Out Volume in Heavy-Ion Collisions

NUCLEAR REACTIONS ¹⁹⁷Au(Fe, X), E=100 MeV/nucleon; analyzed σ(fragment θ, Z), other data; deduced reaction mechanism. Multi-fragmentation, two-step model.

doi: 10.1088/0954-3899/20/9/003
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1993SA17      Phys.Rev. C47, R2457 (1993)

T.C.Sangster, M.Begemann-Blaich, Th.Blaich, H.C.Britt, A.Elmaani, N.N.Ajitanand, M.N.Namboodiri

Fragment Emission Time Scale in Intermediate Energy Heavy Ion Collisions

NUCLEAR REACTIONS ¹⁹⁷Au(⁵⁶Fe, X), E=50, 100 MeV/nucleon; measured fragment charge, velocity distributions; deduced fragment emission T_1/2.

doi: 10.1103/PhysRevC.47.R2457
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1992BE01      Phys.Rev. C45, 677 (1992)

M.Begemann-Blaich, Th.Blaich, M.M.Fowler, J.B.Wilhelmy, H.C.Britt, D.J.Fields, L.F.Hansen, R.G.Lanier, D.J.Massoletti, M.N.Namboodiri, B.A.Remington, T.C.Sangster, G.L.Struble, M.L.Webb, Y.D.Chan, A.Dacal, A.Harmon, J.Pouliot, R.G.Stokstad, S.Kaufman, F.Videbaek, Z.Fraenkel

Fission from Fe and Nb Reactions with Heavy Targets at 50-100 MeV/Nucleon

NUCLEAR REACTIONS Ta, ¹⁹⁷Au, Th(Fe, F), (⁹³Nb, F), E=50-100 MeV/nucleon; measured fission σ, charge loss distribution, fragment velocity systematics, momentum transfers. Peripheral collisions, model analysis.

doi: 10.1103/PhysRevC.45.677
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2414.

1992BL01      Phys.Rev. C45, 689 (1992)

Th.Blaich, M.Begemann-Blaich, M.M.Fowler, J.B.Wilhelmy, H.C.Britt, D.J.Fields, L.F.Hansen, M.N.Namboodiri, T.C.Sangster, Z.Fraenkel

Calculation for Fission Decay from Heavy Ion Reactions at Intermediate Energies

NUCLEAR REACTIONS Ta, ¹⁹⁷Au, Th(Fe, F), (⁹³Nb, F), E=100 MeV/nucleon; analyzed data. Intranuclear cascade model, final state statistical evaporation decay.

doi: 10.1103/PhysRevC.45.689
Citations: PlumX Metrics

1992SA15      Phys.Rev. C46, 1404 (1992)

T.C.Sangster, H.C.Britt, D.J.Fields, L.F.Hansen, R.G.Lanier, M.N.Namboodiri, B.A.Remington, M.L.Webb, M.Begemann-Blaich, T.Blaich, M.M.Fowler, J.B.Wilhelmy, Y.D.Chan, A.Dacal, A.Harmon, J.Pouliot, R.G.Stokstad, S.Kaufman, F.Videbaek, Z.Fraenkel, G.Peilert, H.Stocker, W.Greiner, A.Botvina, I.N.Mishustin

Intermediate Mass Fragment Emission in Fe + Au Collisions

NUCLEAR REACTIONS ¹⁹⁷Au(Fe, X), E=50-100 MeV/nucleon; measured σ(fragment θ), charge, velocity distributions; deduced intermediate mass fragment production mechanism. Quantum molecular dynamics model.

doi: 10.1103/PhysRevC.46.1404
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2416.

1989FI07      Nucl.Phys. A495, 209c (1989)

D.J.Fields, T.C.Sangster, M.L.Webb, B.A.Remington, H.C.Britt, L.F.Hansen, R.G.Lanier, D.Massoletti, M.N.Namboodiri, G.L.Struble, M.L.Begemann-Blaich, T.Blaich, M.M.Fowler, J.Wilhelmy, S.Kaufman, F.Videbaek, Y.D.Chan, A.Dacal, A.Harmon, J.Pouliot, R.Stokstad, Z.Fraenkel

Heavy Ion Reaction Studies of Nb + Au at E/A = 50, 75 and 100 MeV

NUCLEAR REACTIONS ¹⁹⁷Au(⁹³Nb, F), E=50-100 MeV/nucleon; measured fission (fragment)(fragment)-coin, (fragment)(fragment)(θ); deduced fission mechanism.

doi: 10.1016/0375-9474(89)90320-5
Citations: PlumX Metrics

1987GA01      Phys.Rev. C35, 579 (1987)

A.Gavron, A.Gayer, J.Boissevain, H.C.Britt, T.C.Awes, J.R.Beene, B.Cheynis, D.Drain, R.L.Ferguson, F.E.Obenshain, F.Plasil, G.R.Young, G.A.Petitt, C.Butler

Neutron Emission in the Fissioning ¹⁵⁸Er Composite System

NUCLEAR REACTIONS ¹⁴²Nd(¹⁶O, F), E=207 MeV; ¹³⁴Ba(²⁴Mg, F), ¹²⁶Te(³²S, F), E=180 MeV; ¹⁰⁸Pd(⁵⁰Ti, F), E=216 MeV; measured fission (fragment)n-coin. ¹⁵⁸Er deduced fissioning characteristics. NE213 scintillators, tof. Model calculations.

doi: 10.1103/PhysRevC.35.579
Citations: PlumX Metrics

1986GA12      Phys.Lett. 176B, 312 (1986)

A.Gavron, A.Gayer, J.Boissevain, H.C.Britt, J.R.Nix, A.J.Sierk, P.Grange, S.Hassani, H.A.Weidenmuller, J.R.Beene, B.Cheynis, D.Drain, R.L.Ferguson, F.E.Obenshain, F.Plasil, G.R.Young, G.A.Petitt, C.Butler

Neutron Emission Prior to Fission

NUCLEAR REACTIONS ¹⁴²Nd(¹⁶O, F), E=207 MeV; measured fission(fragment)n-coin, σ(En, θn); deduced post, prior fission neutron multiplicity relationship. ¹⁵⁸Er deduced fission barrier, other parameters, reduced nuclear dissipation coefficient limit.

doi: 10.1016/0370-2693(86)90170-X
Citations: PlumX Metrics

1984BR14      Phys.Rev. C30, 559 (1984)

H.C.Britt, D.C.Hoffman, J.van der Plicht, J.B.Wilhelmy, E.Cheifetz, R.J.Dupzyk, R.W.Lougheed

Fission of ^255,256Es, ^255-257Fm, and ²⁵⁸Md at Moderate Excitation Energies

NUCLEAR REACTIONS, ICPND ²⁵⁴Es(d, pF), (t, pF), (³He, dF), (³He, pF), E=tandem; ²⁵⁴Es(p, F), (d, F), (t, F), E=11-17 MeV; ²⁵⁴Es(α, F), E=20-26 MeV; measured fission fragment yield, total kinetic energy vs mass, (fragment)(fragment)-coin. ^255,256Es, ^255,256,257Fm, ²⁵⁸Md deduced fission characteristics, potential energy surface role.

doi: 10.1103/PhysRevC.30.559
Citations: PlumX Metrics

1984GA03      Phys.Rev.Lett. 52, 589 (1984)

A.Gavron, P.Eskola, A.J.Sierk, J.Boissevain, H.C.Britt, K.Eskola, M.M.Fowler, H.Ohm, J.B.Wilhelmy, S.Wald, R.L.Ferguson

New Evaluation of Fission-Fragment Angular Distributions in Heavy-Ion Reactions

NUCLEAR REACTIONS ²³⁸U(¹⁶O, F), E=114, 140, 250 MeV; ²³⁸U, ¹⁷⁴Yb(¹²C, F), E=95, 188 MeV; ¹⁹⁸Pt(¹²C, F), E=95, 186 MeV; ¹⁹²Os, ¹⁷⁰Er, ¹⁴²Nd(¹⁶O, F), E=140, 250 MeV; measured fission fragment σ(θ), yield anisotropies; deduced well defined fission barrier, saddle point K quantum number roles. Transition state model, other data analysis.

doi: 10.1103/PhysRevLett.52.589
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1984GA30      Phys.Rev. C30, 1550 (1984)

A.Gavron, J.Boissevain, H.C.Britt, K.Eskola, P.Eskola, M.M.Fowler, H.Ohm, J.B.Wilhelmy, T.C.Awes, R.L.Ferguson, F.E.Obenshain, F.Plasil, G.R.Young, S.Wald

Fission Cross Sections up to 20 MeV/Nucleon

NUCLEAR REACTIONS, ICPND ¹⁷⁴Yb, ¹⁹⁸Pt, ²³⁸U(¹²C, F), E=95-291 MeV; ¹⁴²Nd, ¹⁷⁰Er, ¹⁹²Os, ²³⁸U(¹⁶O, F), E=140-315 MeV; ¹²⁶Te, ¹⁴⁴Nd, ²³⁸U(³²S, F), E=350, 500, 700; ⁹⁶Zr, ¹¹⁶Cd, ²³⁸U(⁵⁸Ni, F), E=352, 875 MeV; measured fission σ(E), fragment σ(θ) anisotropy; deduced incomplete fusion reaction role.

doi: 10.1103/PhysRevC.30.1550
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0320.

1983PO11      Phys.Rev. C28, 2299 (1983)

S.Pontoppidan, P.R.Christensen, O.Hansen, F.Videbaek, H.C.Britt, B.H.Erkkila, Y.Patin, R.H.Stokes, M.P.Webb, R.L.Ferguson, F.Plasil, G.R.Young

Quasielastic Transfer Reactions Induced by ⁵⁶Fe on ⁵⁸Ni, ⁶⁴Ni, and ¹²²Sn

NUCLEAR REACTIONS ^58,64Ni, ¹²²Sn(⁵⁶Fe, X), E=320, 460 MeV; measured fragment yield vs mass, σ(fragment θ) vs (Q) for X=^51,50V, ^{51,52,53,54,55}Cr, ^{52,53,54,55,56}Mn, ^{54,55,56,57,58,59,60}Fe, ^{56,57,58,59,60}Co, ^{57,58,59,60,61}Ni; deduced reaction mechanism. DWBA analyses.

doi: 10.1103/PhysRevC.28.2299
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1983VA23      Phys.Rev. C28, 2022 (1983)

J.van der Plicht, H.C.Britt, M.M.Fowler, Z.Fraenkel, A.Gavron, J.B.Wilhelmy, F.Plasil, T.C.Awes, G.R.Young

Fission of Polonium, Osmium, and Erbium Composite Systems

NUCLEAR REACTIONS, ICPND ¹⁷⁴Yb(¹⁶O, F), E=10 MeV/nucleon; ¹⁴²Nd(¹⁶O, F), E=95-140 MeV; ¹³⁴Ba(²⁴Mg, F), E=120-180 MeV; ¹²⁶Te(³²S, F), E=150-220 MeV; ⁹⁴Zr(⁶⁴Ni, F), E=250, 270, 290 MeV; ¹⁷⁷Hf(⁹Be, F), E=64-84 MeV; ¹⁷⁴Yb(¹²C, F), E=65-120 MeV; ¹⁷⁰Er(¹⁶O, F), E=80-150 MeV; ¹⁶⁰Gd(²⁶Mg, F), E=120-170 MeV; ¹⁹⁸Pt(¹²C, F), E=55-120 MeV; ¹⁹²Os(¹⁶O, F), E=78-150 MeV; ¹⁸⁸Os(¹⁶O, F), (¹⁸O, F), E=80-140 MeV; measured fission σ(E). ¹⁵⁸Er, ¹⁸⁶Os, ²¹⁰Po deduced fission barrier mass, angular momentum dependences.

doi: 10.1103/PhysRevC.28.2022
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0413.

1982BR22      Phys.Rev. C26, 1999 (1982)

H.C.Britt, B.H.Erkkila, A.Gavron, Y.Patin, R.H.Stokes, M.P.Webb, P.R.Christensen, O.Hansen, S.Pontoppidan, F.Videbaek, R.L.Ferguson, F.Plasil, G.R.Young, J.Randrup

Correlated Charge and Mass Distributions from Reactions of ⁵⁶Fe with ⁵⁸Ni, ⁶⁴Ni, and ¹²²Sn

NUCLEAR REACTIONS ⁵⁸Ni(⁵⁶Fe, X), E=315, 461 MeV; ⁶⁴Ni(⁵⁶Fe, X), E=464 MeV; ¹²²Sn(⁵⁶Fe, X), E=320, 460 MeV; measured σ(fragment θ) vs energy loss, fragment distribution first, second moments; deduced reaction mechanism. Transport theory.

doi: 10.1103/PhysRevC.26.1999
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1982CH26      Nucl.Phys. A390, 336 (1982)

P.R.Christensen, O.Hansen, O.Nathan, F.Videbaek, H.Freiesleben, H.C.Britt, S.Y.Van Der Werf

Bombarding Energy Dependence of Angular Momentum Transfer in Deep Inelastic Collisions

NUCLEAR REACTIONS ¹⁵⁴Sm(⁸⁶Kr, X), E=610 MeV; measured σ(fragment θ, Z), γ-multiplicities; deduced J-transfer, multiplicity distribution moments for deep inelastic collisions.

doi: 10.1016/0375-9474(82)90164-6
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1981CH18      Phys.Rev. C24, 519 (1981)

E.Cheifetz, H.C.Britt, J.B.Wilhelmy

Fission Probabilities for Actinide Nuclei Excited by the (¹²C, ⁸Be(g.s.)) Reaction

NUCLEAR REACTIONS, Fission ²³⁶U, ²³²Th(¹²C, ⁸Be), E=65 MeV; measured σ(⁸Be). ²³⁶U, ²⁴⁰Pu deduced fission probability vs excitation energy.

doi: 10.1103/PhysRevC.24.519
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1981WE05      Phys.Rev. C23, 2100 (1981)

J.Weber, H.C.Britt, J.B.Wilhelmy

Comparison of ²⁵²Cf Spontaneous Fission with ²⁵⁰Cf(t, pf)

RADIOACTIVITY, Fission ²⁵²Cf(SF); measured σ(fragment mass), average total kinetic energy vs mass.

NUCLEAR REACTIONS, Fission ²⁵⁰Cf(t, pF), E=16 MeV; measured σ(fragment mass), average total kinetic energy vs mass, excitation energy.

doi: 10.1103/PhysRevC.23.2100
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12709.

1980BR02      Phys.Rev. C21, 761 (1980)

H.C.Britt, E.Cheifetz, D.C.Hoffman, J.B.Wilhelmy, R.J.Dupzyk, R.W.Lougheed

Fission Barriers for ²⁵⁵Es, ²⁵⁶Es, and ²⁵⁵Fm

NUCLEAR REACTIONS ²⁵⁴Es(t, pF), (d, pF), (³He, dF), E not given; measured fission coin spectra. ²⁵⁵Fm, ^255,256Es deduced first barrier height.

doi: 10.1103/PhysRevC.21.761
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1980CH29      Nucl.Phys. A349, 217 (1980)

P.R.Christensen, F.Folkmann, O.Hansen, O.Nathan, N.Trautner, F.Videbaek, S.Y.Van Der Werf, H.C.Britt, R.P.Chestnut, H.Freiesleben, F.Puhlhofer

Gamma-Ray Multiplicity Moments from ⁸⁶Kr Reactions on ^144,154Sm at 490 MeV

NUCLEAR REACTIONS ^144,154Sm(⁸⁶Kr, X), E=490 MeV; measured σ(fragment θ, Z), γ-ray multiplicities; deduced J-transfer, multiplicity distribution moments for deep inelastic collisions.

doi: 10.1016/0375-9474(80)90452-2
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1979BL01      Phys.Rev. C19, 1288 (1979)

M.Blann, R.H.Stokes, B.Erkkila, H.C.Britt, P.D.Goldstone, R.L.Ferguson, F.Plasil, H.H.Gutbrod

Final and Primary Yields and Dispersions for Strongly Damped Reaction Of ⁸⁶Kr + ¹²⁴Sn

NUCLEAR REACTIONS ¹²⁴Sn(⁸⁶Kr, X), E=440, 720 MeV; measured distributions of fragment energy, mass vs atomic number; deduced primary distribution.

doi: 10.1103/PhysRevC.19.1288
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1978BR07      Phys.Rev.Lett. 40, 1010 (1978)

H.C.Britt, A.Gavron, P.D.Goldstone, R.Schoenmackers, J.Weber, J.B.Wilhelmy

Yet More Complexity in Fission: Barriers for Nuclei with N = 150-154

NUCLEAR REACTIONS ²⁴⁴Pu, ^246,248Cm, ²⁵⁰Cf(t, p), (d, p), (p, p'), E not given; measured fission probability distributions.

doi: 10.1103/PhysRevLett.40.1010
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1978CH08      Phys.Rev.Lett. 40, 1245 (1978)

P.R.Christensen, F.Folkmann, O.Hansen, O.Nathan, N.Trautner, F.Videbaek, S.Y.van der Werf, H.C.Britt, R.P.Chestnut, H.Freiesleben, F.Puhlhofer

Gamma-Ray Multiplicity Moments from Deeply Inelastic Collisions of ⁸⁶Kr and ¹⁴⁴Sm

NUCLEAR REACTIONS ¹⁴⁴Sm(⁸⁶Kr, X), E=490 MeV; measured γ-multiplicity.

doi: 10.1103/PhysRevLett.40.1245
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1978PL02      Phys.Rev.Lett. 40, 1164 (1978)

F.Plasil, R.L.Ferguson, H.C.Britt, R.H.Stokes, B.H.Erkkila, P.D.Goldstone, M.Blann, H.H.Gutbrod

Measurement of the Energy Division Versus Mass in Highly Damped Reactions

NUCLEAR REACTIONS ¹²⁴Sn(⁸⁶Kr, X), E=440, 720 MeV; measured σ(A, Z).

doi: 10.1103/PhysRevLett.40.1164
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1978PL07      Phys.Rev. C18, 2603 (1978)

F.Plasil, R.L.Ferguson, H.C.Britt, B.H.Erkkila, P.D.Goldstone, R.H.Stokes, H.H.Gutbrod

Evaporation Residue Products from Reactions with ⁸⁶Kr

NUCLEAR REACTIONS ⁶⁵Cu, ⁹⁰Zr, ¹⁰⁹Ag(⁸⁶Kr, X), E=366-716 MeV; measured evaporation residue σ(θ). ⁶⁵Cu(⁸⁶Kr, X), E=366, 716 MeV; measured A, Z distributions of evaporation residue products.

doi: 10.1103/PhysRevC.18.2603
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1978WI12      S.Afr.J.Phys. 1, 116 (1978)

J.B.Wilhelmy, H.C.Britt, D.C.Hoffman, W.R.Daniels, E.Cheifetz, A.Gavron, J.Weber, E.K.Hulet, J.H.Landrum, R.W.Lougheed, J.F.Wild

Fission Properties of the Heavy Actinides

NUCLEAR REACTIONS ²⁵⁴Es(d, pF), (t, pF), E not given; measured fission barriers.

RADIOACTIVITY, Fission ²⁵⁶Cf(SF) [from ²⁵⁴Cf(t, p)]; ²⁵⁸Fm(SF) [from ²⁵⁵Es(α, n)²⁵⁸Md+electron capture]; ²⁵⁹Fm(SF) [from ²⁵⁷Fm(t, p)]; measured fragment mass distribution, average kinetic energy release.

1977BR30      Phys.Rev.Lett. 39, 1458 (1977)

H.C.Britt, B.H.Erkkila, P.D.Goldstone, R.H.Stokes, B.B.Back, F.Folkmann, O.Christensen, B.Fernandez, J.D.Garrett, G.B.Hagemann, B.Herskind, D.L.Hillis, F.Plasil, R.L.Ferguson, M.Blann, H.H.Gutbrod

Angular Momentum Limits in Fusion Reactions Induced by Argon and Krypton Projectiles

NUCLEAR REACTIONS ^122,124Sn(⁴⁰Ar, X), ⁷⁶Ge(⁸⁶Kr, X); measured γ-multiplicity. ^70,74Ge(⁸⁶Kr, X); measured σ(A, Z).

doi: 10.1103/PhysRevLett.39.1458
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1977GA09      Phys.Rev. C15, 2238 (1977)

A.Gavron, H.C.Britt, P.D.Goldstone, R.Schoenmackers, J.Weber, J.B.Wilhelmy

Γn/Γf in Heavy Actinides

NUCLEAR REACTIONS ²⁴⁴Pu, ^245,246,248Cm, ^249,250Cf(³He, d), (³He, t), E=8, 11 MeV; measured fission probability of compound systems ^244,245Am, ^{245,246,247,248,249}Bk, ^249,250,251Es.

doi: 10.1103/PhysRevC.15.2238
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1977GA11      Phys.Rev.Lett. 38, 1457 (1977)

A.Gavron, H.C.Britt, P.D.Goldstone, J.B.Wilhelmy, S.E.Larsson

Complexity of the Potential-Energy Surface for Fission of ²³⁸U

NUCLEAR STRUCTURE ²³⁸U; calculated fission saddle points.

doi: 10.1103/PhysRevLett.38.1457
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1977GO05      Phys.Rev.Lett. 38, 1262 (1977)

P.D.Goldstone, H.C.Britt, R.Schoenmackers, J.B.Wilhelmy

Determination of Γn/Γf at 12 to 20 MeV Excitation from Evaporation-Residue Cross Sections

NUCLEAR REACTIONS ¹⁹⁷Au, ²³²Th, ²³⁶U(⁷Li, α), E=34 MeV; measured σ(Eα); deduced evaporation-residue probabilities.

doi: 10.1103/PhysRevLett.38.1262
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1976BR10      Phys.Rev. C13, 1483 (1976)

H.C.Britt, B.H.Erkkila, R.H.Stokes, H.H.Gutbrod, F.Plasil, R.L.Ferguson, M.Blann

Argon- and Krypton-Induced Reactions at Energies of 4-7 MeV/amu

NUCLEAR REACTIONS ¹⁰⁹Ag(⁴⁰Ar, X), E=169-337 MeV; ¹²¹Sb(⁴⁰Ar, X), E=282, 340 MeV; ⁶⁵Cu(⁸⁴Kr, X), E=494, 604 MeV; measured elastic scattering, evaporation residue, fission, fusion σ.

doi: 10.1103/PhysRevC.13.1483
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1976GA11      Phys.Rev. C13, 2374 (1976)

A.Gavron, H.C.Britt, E.Konecny, J.Weber, J.B.Wilhelmy

Γn/Γf for Actinide Nuclei Using (³He, df) and (³He, tf) Reactions

NUCLEAR STRUCTURE ^{230,231,232,233}Pa, ^231,232U, ^{233,234,235,236,237,238,239}Np, ^237,238Pu, ^{239,240,241,242,243}Am, ^{241,242,243,244}Cm; measured fission probability in ³He induced reactions; deduced barrier heights, average Γn/Γf.

NUCLEAR REACTIONS ^230,232Th, ²³¹Pa, ^234,236,238U, ²³⁷Np, ^239,241Pu, ^241,243Am(³He, df), (³He, tf); ²³²U, ²⁴²Pu(³He, df); E=25 MeV; measured fission spectra; deduced barrier heights, average neutron-, fission-widths. ^{230,231,232,233}Pa, ^231,232U, ^{233,234,235,236,237,238,239}Np, ^237,238Pu, ^{239,240,241,242,243}Am, ^{241,242,243,244}Cm deduced fission probability.

doi: 10.1103/PhysRevC.13.2374
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1976WE13      Phys.Rev. C13, 2413 (1976)

J.Weber, H.C.Britt, A.Gavron, E.Konecny, J.B.Wilhelmy

Fission of ²²⁸Ra

NUCLEAR REACTIONS ²²⁶Ra(t, F), E=23 MeV; measured symmetric, asymmetric component fission probability; deduced fission barrier parameters, mass distributions.

doi: 10.1103/PhysRevC.13.2413
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1975GA02      Phys.Rev.Lett. 34, 827 (1975)

A.Gavron, H.C.Britt, E.Konecny, J.Weber, J.B.Wilhelmy

Measurement and Interpretation of Gamma(n)/Gamma(f) for Actinide Nuclei

NUCLEAR REACTIONS ²³²Th, ²³¹Pa, ²³⁶U, ²³⁷Np, ²⁴⁰Pu, ²⁴¹Am(³He, dF), (³He, tF). ^232,233Pa, ^231,232U, ^236,237Np, ^237,238Pu, ^240,241Am, ^241,242Cm; measured σ; deduced neutron-to-fission width.

doi: 10.1103/PhysRevLett.34.827
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1974BA28      Phys.Rev. C9, 1924 (1974)

B.B.Back, O.Hansen, H.C.Britt, J.D.Garrett

Fission of Doubly Even Actinide Nuclei Induced by Direct Reactions

NUCLEAR REACTIONS ^230,232Th, ^234,236,238U, ^238,240,242Pu, ²⁴⁸Cm(t, pF), E=15 MeV; ²³¹Pa(t, αF), E=16 MeV; ²³¹Pa, ²³⁷Np, ²⁴³Am(³He, dF), E=24 MeV; ²³³U(d, pF), E=13 MeV; ²⁴⁸Cm(p, p'F), E=22.5 MeV; measured E(fragment), I(fragment). ^230,232,234Th, ^{232,234,236,238,240}U, ^{238,240,242,244}Pu, ^244,248,250Cm deduced fission probability.

doi: 10.1103/PhysRevC.9.1924
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1974BA73      Phys.Rev. C10, 1948 (1974)

B.B.Back, H.C.Britt, O.Hansen, B.Leroux, J.D.Garrett

Fission of Odd-A and Doubly Odd Actinide Nuclei Induced by Direct Reactions

NUCLEAR REACTIONS ^230,232Th(³He, αF), ^230,232Th, ^{233,234,235,236,238}U, ^239,240,242Pu, ²⁴⁸Cm(³He, dF), E=24 MeV; ²³⁰Th, ²³¹Pa, ²³⁷Np, ²⁴⁸Cm(d, pF), E=15 MeV; ²⁴³Am, ²³⁹Pu(t, pF), E=15 MeV; ²⁴⁸Cm(t, αF), E=16 MeV; measured fission probabilities. ^229,231Th, ^231,232,233Pa, ^{234,235,236,237,238,239}Np, ²⁴¹Pu, ^{240,241,243,245,247}Am, ²⁴⁹Cm, ²⁴⁹Bk deduced barrier heights.

doi: 10.1103/PhysRevC.10.1948
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1974BR03      Phys.Rev. C9, 435 (1974)

H.C.Britt, J.R.Huizenga

Reevaluation of Experimental Estimates of the Pairing Gap at the Fission Saddle Point

NUCLEAR STRUCTURE ²³⁶U, ²⁴⁰Pu; reevaluate pairing gap at fission saddle point.

doi: 10.1103/PhysRevC.9.435
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1974FR07      Phys.Rev. C10, 245 (1974)

H.Freiesleben, H.C.Britt, J.Birkelund, J.R.Huizenga

⁶Li, ⁷Li Induced Reactions on ²⁰⁹Bi

NUCLEAR REACTIONS ²⁰⁹Bi(⁶Li, xn), (⁷Li, xn), (⁶Li, F), (⁷Li, F), (⁷Li, xnα), (⁷Li, xnt), ²⁰⁹Bi(⁷Li, αp), (⁶Li, xnd), (⁶Li, α), E=25-34 MeV; measured σ(E).

doi: 10.1103/PhysRevC.10.245
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1974HU08      Nucl.Phys. A223, 589 (1974)

J.R.Huizenga, A.N.Behkami, R.W.Atcher, J.S.Sventek, H.C.Britt, H.Freiesleben

Comparison of Neutron Resonance Spacings with Microscopic Theory for Nuclei with Static Deformation

COMPILATION A=150-248; compiled level spacings.

doi: 10.1016/0375-9474(74)90708-8
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1973BA55      Phys.Lett. 46B, 183 (1973)

B.B.Back, O.Hansen, H.C.Britt, J.D.Garrett

Fission Barriers for Cm Isotopes; What Is the Nature of the N = 152 Shell

NUCLEAR REACTIONS, Fission ²⁴³Am(³He, dF), ²⁴⁸Cm(p, p'F), (d, pF), (t, pF), Et=15 MeV, Ep=22.5 MeV; measured fission barrier heights for ^{244,248,249,250}Cm. Deduced Q.

doi: 10.1016/0370-2693(73)90678-3
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1973BR04      Phys.Rev. C7, 801 (1973)

H.C.Britt, M.Bolsterli, J.R.Nix, J.L.Norton

Fission Barriers Deduced from the Analysis of Fission Isomer Results

doi: 10.1103/PhysRevC.7.801
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1973BR38      At.Data Nucl.Data Tables 12, 407 (1973)

H.C.Britt

Properties of Fission Isomers

doi: 10.1016/0092-640X(73)90001-6
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1972BA46      Phys.Rev.Lett. 28, 1707 (1972)

B.B.Back, H.C.Britt, J.D.Garrett, O.Hansen

Subbarrier Fission Resonances in Th Isotopes

NUCLEAR REACTIONS, Fission ^230,232Th(t, pF), ²³⁰Th(d, pF), E=15 MeV; measured (fragment)(p)-coin; deduced fission probability. ²³¹Th, ^232,234Th deduced subbarrier fission resonances, fission barrier parameters.

doi: 10.1103/PhysRevLett.28.1707
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1972BE52      Phys.Rev. C6, 1087 (1972)

G.R.Bethune, H.C.Britt, B.H.Erkkila

Excitation Function for the ²³⁵U(α, 3n)²³⁶Pu Reaction

NUCLEAR REACTIONS ²³⁵U(α, 3n), (α, t), (α, F), E=24.5-28 MeV; measured σ(E).

doi: 10.1103/PhysRevC.6.1087
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1972BR35      Phys.Rev. C6, 1090 (1972)

H.C.Britt, B.H.Erkkila, B.B.Back

Excitation Functions for the Production of Fission Isomers in Various Am Isotopes

RADIOACTIVITY, Fission ^239mAm, ^245mAm; measured T_1/2.

NUCLEAR REACTIONS ^{239,240,242,244}Pu(p, 2n), (t, 2n), (t, 3n), E=10-16 MeV; measured σ for SF-isomer production.

doi: 10.1103/PhysRevC.6.1090
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1972RI08      Phys.Rev. C5, 2072 (1972)

F.A.Rickey, E.T.Jurney, H.C.Britt

Level Scheme of ²³⁵U and the Distribution of Single-Particle Strength in its Excited States

NUCLEAR REACTIONS ²³⁴U(n, γ), E=thermal; measured Eγ, Iγ; deduced Q. ²³⁴U(d, p), E=20 MeV; measured σ(Ep, θ). ²³³U(t, p), E=20 MeV; measured σ(Ep). ²³⁵U(d, d'), E=20 MeV; measured σ(Ed'). ²³⁶U(d, t), E=20 MeV; measured σ(Et). ²³⁵U deduced levels, J, π, L.

doi: 10.1103/PhysRevC.5.2072
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1971BR38      Phys.Rev. C4, 1441 (1971)

H.C.Britt, B.H.Erkkila

Population of Fission Isomers in ²³⁶U by the (d, p) Reaction

NUCLEAR REACTIONS, Fission ²³⁵U(d, pf), (d, p), E=12 MeV; measured σ ratios, σ(Ep), (d)(fragment)-delay. ^236mU deduced T_1/2.

RADIOACTIVITY, Fission ^236mU; measured T_1/2.

doi: 10.1103/PhysRevC.4.1441
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1971BR39      Phys.Rev. C4, 1444 (1971)

H.C.Britt, S.C.Burnett, B.H.Erkkila, J.E.Lynn, W.E.Stein

Systematics of Spontaneously Fissioning Isomers

RADIOACTIVITY, Fission ^{235m,237m,238m,239m,240m,241m}Pu, ^{241m,242m,243m,244m,245m}Cm, ^236mU, ^{239m,240m,242m,243m,244m}Am(SF); measured T_1/2, T_1/2 lower limits.

NUCLEAR REACTIONS ^{233,235,236,238}U, ²³⁷Np, ^{239,240,242,244}Pu(α, xn), E=20-29 MeV; ²³⁵U, ²³⁷Np, ^{239,240,242,244}Pu, ²⁴³Am(d, p), (d, np), E=20-29 MeV; measured isomeric σ ratios(E); deduced thresholds for SF-isomer production.

doi: 10.1103/PhysRevC.4.1444
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1970BR32      Phys.Rev. C2, 1758 (1970)

H.C.Britt, J.D.Cramer

Fission of Odd-A Uranium and Plutonium Isotopes Excited by (d, p), (t, d), and (t, p) Reactions

NUCLEAR REACTIONS ^234,236,238U, ²⁴²Pu(d, pF), ^233,235U, ²³⁹Pu(t, pF), ²³⁶U, ^240,242Pu(t, dF), E=18 MeV; measured (p)(fragment)(θ), (d)(fragment)(θ). ^235,237,239U, ^241,243Pu deduced fission probabilities.

doi: 10.1103/PhysRevC.2.1758
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1970BU02      Phys.Lett. 31B, 523 (1970)

S.C.Burnett, H.C.Britt, B.H.Erkkila, W.E.Stein

Systematics of Plutonium Fission Isomers

RADIOACTIVITY, Fission ^233mPu, ^237mPu, ^238mPu, ^239mPu, ^240mPu(SF); measured T_1/2.

NUCLEAR REACTIONS ^{233,235,236,238}U(α, 2n), E=20-28 MeV; ²³⁴U(α, xn), ²³⁶U(α, n), ²³⁸U(α, n), (α, 3n), E=20-29 MeV; measured isomeric σ ratios(E); deduced thresholds for SF-isomer production.

doi: 10.1016/0370-2693(70)90080-8
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1970CO11      Phys.Rev. C1, 945 (1970)

E.R.Cosman, R.Kalish, D.D.Armstrong, H.C.Britt

Analog States of ⁸⁹Sr and the Particle-Core Model in the N = 50 Region

NUCLEAR REACTIONS ⁸⁸Sr(p, p), (p, p'), E=4.8-12 MeV; measured σ(E;Ep'). ⁸⁹Y deduced isobaric analog resonances, J, π.

doi: 10.1103/PhysRevC.1.945
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1970CR09      Phys.Rev. C2, 2350 (1970)

J.D.Cramer, H.C.Britt

Fission Studies of Thorium, Uranium, and Plutonium Isotopes with (t, pf) Reactions

NUCLEAR REACTIONS, Fission ^230,232Th, ^234,236,238U, ^238,240,242Pu(t, pF), E=18 MeV; measured σ(E, E(fragment), θ(fragment)), (fragment)(fragment)(θ). ^232,234Th, ^236,238,240U, ^240,242,244Pu deduced fission probability.

doi: 10.1103/PhysRevC.2.2350
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1969BR11      Phys.Rev. 185, 1553 (1969)

H.C.Britt, J.D.Cramer

(t, p) Q Values for Th, U, and Pu Isotopes

NUCLEAR REACTIONS ²³²Th, ^235,236,238U, ^239,240Pu(t, p), E = 18 MeV; measured Q, σ(Ep).

doi: 10.1103/PhysRev.185.1553
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1969BR17      Phys.Rev. 181, 1634 (1969)

H.C.Britt, J.D.Cramer

Fission-Fragment Angular Correlations for ²³³U, ²³⁵U, and ²³⁹Pu(t, df) Reactions

NUCLEAR REACTIONS, Fission ^233,235U, ²³⁹Pu(t, dF), E = 18 MeV; measured fission fragment correlations; deduced fission probabilities.

doi: 10.1103/PhysRev.181.1634
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1968AL09      Phys.Letters 27B, 11 (1968)

D.L.Allan, H.C.Britt, F.A.Rickey, Jr.

Analogue States and the Nuclear Structure of ¹⁸¹Hf

NUCLEAR STRUCTURE ¹⁸¹Ta; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(68)90319-5
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1968BR32      Phys.Rev. 175, 1525 (1969)

H.C.Britt, F.A.Rickey, Jr., W.S.Hall

Characteristics of the Transition-State Spectra for ²³⁴U, ²³⁶U, and ²⁴⁰Pu from (d, pf) and (t, pf) Angular-Correlation Experiments

NUCLEAR REACTIONS ^233,235U, ²³⁹Pu(d, pF), E = 15, 18 MeV; ²³⁴U(t, pF), E = 18 MeV; measured σ(Ep, θ(fragment)). ^234,236U, ²⁴⁰Pu deduced vibrational bands. ²³⁶U, ²⁴⁰Pu deduced pairing energy gap.

doi: 10.1103/PhysRev.175.1525
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1967RI12      Bull.Am.Phys.Soc. 12, No.4, 522, EF8 (1967); Priv.Comm. (1970)

F.A.Rickey, Jr., H.C.Britt

Levels in ²³⁵U Excited by (d, p), (d, t), and (t, p) Reactions

NUCLEAR STRUCTURE ²³⁵U; measured not abstracted; deduced nuclear properties.

1965BR40      Phys.Rev. 139, B354 (1965)

H.C.Britt, W.R.Gibbs, J.J.Griffin, R.H.Stokes

(d, p-f) Angular-Correlation Study of Fission-Barrier Transition States: Energy Gap of a Highly Deformed Nucleus

NUCLEAR REACTIONS, Fission ²³³U, ²³⁹Pu(d, pF), E=14.9 MeV; measured σ(Ep, θ(p), θ(fragment)). ²³⁴U, ²⁴⁰Pu deduced fission-barrier transition states.

doi: 10.1103/PhysRev.139.B354
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1964BR44      Phys.Rev. 133, B603 (1964)

H.C.Britt, S.L.Whetstone, Jr.

Alpha-Particle-Induced Fission of Th²³⁰, Th²³², and U²³³

NUCLEAR REACTIONS ^230,232Th, ²³³U(α, F), E=22.1, 25.7, 29.5 MeV; measured fission products; deduced yields, average initial total kinetic energies, mass distributions.

RADIOACTIVITY ²⁵²Cf(SF); measured decay products; deduced mass distributions.

doi: 10.1103/physrev.133.b603
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1963BR34      Phys.Rev. 129, 2239 (1963)

H.C.Britt, H.E.Wegner, J.C.Gursky

Energetics of Charged Particle-Induced Fission Reactions

NUCLEAR REACTIONS ¹⁹⁷Au, Tl, ²⁰⁶Pb, ²⁰⁹Bi(³He, F), E=25.5 MeV;²²⁶Ra(d, F), E=9.8, 11.7, 14 MeV; ²²⁶Ra(α, F), E=22.1, 27.1 MeV; ²²⁶Ra(³He, F), E=20.9, 23.4 MeV; ²³⁰Th(p, F), E=6.8, 8 MeV; ²³³U(α, F), E=25.5 MeV; measured reaction products; deduced symmetric and asymmetric fission yields, total kinetic energies of fragments.

RADIOACTIVITY ²⁵²Cf(SF); measured decay products; deduced symmetric and asymmetric fission yields, total kinetic energies of fragments.

doi: 10.1103/PhysRev.129.2239
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1961BR20      Phys.Rev. 124, 877 (1961) H.C.Britt, A.R.Quinton - Phys.Rev. 124, 877 (1961)

H.C.Britt, A.R.Quinton

Alpha Particles and Protons Emitted in the Bombardment of Au¹⁹⁷ and Bi²⁰⁹ by C¹², N¹⁴, and O¹⁶ Projectiles

doi: 10.1103/PhysRev.124.877
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