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Search: Author = P.R.Christensen

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2012NA18      Phys.Rev. C 86, 024916 (2012)

P.Naselsky, C.H.Christensen, P.R.Christensen, P.H.Damgaard, A.Frejsel, J.J.Gaardhoje, A.Hansen, M.Hansen, J.Kim, O.Verkhodanov, U.A.Wiedemann

Morphology of high-multiplicity events in heavy ion collisions

doi: 10.1103/PhysRevC.86.024916
Citations: PlumX Metrics


1986TR07      Phys.Rev. C34, 1299 (1986)

W.Trautmann, P.D.Bond, O.Hansen, M.J.LeVine, C.E.Thorn, F.Videbaek, P.R.Christensen

Transfer Reactions for 28Si + 28Si at E(lab) = 151.25 MeV

NUCLEAR REACTIONS 28Si(28Si, xnyp)29Si/27Si/27Al/29P, E=151.25 MeV; measured σ(θ) for residuals production. 27,29Si, 27Al, 29P levels deduced spectroscopic factors. Enriched target, magnetic spectrometer. DWBA analysis.

doi: 10.1103/PhysRevC.34.1299
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1984BA29      Phys.Rev. C29, 2392 (1984)

A.J.Baltz, P.D.Bond, O.Hansen, Jiang Cheng-Lie, P.R.Christensen, S.Pontoppidan, F.Videbaek, D.Schull, Shen Wen-Qing, H.Freiesleben

Single Neutron Transfer Induced by Massive Heavy Ions

NUCLEAR REACTIONS 208Pb(86Kr, 87Kr), E=695 MeV; measured σ(E(87Kr)), σ(θ); deduced quasielastic transfer contribution to reaction σ. 87Kr, 207Pb deduced average excitation energy ratio. Single neutron pickup DWBA analysis.

doi: 10.1103/PhysRevC.29.2392
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1984CH01      Phys.Rev. C29, 455 (1984)

P.R.Christensen, S.Pontoppidan, F.Videbaek, J.Barrette, P.D.Bond, O.Hansen, C.E.Thorn

Scattering of 28Si from 208Pb

NUCLEAR REACTIONS 208Pb(28Si, 28Si), (28Si, 28Si'), E=209.8 MeV; measured σ(θ); deduced ion-ion potential diffusivity parameter. 28Si, 208Pb levels deduced deformation lengths.

doi: 10.1103/PhysRevC.29.455
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1983CH20      Phys.Rev. C28, 159 (1983)

P.R.Christensen, S.Pontoppidan, F.Videbaek, P.D.Bond, O.Hansen, C.E.Thorn, M.J.LeVine, Jiang Cheng-Lie

Excitation of the Lowest 4+ and 3- States in the 60Ni(28Si, 28Si') Reaction

NUCLEAR REACTIONS 60Ni(28Si, 28Si'), E=140 MeV; measured σ(E(28Si)), σ(θ); deduced optical model parameters. 60Ni levels deduced deformation length parameters. Coupled-channels model.

doi: 10.1103/PhysRevC.28.159
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1983JI03      Chin.J.Nucl.Phys. 5, 150 (1983)

Jiang Chenglie, P.R.Christensen, O.Hansen, S.Pontoppidan, F.Videbaek, P.D.Bond, D.Schull, Shen Wenqing, H.Freiesleben, F.Busch, E.R.Flynn

A Semiclassical Model Used for Elastic and Inelastic Scattering of Heavy Ions

NUCLEAR REACTIONS 208Pb(86Kr, 86Kr), (86Kr, 86Kr'), E=695 MeV; calculated σ(θ), Coulomb excitation. 184W(18O, 18O), E=90 MeV; 209Bi(84Kr, 84Kr), E=600 MeV; 209Bi(136Xe, 136Xe), E=1130 MeV; calculated σ(θ). Semi-classical model.


1983JI05      Chin.J.Nucl.Phys. 5, 27 (1983)

Jiang Chenglie, P.R.Christensen, O.Hansen, S.Pontoppidan, F.Videbaek, P.D.Bond, D.Schull, Shen Wenqing, H.Freiesleben, F.Busch, E.R.Flynn

Obtaining of the High Energy-Resolution Spectra of Heavy-Ion on a QQDQ Magnetic Spectrometer

NUCLEAR REACTIONS 208Pb(86Kr, X), E=695 MeV; measured fragment spectra. High resolution, QQDQ magnetic spectrometer.


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, 51,52,53,54,55Cr, 52,53,54,55,56Mn, 54,55,56,57,58,59,60Fe, 56,57,58,59,60Co, 57,58,59,60,61Ni; deduced reaction mechanism. DWBA analyses.

doi: 10.1103/PhysRevC.28.2299
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1982BO25      Phys.Lett. 114B, 423 (1982)

P.D.Bond, O.Hansen, C.E.Thorn, M.J.LeVine, P.R. Christensen, S.Pontoppidan, F.Videbaek, Jiang Cheng-Lie, M.J.Rhoades-Brown

Mutual Inelastic Excitation of 28Si + 60Ni

NUCLEAR REACTIONS 60Ni(28Si, 28Si), (28Si, 28Si'), E= 140 MeV; measured σ(θ). 28Si, 60Ni levels deduced sequential, simultaneous excitation. Coupled-channels method.

doi: 10.1016/0370-2693(82)90084-3
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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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1981BR19      Phys.Lett. 105B, 89 (1981)

R.A.Broglia, P.R.Christensen, C.H.Dasso, O.Hansen, G.Pollarolo, A.Winther

Analysis of Elastic Scattering of very Heavy Ions with Poor Energy and Mass Resolution

NUCLEAR REACTIONS 144Sm(86Kr, 86Kr), E=493, 614 MeV; calculated σ(θ), transmission coefficients. Surface excitation model, Christensen-Winther ion-ion potential.

doi: 10.1016/0370-2693(81)90995-3
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1981JI04      Phys.Rev.Lett. 47, 1039 (1981)

Jiang Cheng-Lie, P.R.Christensen, O.Hansen, S.Pontoppidan, F.Videbaek, D.Schull, Shen Wen-Qing, A.J.Baltz, P.D.Bond, H.Freiesleben, F.Busch, E.R.Flynn

Elastic and Inelastic Scattering of 86Kr from 208Pb at 695 MeV

NUCLEAR REACTIONS 208Pb(86Kr, 86Kr), (86Kr, 86Kr'), E=695 MeV; measured σ(θ), σ(E(86Kr)); deduced ion-ion potential. Magnetic spectrometer. Coupled-channels calculation.

doi: 10.1103/PhysRevLett.47.1039
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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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1979AR05      Nucl.Phys. A320, 479 (1979)

K.P.Artemov, V.Z.Goldberg, I.P.Petrov, V.P.Rudakov, I.N.Serikov, V.A.Timofeev, P.R.Christensen

About the Limits of Existence of α-Cluster Structure in Nuclei

NUCLEAR REACTIONS 12C(6Li, d), E=35 MeV; measured dα-coin spectrum, dα(θ) following 16O breakup. 12C, 16O(α, α), E=17-23 MeV; measured σ(Eα). 16O deduced α-cluster states.

doi: 10.1016/0375-9474(79)90202-1
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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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1977CH10      Nucl.Phys. A280, 189 (1977)

P.R.Christensen, Z.E.Switkowski, R.A.Dayras

Sub-Barrier Fusion Measurements for 12C + 16O

NUCLEAR REACTIONS 12C(16O, X), E(cm)=3.9-12.0 MeV; measured γ-yields for 20Ne, 23Na, 24,26Mg, 26,27Al products; deduced total fusion σ. Ge(Li) detector, natural targets.

doi: 10.1016/0375-9474(77)90303-7
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1977CH11      Nucl.Phys. A280, 205 (1977)

P.R.Christensen, Z.E.Switkowski

IWB Analysis of Scattering and Fusion Cross Sections for the 12C + 12C, 12C + 16O and 16O + 16O Reactions for Energies Near and below the Coulomb Barrier

NUCLEAR REACTIONS 12C(12C, 12C), (12C, X), 12C, 16O(16O, 16O), (16O, X); calculated elastic, fusion σ(E).

doi: 10.1016/0375-9474(77)90304-9
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1977SW01      Phys.Rev. C15, 449 (1977)

Z.E.Switkowski, H.Winkler, P.R.Christensen

Structure in Gamma-Ray Yields from the 12C + 16O Reaction Above the Coulomb Barrier

NUCLEAR REACTIONS 12C(16O, X), E(cm)=10.85-27.36 MeV; measured σ(E, Eγ).

doi: 10.1103/PhysRevC.15.449
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1976VI01      Nucl.Phys. A256, 301 (1976)

F.Videbaek, P.R.Christensen, O.Hansen, K.Ulbak

Coulomb-Nuclear Interference and Nuclear Reorientation in the Scattering of 16,18O by 58Ni and 64Ni

NUCLEAR REACTIONS 58Ni(18O, 18O), E=50, 60 MeV; 64Ni(16O, 16O), E=50 MeV; 64Ni(18O, 18O), E=50 MeV; measured σ(θ) for ground state, first 2+ in Ni, first 2+ in 18O; deduced optical model potentials, vibrational amplitude. Enriched targets.

doi: 10.1016/0375-9474(76)90110-X
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1975WI07      Nucl.Phys. A244, 147 (1975)

J.Wilczynski, K.Siwek-Wilczynska, J.S.Larsen, J.C.Acquadro, P.R.Christensen

Optimum Q-Values for the 58Ni(16O, 12C) Reaction Well Above the Coulomb Barrier

NUCLEAR REACTIONS 58Ni(16O, 12C), E=60, 72, 81 MeV; measured σ(θ, E); deduced tangential friction parameter, energy dependence of optimum Q. Surface-barrier detector telescopes. Enriched target.

doi: 10.1016/0375-9474(75)90014-7
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1974SI19      Nucl.Phys. A229, 461 (1974)

K.Siwek-Wilczynska, J.Wilczynski, P.R.Christensen

Elastic and Inelastic Scattering in the 16O + 24Mg System

NUCLEAR REACTIONS 24Mg(16O, 16O), (16O, 16O'), E=47-72 MeV; measured σ(E), σ(θ); deduced optical model parameters. 24Mg deduced quadrupole deformation parameter by DWBA, coupled channel analyses. Surface-barrier detector telescopes. Enriched target.

doi: 10.1016/0375-9474(74)90664-2
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1973BE12      Phys.Lett. 43B, 279 (1973)

F.D.Becchetti, P.R.Christensen, V.I.Manko, R.J.Nickles

Ambiguities in Spectroscopic Factors Deduced from a DWBA Analysis of the (16O, 15N) Reaction

NUCLEAR REACTIONS 40,48Ca, 50Ti, 52Cr, 54Fe, 58,60,62,64Ni, 86,88Sr, 90,92,94,96Zr, 92Mo(16O, 15N), E approx 60 MeV; measured σ(E(15N), θ). 41,49Sc, 55Co, 59,65Cu, 87,89Y, 93,97Nb; deduced S.

doi: 10.1016/0370-2693(73)90439-5
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1973BE13      Nucl.Phys. A203, 1 (1973)

F.D.Becchetti, P.R.Christensen, V.I.Manko, R.J.Nickles

Elastic and Inelastic Scattering of 16O and 12C from A = 40-96 Nuclei

NUCLEAR REACTIONS 40,48Ca, 50Ti, 52Cr, 54Fe, 58,60,62,64Ni, 86,88Sr, 92,96Zr, 92Mo(16O, 16O), E=60 MeV; 96Zr(16O, 16O), E=49 MeV; 96Zr(12C, 12C), E=38 MeV; 96Zr(12C, 12C'), E=38 MeV; 48Ca, 54Fe, 58Ni, 88Sr, 96Zr(16O, 16O'), E=60 MeV; measured σ(θ); deduced optical model parameters. 48Ca, 54Fe, 58Ni, 88Sr, 96Zr, deduced deformation parameters β.

doi: 10.1016/0375-9474(73)90420-X
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1973CH10      Nucl.Phys. A207, 33 (1973)

P.R.Christensen, V.I.Manko, F.D.Becchetti, R.J.Nickles

A Study of 16,18O and 12C Induced Reactions on A = 40-96 Nuclei

NUCLEAR REACTIONS 58Ni(16O, 13N), 54Fe(16O, 15O), 40,48Ca, 50Ti, 52Cr, 54Fe, 58,60,62,64Ni, 86,88Sr, 90,92,94Zr, 92Mo(16O, 16O), (16O, 15N), (16O, 12C), 50Ti, 52Cr, 54Fe, 58,60,62,64Ni, 86,88Sr, 90,92,94Zr, 92Mo(16O, 14C), 48Ca, 92,94,96Zr(16O, 17O), 54Fe, 86,88Sr, 90Zr(16O, 14N), 58Ni, 88Sr(16O, 13C), 54Fe, 58,60Ni, 64Zn, 90Zr(18O, 20Ne), (18O, 19F), (18O, 18O), 54Fe, 58,60Ni(18O, 16O), E=60 MeV; 96Zr(12C, 12C), (12C, 13C), (12C, 11B), E=38 MeV; 90Zr(16O, 16O), (16O, 14N), (16O, 15N), (16O, 12C), (16O, 14C), (18O, 20Ne), (18O, 19F), (18O, 18O), E=66 MeV; 96Zr(16O, 16O), (16O, 17O), (16O, 15N), (16O, 12C), (16O, 14C), E=47, 49 MeV; measured σ(θ); deduced optical model parameters, Q-value effects, particle transfer probabilities.

doi: 10.1016/0375-9474(73)90023-7
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1973CH13      Nucl.Phys. A207, 433 (1973)

P.R.Christensen, I.Chernov, E.E.Gross, R.Stokstad, F.Videbaek

The Interference of Coulomb and Nuclear Excitation in the Scattering of 16O from 58Ni, 88Sr and 142Nd

NUCLEAR REACTIONS 58Ni(16O, 16O), E=35-60 MeV; 88Sr(16O, 16O), E=45-60 MeV; 142Nd(16O, 16O), E=54-72 MeV; measured dσ(θ, E) for g.S., first 2+ state. 58Ni, 88Sr, 142Nd deduced optical model potentials, (βr), B(E2). Enriched targets.

doi: 10.1016/0375-9474(73)90854-3
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1973CH23      Phys.Lett. 45B, 107 (1973)

P.R.Christensen, O.Hansen, J.S.Larsen, D.Sinclair, F.Videbaek

Abrupt Change between Smooth and Oscillatory Angular Distributions in 16O Induced Transfer Reactions on 26Mg

NUCLEAR REACTIONS 26Mg(16O, 15N), (16O, 14C), E=45, 60 MeV; measured σ(θ).

doi: 10.1016/0370-2693(73)90076-2
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1973TR03      Phys.Lett. 44B, 41 (1973)

N.Trautner, G.Lovhoiden, P.R.Christensen

Elastic and Inelastic Deuteron Scattering from 152Sm and 162Dy

NUCLEAR REACTIONS 152Sm, 162Dy(d, d'), E=12 MeV; measured σ(E, θ). 152Sm, 162Dy levels deduced β.

doi: 10.1016/0370-2693(73)90295-5
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1972FL08      Nucl.Phys. A193, 247 (1972)

E.R.Flynn, P.R.Christensen, O.Nathan, D.G.Fleming

Resonant Proton Scattering from 204Hg (II)

NUCLEAR REACTIONS 204Hg(p, p), 204Hg(p, p'), E=12.5-14.2 MeV, 16.0-18.8 MeV; measured σ(Ep, θ). 205Tl deduced levels, L, J, π, S, T, isobaric analogs. Enriched target.

doi: 10.1016/0375-9474(72)90250-3
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1972VI01      Phys.Rev.Lett. 28, 1072 (1972)

F.Videbaek, I.Chernov, P.R.Christensen, E.E.Gross

Interference between Coulomb and Nuclear Excitation in Inelastic Scattering of 16O Ions

NUCLEAR REACTIONS 58Ni(16O, 16O'), (16O, 16O), E=34-58 MeV; measured σ(E); deduced Coulomb, nuclear excitation interference. 58Ni deduced B(E2).

doi: 10.1103/PhysRevLett.28.1072
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1971LO04      Phys.Lett. 34B, 125 (1971)

G.Lovhoiden, B.Skaali, P.R.Christensen

Wave Functions for the Two-Quadrupole Phonon States in 124Te

NUCLEAR REACTIONS 124Te(p, p), (p, p'), E=13 MeV; measured σ(θ). 124Te levels deduced deformation parameters.

doi: 10.1016/0370-2693(71)90685-X
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1971NI03      Phys.Rev.Lett. 26, 1267 (1971)

R.J.Nickles, V.I.Manko, P.R.Christensen, F.D.Becchetti

Study of One- and Two-Nucleon Transfer Reactions Induced by 16O Ions Incident on the Even Zr Isotopes

NUCLEAR REACTIONS 90,92,94,96Zr(16O, 15N), (16O, 14C), E=60 MeV; measured σ(E(15N), θ(15N)), σ(E(14C), θ(14C)). 91,93,95,97Nb, 92,94,96Mo deduced transition strengths.

doi: 10.1103/PhysRevLett.26.1267
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1970CH14      Nucl.Phys. A149, 302 (1970)

P.R.Christensen, G.Lovhoiden, J.Rasmussen

Elastic and Inelastic Deuteron Scattering from 124Te and 146Nd

NUCLEAR REACTIONS 124Te, 146Nd(d, d), (d, d'), E=12 MeV; measured σ(Ed, θ), σ(Ed', θ). 124Te, 146Nd(α, α'), E=12, 14 MeV measured B(E2), B(E3). 124Te, 146Nd deduced levels. Enriched targets. First-, second-order DWBA calculations.

doi: 10.1016/0375-9474(70)90697-4
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1969CH09      Nucl.Phys. A129, 337 (1969)

P.R.Christensen, A.Berinde, I.Neamu, N.Scintei

Elastic Scattering of 12 MeV Deuterons on Even Rare-Earth Nuclei

NUCLEAR REACTIONS 144,148,152Sm, 154,158,160Gd, 160,162,164Dy, 166,168,170Er, 172Yb, 180Hf, 186W, 208Pb(d, d), Ed=12 MeV; measured σ(θ); deduced optical-model parameters. Enriched targets.

doi: 10.1016/0375-9474(69)90672-1
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0226.


1968CO08      Nucl.Phys. A111, 623(1968)

C.L.Cocke, P.R.Christensen

Neutron Widths in 9Be

NUCLEAR REACTIONS 7Li(3He, pn), E=5-10 MeV; measured σ(Ep, En, θ). 9Be levels deduced neutron decay probabilities. Enriched target.

doi: 10.1016/0375-9474(68)90245-5
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1968KU11      Nucl.Phys. A115, 471(1968)

A.B.Kurepin, P.R.Christensen, N.Trautner

Proton Spin-Flip Probability Measurements for (p, p') on 148Sm and 152Sm

NUCLEAR REACTIONS 148,152Sm(p, p'γ), E = 10-12 MeV; measured σ(Ep', Eγ, θ p'γ); deduced proton spin-flip probability.

doi: 10.1016/0375-9474(68)90020-1
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1968VA31      Nucl.Phys. A115, 265 (1968)

J.G.van der Baan, P.R.Christensen, J.Rasmussen, P.O.Tjom

Elastic Deuteron Scattering on the Even Nd Isotopes

NUCLEAR REACTIONS 142,144,146,148,150Nd(d, d), E=12 MeV; measured σ(θ); deduced optical model parameters. Enriched targets.

doi: 10.1016/0375-9474(68)90003-1
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1834.


1967CH16      Nucl.Phys. A102, 481 (1967)

P.R.Christensen, B.Herskind, R.R.Borchers, L.Westgaard

Neutron Single-Particle States in 143Nd and 145Sm

NUCLEAR REACTIONS 142Nd, 144Sm(d, d), E=12 MeV; measured σ(θ), 143Nd(d, d'), E=12 MeV; measured σ(Ed', θ). 142Nd, 144Sm(d, p), (d, pγ), E=12 MeV; measured σ(Ep, θ), pγ-coin; deduced Q. 143Nd, 145Sm deduced levels, J, π, L(n), S. Enriched targets.

doi: 10.1016/0375-9474(67)90387-9
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF1204.


1966CH18      Phys.Letters 22, 503 (1966)

P.R.Christensen, C.L.Cocke

Non-Existence of the 5.51 MeV and 6.10 MeV Levels in 13C

NUCLEAR STRUCTURE 11B, 13C, 13N; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(66)91244-3
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1966CH20      Nucl.Phys. 89, 656(1966)

P.R.Christensen, C.L.Cocke

Neutron Decay of the 2.43 MeV and 3.03 MeV States in 9Be to 8Be(g.s.)

NUCLEAR REACTIONS 7Li(3He, pn), E = 2.2 MeV; measured σ(Ep, En, θ). 9Be levels deduced neutron decay probabilities. Enriched target.

doi: 10.1016/0029-5582(66)90939-4
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1965CH20      Nucl.Phys. 72, 657 (1965)

P.R.Christensen, F.-C.Yang

0+ States in the N = 82 Nuclei

NUCLEAR REACTIONS 138Ba, 140Ce, 142Nd, 144Sm(p, p'γ), (d, d'γ), E = 12 MeV; measured σ(E(ce)); 142Nd, 144Sm measured σ(Ep'), σ(Ed'). 140Ce, 142Nd, 144Sm deduced levels, J, π. Enriched 140Ce, 142Nd, 144Sm target, natural Ba target.

doi: 10.1016/0029-5582(65)90418-9
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1963CH07      Nucl.Phys. 41, 17 (1963)

P.R.Christensen

Lifetime of the 74.6 keV Level in Np239

NUCLEAR STRUCTURE 239Np, 243Am; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(63)90473-5
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1963CH09      Phys.Letters 4, 318 (1963)

P.R.Christensen, O.B.Nielsen, H.Nordby

The β-Branch from Tl207 to the p3/2- Level in Pb207

NUCLEAR STRUCTURE 207Tl; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(63)90492-X
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1963VA05      Nucl.Phys. 41, 482 (1963)

S.E.Vandenbosch, C.V.K.Baba, P.R.Christensen, O.B.Nielsen, H.Nordby

The Decay Scheme of Pb211

NUCLEAR STRUCTURE 211Pb, 207Tl; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(63)90525-X
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1962CH19      Nuclear Phys. 37, 482 (1962)

P.R.Christensen

Lifetime of the First 2+ Level in Cm244

NUCLEAR STRUCTURE 244Am; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(62)90281-X
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1962VA16      Conf.Low Energy Nuclear Phys.Harwell, AERE-R-4131, 23, 7B.1 (September 1962)

S.E.Vandenbosch, C.V.K.Baba, P.R.Christensen, O.B.Nielsen, H.Nordby

NUCLEAR STRUCTURE 211Pb; measured not abstracted; deduced nuclear properties.


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