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2014BR12      Nucl.Data Sheets 120, 115 (2014)

B.A.Brown, W.D.M.Rae

The Shell-Model Code NuShellX@MSU

NUCLEAR STRUCTURE 53Fe, 42Si, 62Ni; calculated level structure, J, π. Shell model, comparison with ENSDF data.

doi: 10.1016/j.nds.2014.07.022
Citations: PlumX Metrics


2012SC18      Eur.Phys.J. A 48, 191 (2012)

S.Schwertel, P.Maierbeck, R.Krucken, R.Gernhauser, T.Kroll, H.Alvarez-Pol, F.Aksouh, T.Aumann, K.Behr, E.A.Benjamim, J.Benlliure, V.Bildstein, M.Bohmer, K.Boretzky, M.J.G.Borge, A.Brunle, A.Burger, M.Caamano, E.Casarejos, A.Chatillon, L.V.Chulkov, D.Cortina-Gil, J.Enders, K.Eppinger, T.Faestermann, J.Friese, L.Fabbietti, M.Gascon, H.Geissel, J.Gerl, M.Gorska, P.G.Hansen, B.Jonson, R.Kanungo, O.Kiselev, I.Kojouharov, A.Klimkiewicz, T.Kurtukian, N.Kurz, K.Larsson, T.Le Bleis, K.Mahata, L.Maier, T.Nilsson, C.Nociforo, G.Nyman, C.Pascual-Izarra, A.Perea, D.Perez, A.Prochazka, C.Rodriguez-Tajes, D.Rossi, H.Schaffner, G.Schrieder, H.Simon, B.Sitar, M.Stanoiu, K.Summerer, O.Tengblad, H.Weick, S.Winkler, B.A.Brown, T.Otsuka, J.A.Tostevin, W.D.M.Rae

One-neutron knockout from 51-55Sc

NUCLEAR REACTIONS 9Be(55Sc, 54Sc), (54Sc, 53Sc), (53Sc, 52Sc), (52Sc, 51Sc), (51Sc, 50Sc), E≈420 MeV/nucleon; measured relativistic reaction products, Eγ, Iγ; deduced longitudinal momentum distribution, σ; calculated σ.

doi: 10.1140/epja/i2012-12191-5
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2348.


2009HI08      Phys.Rev. C 80, 014313 (2009)

G.W.Hitt, R.G.T.Zegers, Sam M.Austin, D.Bazin, A.Gade, D.Galaviz, C.J.Guess, M.Horoi, M.E.Howard, W.D.M.Rae, Y.Shimbara, E.E.Smith, C.Tur

Gamow-Teller transitions to 64Cu measured with the 64Zn(t, 3He) reaction

NUCLEAR REACTIONS 64Zn(t, 3He), E=115 MeV/nucleon; measured particle spectra, σ(θ) and Gamow-Teller strength distributions; deduced electron capture rate on 64Zn as a function of stellar temperature. Comparison with shell model calculations and experimental data from 64Zn(d, 2He) reaction.

doi: 10.1103/PhysRevC.80.014313
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1721. Data from this article have been entered in the XUNDL database. For more information, click here.


2009MA16      Phys.Lett. B 675, 22 (2009)

P.Maierbeck, R.Gernhauser, R.Krucken, T.Kroll, H.Alvarez-Pol, F.Aksouh, T.Aumann, K.Behr, E.A.Benjamim, J.Benlliure, V.Bildstein, M.Bohmer, K.Boretzky, M.J.G.Borge, A.Brunle, A.Burger, M.Caamano, E.Casarejos, A.Chatillon, L.V.Chulkov, D.Cortina-Gil, J.Enders, K.Eppinger, T.Faestermann, J.Friese, L.Fabbietti, M.Gascon, H.Geissel, J.Gerl, M.Gorska, P.G.Hansen, B.Jonson, R.Kanungo, O.Kiselev, I.Kojouharov, A.Klimkiewicz, T.Kurtukian, N.Kurz, K.Larsson, T.Le Bleis, K.Mahata, L.Maier, T.Nilsson, C.Nociforo, G.Nyman, C.Pascual-Izarra, A.Perea, D.Perez, A.Prochazka, C.Rodriguez-Tajes, D.Rossi, H.Schaffner, G.Schrieder, S.Schwertel, H.Simon, B.Sitar, M.Stanoiu, K.Summerer, O.Tengblad, H.Weick, S.Winkler, B.A.Brown, T.Otsuka, J.Tostevin, W.D.M.Rae

Structure of 55Ti from relativistic one-neutron knockout

NUCLEAR REACTIONS 9Be(48Ca, n47Ca), (56Ti, n55Ti), E=450 MeV/nucleon; measured σ, Eγ, Iγ, (recoil)γ-coin after Doppler correction, momentum distributions. 47Ca, 55Ti; deduced J, π, levels. Comparison with shell-model calculations. FRS with secondary beam and MINIBALL array.

doi: 10.1016/j.physletb.2009.03.049
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0614. Data from this article have been entered in the XUNDL database. For more information, click here.


2009ST28      Eur.Phys.J. A 42, 407 (2009)

I.Stefanescu, W.B.Walters, P.F.Mantica, B.A.Brown, A.D.Davies, A.Estrade, P.T.Hosmer, N.Hoteling, S.N.Liddick, W.D.M.Rae, T.J.Mertzimekis, F.Montes, A.C.Morton, W.F.Mueller, M.Ouellette, E.Pellegrini, P.Santi, D.Seweryniak, H.Schatz, J.Shergur, A.Stolz, J.R.Stone, B.E.Tomlin

Spectroscopy of exotic 121, 123, 125Ag produced in fragmentation reactions

NUCLEAR REACTIONS 9Be(136Xe, X)121Pd/123Ag/125Ag, E=120 MeV/nucleon; measured Eγ, Iγ, γγ-, (fragment)γ-coin. 121,123,125Ag; deduced levels, J, π, T1/2. Comparison with shell model and systematics.

RADIOACTIVITY 121Pd(β-) [from 9Be(136Xe, X), E=120 MeV/nucleon]; measured Eγ, Iγ, γγ-, (fragment)γ-coin. 121Ag; deduced levels, J, π. Comparison with shell model and systematics.

doi: 10.1140/epja/i2008-10754-7
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


2008RI04      Phys.Rev. C 78, 011303 (2008)

L.A.Riley, P.Adrich, T.R.Baugher, D.Bazin, B.A.Brown, J.M.Cook, P.D.Cottle, C.Aa.Diget, A.Gade, D.A.Garland, T.Glasmacher, K.E.Hosier, K.W.Kemper, T.Otsuka, W.D.M.Rae, A.Ratkiewicz, K.P.Siwek, J.A.Tostevin, Y.Utsuno, D.Weisshaar

d5/2 proton hole strength in neutron-rich 43P: Shell structure and nuclear shapes near N = 28

NUCLEAR REACTIONS 9Be(44S, p43P), E=91.7 MeV/nucleon; measured Eγ, Iγ, γγ-, (particle)γ-coin, partial σ, momentum distributions. 43P; deduced levels, J, π. Comparison with shell-model calculations.

doi: 10.1103/PhysRevC.78.011303
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


2007FR17      Phys.Rev. C 76, 034320 (2007)

M.Freer, I.Boztosun, C.A.Bremner, S.P.G.Chappell, R.L.Cowin, G.K.Dillon, B.R.Fulton, B.J.Greenhalgh, T.Munoz-Britton, M.P.Nicoli, W.D.M.Rae, S.M.Singer, N.Sparks, D.L.Watson, D.C.Weisser

Reexamination of the excited states of 12C

NUCLEAR REACTIONS 12C(12C, 3α), E=82-106 MeV; analyzed energy and angular distributions data. 8Be deduced levels.

doi: 10.1103/PhysRevC.76.034320
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


2005FR14      Phys.Rev. C 71, 047305 (2005)

M.Freer, I.Boztosun, C.A.Bremner, S.P.G.Chappell, R.L.Cowin, G.K.Dillon, B.R.Fulton, B.J.Greenhalgh, M.P.Nicoli, W.D.M.Rae, S.M.Singer, D.L.Watson, D.C.Weisser

8Be + 12C(0+2) decay of excited states in 20Ne

NUCLEAR REACTIONS 12C(12C, 8Be12C), E=82-120 MeV; measured particle spectra, angular distributions. 20Ne deduced possible resonance states energies, J, π.

doi: 10.1103/PhysRevC.71.047305
Citations: PlumX Metrics


2004FR34      Phys.Rev. C 70, 064311 (2004)

M.Freer, M.P.Nicoli, S.M.Singer, C.A.Bremner, S.P.G.Chappell, W.D.M.Rae, I.Boztosun, B.R.Fulton, D.L.Watson, B.J.Greenhalgh, G.K.Dillon, R.L.Cowin, D.C.Weisser

8Be+8Be decay of excited states in 16O

NUCLEAR REACTIONS 12C(12C, 28Be), E=82-120 MeV; measured excitation energy spectra, angular correlations. 16O deduced levels, J, π. Comparison with model predictions.

doi: 10.1103/PhysRevC.70.064311
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0277.


2004GR12      Phys.Rev. C 69, 054316 (2004)

B.J.Greenhalgh, G.K.Dillon, B.R.Fulton, D.L.Watson, R.L.Cowin, M.Freer, S.M.Singer, S.P.G.Chappell, C.A.Bremner, W.D.M.Rae, D.C.Weisser

Structures in the excitation functions of high lying inelastic channels of the 16O + 16O system in the region Ec.m. = 26 to 47 MeV

NUCLEAR REACTIONS 16O(16O, α12C), E=52-94 MeV; measured particle spectra, angular correlations, σ(E, θ), excitation function; deduced resonance features.

doi: 10.1103/PhysRevC.69.054316
Citations: PlumX Metrics


2002BO03      Phys.Rev. C65, 024603 (2002)

I.Boztosun, W.D.M.Rae

Global Potential Analysis of the 16O + 28Si Reaction using a New Type of Coupling Potential

NUCLEAR REACTIONS 28Si(16O, 16O), (16O, 16O'), E=29.0-142.5 MeV; calculated σ(θ). New coupling potential, comparison with data.

doi: 10.1103/PhysRevC.65.024603
Citations: PlumX Metrics


2002BR43      Phys.Rev. C66, 034605 (2002)

C.A.Bremner, S.P.G.Chappell, W.D.M.Rae, I.Boztosun, M.Freer, M.P.Nicoli, S.M.Singer, B.R.Fulton, D.L.Watson, B.J.Greenhalgh, G.K.Dillon, R.L.Cowin

Excitation Function Measurements for 12C + 12C Inelastic Scattering Channels

NUCLEAR REACTIONS 12C(12C, 12C'), E(cm)=40-59 MeV; measured excitation energy spectra, σ(E); deduced excitation functions, resonance features.

doi: 10.1103/PhysRevC.66.034605
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0436.


2001BO18      Phys.Rev. C63, 054607 (2001)

I.Boztosun, W.D.M.Rae

Analysis of the 12C + 12C Reaction using a New Type of Coupling Potential

NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=32.0-126.7 MeV; calculated σ(θ), excitation functions. Coupled-channels approach, new potential, comparisons with data.

doi: 10.1103/PhysRevC.63.054607
Citations: PlumX Metrics


2001BO41      Phys.Lett. 518B, 229 (2001)

I.Boztosun, W.D.M.Rae

A New Coupling Potential for the Analysis of Deformed Light Heavy-Ion Reactions

NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=20.0-126.7 MeV; 28Si(16O, 16O), (16O, 16O'), E=29.0-142.5 MeV; 24Mg(12C, 12C), (12C, 12C'), E=16.0-24.0 MeV; calculated σ(θ). New coupling potential, comparisons with data.

doi: 10.1016/S0370-2693(01)01063-2
Citations: PlumX Metrics


2001BO46      Phys.Rev. C64, 054607 (2001); Erratum Phys.Rev. C66, 049904 (2002)

I.Boztosun, W.D.M.Rae

Analysis of the 12C + 24Mg Reaction using a New Coupling Potential

NUCLEAR REACTIONS 24Mg(12C, 12C), (12C, 12C'), E=16-24 MeV; calculated σ(θ). Coupled-channels approach, second-derivative coupling potential, comparison with data.

doi: 10.1103/PhysRevC.64.054607
Citations: PlumX Metrics


2000SI36      Phys.Rev. C62, 054609 (2000)

S.M.Singer, W.N.Catford, G.J.Gyapong, M.Shawcross, N.M.Clarke, N.Curtis, M.Freer, B.R.Fulton, S.J.Hall, R.A.Le Marechal, M.J.Leddy, J.S.Pople, G.Tungate, R.P.Ward, W.D.M.Rae, P.M.Simmons, S.P.G.Chappell, S.P.Fox, C.D.Jones, P.Lee, D.L.Watson

Mechanism of the 12C(24Mg, 12C12C)12C Breakup Reaction: Direct vs compound

NUCLEAR REACTIONS 24Mg(12C, 212C), E=85 MeV; measured particle spectra, angular distributions, coincidences, symmetric breakup yield; deduced forward-backward asymmetry, reaction mechanism features. Coupled channels DWBA calculations, comparison with reversed kinematics.

doi: 10.1103/PhysRevC.62.054609
Citations: PlumX Metrics


1999FO16      Phys.Rev. C60, 064620 (1999)

S.P.Fox, D.L.Watson, C.D.Jones, S.P.Chappell, P.Lee, W.D.M.Rae, M.Freer, S.J.A.Hall, G.Kelly, R.Le Marechal, R.P.Ward, W.N.Catford, G.J.Gyapong, S.Singer

Structures in the 12C(16O, 12C(02+) → 3α)16O Reaction in the Region Ec.m. = 15 to 34 MeV

NUCLEAR REACTIONS 12C(16O, 12C), E(cm)=15-34 MeV; measured Eα, Iα(θ), αα-coin following carbon breakup; deduced excitation functions. 28Si deduced possible resonance structures energy and angular momenta. Comparisons with model predictions.

doi: 10.1103/PhysRevC.60.064620
Citations: PlumX Metrics


1999HO07      Phys.Rev. C59, 1456 (1999)

S.J.Hoad, N.M.Clarke, M.Freer, B.R.Fulton, P.Fry, W.D.M.Rae, A.H.Wuosmaa

Excitation Function Measurements for the 12C(20Ne, 12C[02+])20Ne Reaction

NUCLEAR REACTIONS 12C(20Ne, 12C), E(cm)=22.5-31.9 MeV; measured excitation functions, σ(θ); deduced no highly deformed cluster structure. Coupled channels calculations.

doi: 10.1103/PhysRevC.59.1456
Citations: PlumX Metrics


1998CH48      Phys.Lett. 444B, 260 (1998)

S.P.G.Chappell, W.D.M.Rae, C.A.Bremner, G.K.Dillon, D.L.Watson, B.Greenhalgh, R.L.Cowin, M.Freer, S.M.Singer

High Spin Resonances in 12C + 12C Scattering

NUCLEAR REACTIONS 12C(12C, 12C'), E(cm)=31-45 MeV; measured excitation function, particle angular correlations following breakup. 24Mg deduced high-spin resonances. α-cluster model calculations.

doi: 10.1016/S0370-2693(98)01415-4
Citations: PlumX Metrics


1998HO03      J.Phys.(London) G24, 167 (1998)

S.J.Hoad, N.M.Clarke, N.Curtis, M.Freer, B.R.Fulton, S.J.Hall, M.J.Leddy, A.St.J.Murphy, J.S.Pople, G.Tungate, R.P.Ward, S.P.G.Chappell, S.P.Fox, C.D.Jones, D.L.Watson, W.D.M.Rae, P.M.Simmons, W.N.Catford, G.J.Gyapong, S.M.Singer

Can Break-Up Reactions be Used to Probe High-Lying Inelastic Channels in 12C + 12C Scattering ( Question )

NUCLEAR REACTIONS C(24Mg, 212C), E=170 MeV; measured (12C)(12C(0+2))-coin, total energy.

doi: 10.1088/0954-3899/24/1/020
Citations: PlumX Metrics


1998MU16      Phys.Rev. C58, 1569 (1998)

J.T.Murgatroyd, J.S.Pople, N.M.Clarke, B.R.Fulton, M.J.Leddy, W.N.Catford, S.P.Fox, G.J.Gyapong, C.D.Jones, D.L.Watson, W.D.M.Rae, Y.Chan, R.G.Stokstad, S.J.Bennett

16O + 8Be Breakup of 24Mg Via the 12C(20Ne, 16O8Be)8Be and 12C(24Mg, 16O8Be)12C Reactions

NUCLEAR REACTIONS 12C(20Ne, 8Be16O), E=160 MeV; 12C(24Mg, 8Be16O), E=170 MeV; measured (Be)(O)-coin, angular correlations, excitation energy spectra. 24Mg deduced levels E, J. Comparison with 12C + 12C breakup channel.

doi: 10.1103/PhysRevC.58.1569
Citations: PlumX Metrics


1997CH51      Nucl.Instrum.Methods Phys.Res. A396, 383 (1997)

S.P.G.Chappell, W.D.M.Rae, P.M.Simmons

Calibration of Position Sensitive Detectors with Low-Energy Elastic Scattering

doi: 10.1016/S0168-9002(97)00808-5
Citations: PlumX Metrics


1997GY02      Nucl.Phys. A620, 55 (1997)

G.J.Gyapong, N.Curtis, W.N.Catford, S.M.Singer, W.D.M.Rae, M.Freer, S.J.Hall, G.R.Kelly, R.A.Le Marechal, R.P.Ward, S.P.G.Chappell, S.P.Fox, C.D.Jones, P.R.Lee, D.L.Watson

Two-Dimensional Alpha Cluster Structures in 28Si

NUCLEAR REACTIONS 12C(16O, 212C), E(cm)=28.3-36.8 MeV; measured (12C)(12C)-coin; deduced σ(E). 28Si deduced resonance angular momenta, cluster state characteristics.

doi: 10.1016/S0375-9474(97)00152-8
Citations: PlumX Metrics


1997RA38      Nuovo Cim. 110A, 1001 (1997)

W.D.M.Rae, S.P.G.Chappell, P.E.Fry

The Role of Alpha Clustering in 12C + 12C Scattering

NUCLEAR REACTIONS 12C(12C, X), E(cm)=5-35 MeV; calculated resonances. α-cluster model.

doi: 10.1007/BF03035937
Citations: PlumX Metrics


1997ZH01      Nucl.Phys. A613, 14 (1997)

J.Zhang, A.C.Merchant, W.D.M.Rae

Study of α-Cluster Structure using Angular Momentum Projection: Form factors and B(E2) values

NUCLEAR STRUCTURE 24Mg, 28Si, 32S, 20Ne; calculated elastic, inelastic α-particle form factors, E2 transitions Γγ, rms charge radii. 24Mg, 28Si; calculated B(λ). 40Ca calculated rms charge radius. 36Ar; 48Cr; calculated B(λ). Bloch-Brink α-cluster model.

doi: 10.1016/S0375-9474(96)00421-6
Citations: PlumX Metrics


1996CH14      Phys.Rev. C53, 2879 (1996)

S.P.G.Chappell, W.D.M.Rae

Angular Correlations for α-Particle Decay in the Reaction 12C[12C, 12C(3-1) → 8Be(0+1) + α]12C(*) at E(c.m.) = 32.5 MeV

NUCLEAR REACTIONS 12C(12C, 12C'), E(cm)=32.5 MeV; measured (particle)(particle)(θ), sequential mutual, breakup. Semi-classical model.

doi: 10.1103/PhysRevC.53.2879
Citations: PlumX Metrics


1996CU02      Phys.Rev. C53, 1804 (1996)

N.Curtis, A.St.J.Murphy, N.M.Clarke, M.Freer, B.R.Fulton, S.J.Hall, M.J.Leddy, J.S.Pople, G.Tungate, R.P.Ward, W.N.Catford, G.J.Gyapong, S.M.Singer, S.P.G.Chappell, S.P.Fox, C.D.Jones, D.L.Watson, W.D.M.Rae, P.M.Simmons, P.H.Regan

Evidence for a Highly Deformed Band in 16O + 16O Breakup of 32S

NUCLEAR REACTIONS 12C(24Mg, 216O), E=170 MeV; measured (16O)(16O)(θ). 32S deduced levels, possible J, π, rotational parameter, band structure. Compared to DWBA.

doi: 10.1103/PhysRevC.53.1804
Citations: PlumX Metrics


1996ME02      Phys.Rev. C53, 775 (1996)

A.C.Merchant, W.D.M.Rae

Coupled-Channels Model for Superdeformed Prolate Nuclei: α-Chain states in 16O

NUCLEAR STRUCTURE 16O; calculated 4α-chain states, fission, escape widths. Comparison with 12C(16O, 4α) reaction data, schematic coupled-channels model, 8Be-8Be cluster states.

doi: 10.1103/PhysRevC.53.775
Citations: PlumX Metrics


1996MU03      Phys.Rev. C53, 1963 (1996)

A.St.J.Murphy, R.A.Le Marechal, S.J.Bennett, N.M.Clarke, N.Curtis, M.Freer, B.R.Fulton, S.J.Hall, M.J.Leddy, J.T.Murgatroyd, J.S.Pople, G.Tungate, R.P.Ward, W.D.M.Rae, P.M.Simmons, W.N.Catford, G.J.Gyapong, S.M.Singer, S.P.G.Chappell, S.P.Fox, C.D.Jones, P.Lee, D.L.Watson

Search for 16O + 16O + 16O Structure in 48Cr

NUCLEAR REACTIONS 12C, 24Mg(24Mg, 216O), E=150, 170 MeV; measured Eγ, Iγ, σ(θ1, θ2).

doi: 10.1103/PhysRevC.53.1963
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1996RA08      J.Phys.(London) G22, L13 (1996)

W.D.M.Rae, P.E.Fry, A.C.Merchant

Evidence for the 3-Fold α-Cluster Symmetry of 12C

NUCLEAR REACTIONS 12C(12C, 12C'), E(cm) ≈ 33 MeV; analyzed data. 12C deduced 3-fold α-cluster evidence. Oblate nuclei, coupled-channels formalism.

doi: 10.1088/0954-3899/22/2/002
Citations: PlumX Metrics


1996ZH01      Phys.Rev. C53, 515 (1996)

J.Zhang, W.D.M.Rae, A.C.Merchant

α-Cluster Structure of the Yrast Bands of 44Ti

NUCLEAR STRUCTURE 44Ti; calculated intrabrand B(λ). Bloch-Brink microscopic α-cluster model.

doi: 10.1103/PhysRevC.53.515
Citations: PlumX Metrics


1995CH07      Phys.Rev. C51, 695 (1995)

S.P.G.Chappell, D.L.Watson, S.P.Fox, C.D.Jones, W.D.M.Rae, P.M.Simmons, M.Freer, B.R.Fulton, N.M.Clarke, N.Curtis, M.J.Leddy, J.S.Pople, S.J.Hall, R.P.Ward, G.Tungate, W.N.Catford, G.J.Gyapong, S.M.Singer, P.H.Regan

12C + 12C ' 6α-Chain State ' Resonance

NUCLEAR REACTIONS 12C(12C, 12C'), E(cm)=25-40 MeV; measured spectra, σ(θ). 24Mg deduced resonance features.

doi: 10.1103/PhysRevC.51.695
Citations: PlumX Metrics


1995CU01      Phys.Rev. C51, 1554 (1995)

N.Curtis, N.M.Clarke, B.R.Fulton, S.J.Hall, M.J.Leddy, A.St.J.Murphy, J.S.Pople, R.P.Ward, W.N.Catford, G.J.Gyapong, S.M.Singer, S.P.G.Chappell, S.P.Fox, C.D.Jones, D.L.Watson, W.D.M.Rae, P.M.Simmons, and the Charissa Collaboration

Association of the 12C + 12C Breakup States in 24Mg with the Quasimolecular Resonances

NUCLEAR REACTIONS 12C(24Mg, 212C), E=170 MeV; measured (12C)(12C)-coin spectra. 24Mg deduced resonances, J, π, Γ upper limit.

doi: 10.1103/PhysRevC.51.1554
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1995FR05      Phys.Rev. C51, 1682 (1995)

M.Freer, N.M.Clarke, N.Curtis, B.R.Fulton, S.J.Hall, M.J.Leddy, J.S.Pople, G.Tungate, R.P.Ward, P.M.Simmons, W.D.M.Rae, S.P.G.Chappell, S.P.Fox, C.D.Jones, D.L.Watson, G.J.Gyapong, S.M.Singer, W.N.Catford, P.H.Regan

8Be and α Decay of 16O

NUCLEAR REACTIONS 12C(16O, 4α), E=99 MeV; measured Q-value spectra, 16O excitation spectra leading to breakup, (12C)(α)(θ). 16O deduced resonances, decay channels, partial Γ, J.

doi: 10.1103/PhysRevC.51.1682
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1995FR12      Phys.Rev. C51, 3174 (1995)

M.Freer, N.M.Clarke, R.A.Le Marechal, G.Tungate, R.P.Ward, W.D.M.Rae

Final-State Interactions in the 12C(16O, 12C12C)α and 16O(16O, 12C16O)α Reactions

NUCLEAR REACTIONS 12C(16O, 212C), 16O(16O, 12C16O), E=80.5, 99 MeV; measured (fragment)(fragment)(θ). 24Mg, 28Si deduced breakup states J.

doi: 10.1103/PhysRevC.51.3174
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1995JA06      Phys.Rev. C51, 2606 (1995)

N.S.Jarvis, D.L.Watson, G.J.Gyapong, C.D.Jones, S.J.Bennett, M.Freer, B.R.Fulton, O.Karban, J.T.Murgatroyd, G.Tungate, W.D.M.Rae, A.E.Smith

Breakup Studies with 23Na

NUCLEAR REACTIONS 12C(23Na, 11B12C), E=176 MeV; 12C(23Na, 212C), E=156 MeV; measured fragment E(total), spectra. 23Na, 24Mg deduced breakup state energies, width upper limits, fragmentation characteristics.

doi: 10.1103/PhysRevC.51.2606
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1995LE22      Nucl.Phys. A589, 363 (1995)

M.J.Leddy, S.J.Bennett, N.M.Clarke, M.Freer, B.R.Fulton, J.T.Murgatroyd, G.J.Gyapong, C.D.Jones, D.L.Watson, W.D.M.Rae, A.E.Smith, W.N.Catford

Comparison of Resonances Observed in the 12C(24Mg, 12C12C)12C and 12C(20Ne, 12C12C)8Be Reactions

NUCLEAR REACTIONS 12C(24Mg, 212C), E=170 MeV; measured (fragment)(fragment)-coin. 24Mg deduced excitation energies, J.

doi: 10.1016/0375-9474(95)00053-4
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1995MU03      Phys.Rev. C51, 2230 (1995)

J.T.Murgatroyd, S.J.Bennett, B.R.Fulton, J.S.Pople, N.S.Jarvis, D.L.Watson, W.D.M.Rae, Y.Chan, D.DiGregorio, J.Scarpaci, J.Suro Perez, R.G.Stokstad

Evidence for 16O + 12C Cluster Structure in 28Si

NUCLEAR REACTIONS 12C(20Ne, 12C16O), E=160 MeV; measured (12C)(16O)-coin total energy spectra. 28Si levels deduced 12C + 16O cluster structure, shape features.

doi: 10.1103/PhysRevC.51.2230
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1995RA21      Phys.Rev.Lett. 74, 4145 (1995)

W.D.M.Rae, A.C.Merchant

Schematic Model of a 6α Chain State

NUCLEAR STRUCTURE 24Mg; calculated resonances, fission, escape widths. Approximate coupled channels model of a 6-α chain state.

doi: 10.1103/PhysRevLett.74.4145
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1995SI13      Phys.Rev. C51, 3500 (1995)

P.M.Simmons, W.D.M.Rae, S.P.G.Chappell, S.P.Fox, C.D.Jones, D.L.Watson, M.Freer, B.R.Fulton, N.M.Clarke, N.Curtis, M.J.Leddy, J.S.Pople, S.J.Hall, R.P.Ward, G.Tungate, W.N.Catford, G.J.Gyapong, S.M.Singer, P.H.Regan

Search for a 7-α Chain State

NUCLEAR REACTIONS 12C(16O, X), E(cm)=37.7-51.4 MeV; measured σ(E) for (12C)(12C)(α), (12C)(8Be)(8Be) production. 28Si deduced no 7α-chain state.

doi: 10.1103/PhysRevC.51.3500
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1995TI06      Phys.Rev. C52, 1315 (1995)

M.A.Tiede, K.W.Kemper, N.R.Fletcher, D.Robson, D.D.Caussyn, S.J.Bennett, J.D.Brown, W.N.Catford, C.D.Jones, D.L.Watson, W.D.M.Rae

Measurement of Low-Lying States in 9B

NUCLEAR REACTIONS 6Li(6Li, t), E=56 MeV; measured 8Be+p relative energy spectra. 9B deduced levels, parameters. Line shape analysis.

doi: 10.1103/PhysRevC.52.1315
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1994CU05      Nucl.Instrum.Methods Phys.Res. A351, 359 (1994)

N.Curtis, A.St.J.Murphy, M.J.Leddy, J.S.Pople, N.M.Clarke, M.Freer, B.R.Fulton, S.J.Hall, G.Tungate, R.P.Ward, S.M.Singer, W.N.Catford, G.J.Gyapong, R.A.Cunningham, J.S.Lilley, S.P.Chappell, S.P.Fox, C.D.Jones, D.L.Watson, P.M.Simmons, R.A.Hunt, A.C.Merchant, A.E.Smith, W.D.M.Rae, J.Zhang, and the Charissa Collaboration

The Construction and Operation of a Hybrid Gas-Silicon Detector for Studies of Cluster Breakup Reactions

NUCLEAR REACTIONS 12C(24Mg, 212C), E=170 MeV; measured (12C)(12C)-coin spectra following projectile breakup. 197Au(12C, 12C), E=84 MeV; 197Au(24Mg, 24Mg), E=170 MeV; measured spectra. Hybrid gas-silicon detector.

doi: 10.1016/0168-9002(94)91364-1
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1994FU01      J.Phys.(London) G20, 151 (1994)

B.R.Fulton, S.J.Bennett, J.T.Murgatroyd, N.S.Jarvis, D.L.Watson, W.D.M.Rae, Y.Chan, D.DiGregorio, J.Scarpaci, J.Suro Perez, R.G.Stokstad

Resonances in 24Mg Revealed in the 12C(20Ne, 12C12C)8Be Reaction

NUCLEAR REACTIONS 12C(20Ne, 212C), E=160 MeV; measured coincident 12C nuclei total energy spectra. 24Mg deduced excited state population, breakup mechanism.

doi: 10.1088/0954-3899/20/1/015
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1994GY01      Nucl.Phys. A579, 207 (1994)

G.J.Gyapong, D.L.Watson, W.N.Catford, N.M.Clarke, S.J.Bennett, M.Freer, B.R.Fulton, C.D.Jones, M.Leddy, J.T.Murgatroyd, W.D.M.Rae, P.Simmons

Reaction Mechanism for the Symmetric Breakup of 24Mg following an Interaction with 12C

NUCLEAR REACTIONS 12C(24Mg, 212C), E(cm)=43.3-60 MeV; measured symmetric breakup yield; deduced reaction mechanism. 24Mg deduced cluster states characteristics.

doi: 10.1016/0375-9474(94)90802-8
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1994ME06      Nucl.Phys. A571, 43 (1994)

A.C.Merchant, W.D.M.Rae

Calculations of Particle Decay Widths of Hyper-Deformed Nuclei using Prolate Spheroidal Coordinates

NUCLEAR STRUCTURE 24Mg, 48Cr; calculated α-decay widths, hyperdeformed nuclei. Prolate spheroidal coordinates, coupled-channels calculations.

doi: 10.1016/0375-9474(94)90340-9
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1994ME18      Z.Phys. A349, 243 (1994)

A.C.Merchant, W.D.M.Rae

Alpha Chain States in 4N-Nuclei

NUCLEAR REACTIONS 12C(12C, 12C'), E(cm)=33, 35 MeV; compiled, reviewed data, analyses. 24Mg deduced 6-α chain state features.

NUCLEAR STRUCTURE 16O, 20Ne, 24Mg, 28Si; calculated α-emission widths from α-chain states. Semi-classical, quantum mechanical approaches.

doi: 10.1007/BF01288968
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1994PO19      Z.Phys. A349, 349 (1994)

J.S.Pople, N.M.Clarke, B.R.Fulton, M.J.Leddy, J.T.Murgatroyd, Y.Chan, R.G.Stokstad, W.D.M.Rae, W.N.Catford, S.P.Fox, G.J.Gyapong, D.L.Watson, S.J.Bennett, and the Charissa Collaboration

The Breakup of 24Mg into 16O and 8Be

NUCLEAR REACTIONS 12C(24Mg, 8Be16O), E=170 MeV; 12C(20Ne, 8Be16O), E=160 MeV; measured breakup spectra; deduced reaction mechanism. 24Mg deduced breakup level configuration, shape features.


1994RA03      Phys.Lett. 321B, 1 (1994)

W.D.M.Rae, A.C.Merchant, J.Zhang

Geometry and Collectivity in the Bloch-Brink α-Cluster Model

NUCLEAR STRUCTURE 24Mg, 32S, 12C, 20Ne, 28Si, 16O; calculated energies. Constrained, unconstrained Block-Brink α-cluster model.

doi: 10.1016/0370-2693(94)90318-2
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1994RA04      Nucl.Phys. A568, 271 (1994)

W.D.M.Rae, S.C.Allcock, J.Zhang

Spin Assignments for States in 20Ne via the 12C(16O, 20Ne(*))8Be Transfer Reaction

NUCLEAR REACTIONS 12C(16O, 20Ne), E=150 MeV; measured σ(θα, φα) following 20Ne decay. 20Ne levels deduced J, π. Strong absorption model analyses.

doi: 10.1016/0375-9474(94)90202-X
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1994RA05      Nucl.Phys. A568, 287 (1994)

W.D.M.Rae, S.C.Allcock, J.Zhang

Spin Assignments for States in 16O using the 12C(12C, 16O(*))8Be Transfer Reaction

NUCLEAR REACTIONS 12C(12C, 16O), E=120 MeV; measured σ(θα, φα). 16O levels deduced J, π. Strong absorption model analyses.

doi: 10.1016/0375-9474(94)90203-8
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1994RA15      Nucl.Phys. A575, 175 (1994)

W.D.M.Rae, P.R.Keeling

Spin and Structure of 12C - 12C Resonances I

NUCLEAR REACTIONS 12C(12C, 2α), E=38-64 MeV; measured σ(θ, psi). 24Mg levels deduced J, π.

doi: 10.1016/0375-9474(94)90144-9
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1994RA16      Nucl.Phys. A575, 207 (1994)

W.D.M.Rae, P.R.Keeling

Spin and Structure of 12C - 12C Resonances II

NUCLEAR REACTIONS 12C(12C, 8Be), E=44-55 MeV; 12C(12C, α8Be), E=50 MeV; measured σ(θ), σ(θ, psi). 24Mg levels deduced J, π.

doi: 10.1016/0375-9474(94)90145-7
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1994ZH01      Phys.Rev. C49, 562 (1994)

J.Zhang, A.C.Merchant, W.D.M.Rae

Superdeformed and Hyperdeformed States in 56Ni

NUCLEAR STRUCTURE 56Ni; calculated superdeformed, hyperdeformed states features. Alpha-cluster model.

doi: 10.1103/PhysRevC.49.562
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1994ZH16      Nucl.Phys. A575, 61 (1994)

J.Zhang, W.D.M.Rae, A.C.Merchant

Systematics of Some 3-Dimensional α-Cluster Configurations in 4N Nuclei from 16O to 44Ti

NUCLEAR STRUCTURE 16O, 20Ne, 24Mg, 28Si, 32S, 36Ar, 40Ca, 44Ti; calculated α-cluster states characteristics systematics. Bloch-Brink α-cluster model.

doi: 10.1016/0375-9474(94)90137-6
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1993BE56      Nucl.Instrum.Methods Phys.Res. A332, 476 (1993)

S.J.Bennett, N.M.Clarke, M.Freer, B.R.Fulton, S.J.Hall, O.Karban, J.T.Murgatroyd, G.Tungate, G.J.Gyapong, N.S.Jarvis, D.L.Watson, W.D.M.Rae, A.E.Smith, J.S.Lilley, P.J.Woods, R.D.Page, and the Charissa Collaboration

Application of Inverse Kinematics to 1H + 23Na → 12C + 12C using a Thick Target

NUCLEAR REACTIONS 1H(23Na, 12C), E=180 MeV; measured 12C-spectra, σ(θ) vs 24Mg excitation. Kinematically complete experiment.

doi: 10.1016/0168-9002(93)90303-Y
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1993ME04      J.Phys.(London) G19, L89 (1993)

A.C.Merchant, W.D.M.Rae

Energy Dependence of the Angular Distributions of the New Resonance Seen in 12C(12C, 12C(0+2))12C(0+2)

NUCLEAR REACTIONS 12C(12C, 12C'), E(cm) ≈ 32-36 MeV; analyzed σ(θ). 24Mg deduced resonance features.

doi: 10.1088/0954-3899/19/5/002
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1993ZH21      Phys.Rev. C48, 2117 (1993)

J.Zhang, A.C.Merchant, W.D.M.Rae

Comment on ' Evidence for Superdeformed Shape Isomeric States in 28Si at Excitations Above 40 MeV Through Observations of Selective Particle Decays of 16O + 12C Resonances in 8Be and Alpha Channels '

NUCLEAR REACTIONS 12C(16O, 8Be), (16O, α), E(cm)=25.7-38.6 MeV; analyzed previous data analyses. 28Si deduced superdeformed shape isomeric states structure.

doi: 10.1103/PhysRevC.48.2117
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1993ZH22      Nucl.Phys. A564, 252 (1993)

J.Zhang, W.D.M.Rae

Systematics of 2-Dimensional α-Cluster Configurations in 4N Nuclei from 12C to 44Ti

NUCLEAR STRUCTURE 12C, 16O, 20Ne, 24Mg, 28Si, 32S, 36Ar, 40Ca, 44Ti; calculated α-cluster states, configurations; deduced systematics.

doi: 10.1016/0375-9474(93)90520-8
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1992ME09      Phys.Rev. C46, 2096 (1992)

A.C.Merchant, W.D.M.Rae

Alpha-Chain States in 4N-Nuclei from 20Ne to 32S

NUCLEAR STRUCTURE 20Ne, 24Mg, 28Si, 32S; calculated α-chain states, properties. Bloch-Brink cranked cluster model, effective interaction.

doi: 10.1103/PhysRevC.46.2096
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1992ME11      Nucl.Phys. A549, 431 (1992)

A.C.Merchant, W.D.M.Rae

Systematics of Alpha-Chain States in 4N-Nuclei

NUCLEAR STRUCTURE 8Be, 12C, 16O, 20Ne, 24Mg, 28Si, 32S, 36Ar, 40Ca, 44Ti, 48Cr, 52Fe, 56Ni, 60Zn; calculated α-chain nuclei binding energy, levels; deduced systematics. Block-Brink cranked cluster model.

doi: 10.1016/0375-9474(92)90089-3
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1992RA06      Phys.Lett. 279B, 207 (1992)

W.D.M.Rae, A.C.Merchant

Hyperdeformed States in 36Ar and 48Cr in the Cranked Cluster Model

NUCLEAR STRUCTURE 36Ar, 48Cr; calculated hyperdeformed states α-particle constituents, single particle density contours; deduced possible evidence from reaction data. Cranked cluster model.

doi: 10.1016/0370-2693(92)90380-M
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1992RA25      Phys.Rev.Lett. 69, 3709 (1992)

W.D.M.Rae, A.C.Merchant, B.Buck

The Shape Eigenstate: A new kind of resonance

NUCLEAR REACTIONS 12C(12C, 12C'), E(cm)=33, 35 MeV; analyzed σ(θ); deduced new type of resonance evidence. Coherence between nearly degenerate resonances.

doi: 10.1103/PhysRevLett.69.3709
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1991BE27      Nucl.Phys. A534, 445 (1991)

S.J.Bennett, M.Freer, B.R.Fulton, J.T.Murgatroyd, P.J.Woods, S.C.Allcock, W.D.M.Rae, A.E.Smith, J.S.Lilley, R.R.Betts

Symmetric and Near-Symmetric Fission of 24Mg, 28Si and 32S

NUCLEAR REACTIONS 12C(28Si, F), (28Si, X), (32S, F), (32S, X), E=200 MeV; 12C(24Mg, F), (24Mg, X), E=180 MeV; measured fission, reaction (fragment)(fragment)-coin; deduced reaction mechanism. 24Mg, 28Si, 32S deduced fission characteristics.

doi: 10.1016/0375-9474(91)90511-4
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1991CO09      Europhys.Lett. 14, 221 (1991)

E.Costanzo, M.Lattuada, S.Romano, D.Vinciguerra, M.Zadro, N.Cindro, M.Freer, B.R.Fulton, W.D.M.Rae

Evidence for Excitation of 24Mg Resonant States through the 12C(16O, 12C12C)4He Reaction at 85 MeV

NUCLEAR REACTIONS 12C(16O, α12C), E=85 MeV; measured (12C)(12C)-coin; deduced reaction mechanism. 24Mg deduced resonant state excitation evidence. Kinematically complete experiment.

doi: 10.1209/0295-5075/14/3/006
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1991CO10      Phys.Rev. C44, 111 (1991)

E.Costanzo, M.Lattuada, S.Romano, D.Vinciguerra, N.Cindro, M.Zadro, M.Freer, B.R.Fulton, W.D.M.Rae

Excitation of 24Mg States through the Interaction of 85 MeV 16O Ions with 12C and 24Mg Targets

NUCLEAR REACTIONS 12C, 24Mg(16O, x12C), E=85 MeV; measured σ(θ1, θ2, E1) for x=2. 24Mg deduced levels, J.

doi: 10.1103/PhysRevC.44.111
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1991FU03      J.Phys.(London) G17, 555 (1991)

B.R.Fulton, S.J.Bennett, M.Freer, J.T.Murgatroyd, S.C.Allcock, W.D.M.Rae, A.E.Smith, R.R.Betts, B.B.Back, S.Sanders, F.Videbaek

Search for Large Cluster Breakup of 40Ca

NUCLEAR REACTIONS 12C(40Ca, 12CX), E=300 MeV; measured total energy spectra following projectile breakup. 12C(24Mg, 212C), E not given; analyzed total energy spectra following projectile breakup; deduced no large cluster 40Ca breakup evidence.

doi: 10.1088/0954-3899/17/4/014
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1991FU09      Phys.Lett. 267B, 325 (1991)

B.R.Fulton, S.J.Bennett, M.Freer, J.T.Murgatroyd, G.J.Gyapong, N.S.Jarvis, C.D.Jones, D.L.Watson, J.D.Brown, W.D.M.Rae, A.E.Smith, J.S.Lilley

Spin Measurement for Symmetric Fission States of 24Mg. A New Angle on the 12C + 12C Interaction

NUCLEAR REACTIONS 12C(24Mg, 212C), E=170 MeV; measured (12C)(12C)(θ). 24Mg deduced symmetric fission decay states J, deformation features. Cranked cluster model, Nilsson-Strutinsky calculations.

doi: 10.1016/0370-2693(91)90940-R
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1991GY01      Phys.Rev. C44, 520 (1991)

G.J.Gyapong, N.S.Jarvis, D.L.Watson, S.J.Bennett, M.Freer, B.R.Fulton, J.T.Murgatroyd, R.Hunt, W.D.M.Rae, A.E.Smith

Near-Symmetric Breakup of 25Mg

NUCLEAR REACTIONS 12C(25Mg, X), E=180 MeV; measured (fragment)(fragment)-coin, X=12C, 13C following projectile breakup. 24,25Mg deduced symmetric fissioning states energy.

doi: 10.1103/PhysRevC.44.520
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1990AL14      Nucl.Instrum.Methods Phys.Res. A289, 213 (1990)

S.C.Allcock, P.R.Keeling, W.D.M.Rae, A.E.Smith, S.J.Bennett, M.Freer, B.R.Fulton, R.D.Page, P.J.Woods

A Compact High-Efficiency 8Be Detector

NUCLEAR REACTIONS 12C(24Mg, X), E not given; analyzed 8Be spectra following projectile breakup. Compact high efficiency 8Be detector.

doi: 10.1016/0168-9002(90)90261-4
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1990FU02      J.Phys.(London) G16, 333 (1990)

B.R.Fulton, W.D.M.Rae

Fission of Light Nuclei

NUCLEAR STRUCTURE 23Na, 24Mg, 28Si, 7Li; compiled fission data; deduced clustering role. Different projectile, ejectile combinations.

doi: 10.1088/0954-3899/16/3/007
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1989FU10      Phys.Lett. 232B, 56 (1989)

B.R.Fulton, S.J.Bennett, M.Freer, R.D.Page, P.J.Woods, S.C.Allcock, A.E.Smith, W.D.M.Rae, J.S.Lilley

16O + 8Be Breakup of 24Mg

NUCLEAR REACTIONS C(24Mg, X), E=180 MeV; measured αα-coin; deduced projectile 16O+8Be breakup.

doi: 10.1016/0370-2693(89)90558-3
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1989WO02      Nucl.Instrum.Methods Phys.Res. A276, 195 (1989)

P.J.Woods, S.J.Bennett, M.Freer, B.R.Fulton, R.D.Page, K.A.Connell, R.A.Cunningham, J.Groves, J.Simpson, A.N.James, M.A.C.Hotchkis, W.D.M.Rae

A Detection System for the Study of Alpha and Proton Radioactivity on the Daresbury Recoil Mass Separator

NUCLEAR REACTIONS 110Cd(58Ni, X), E=260 MeV; measured E(α), I(α) following evaporation residue decay. 153Tm, 161,162W, 158,157Hf, 154Yb deduced α-branching ratio. Position sensitive silcon surface barrier detector.

doi: 10.1016/0168-9002(89)90632-3
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1988AL07      Phys.Lett. 201B, 201 (1988)

S.C.Allcock, W.D.M.Rae, P.R.Keeling, A.E.Smith, B.R.Fulton, D.W.Banes

10+ States in 20Ne

NUCLEAR REACTIONS 12C(16O, 20Ne), E=150 MeV; measured α-16O relative energy spectra, double differential σ following 20Ne breakup. 20Ne deduced levels, J, π. Detector telescopes.

doi: 10.1016/0370-2693(88)90212-2
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1987RA02      Phys.Lett. 184B, 133 (1987)

W.D.M.Rae, P.R.Keeling, S.C.Allcock

Spins of 12C + 12C Resonances via the 12C(12C, αα)16O Reaction

NUCLEAR REACTIONS 12C(12C, 2α), E=19-27 MeV; measured σ(θ1, θ2) vs E. 24Mg deduced levels, J, π. Position sensitive Si detectors.

doi: 10.1016/0370-2693(87)90556-9
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1987RA22      Phys.Lett. 198B, 49 (1987)

W.D.M.Rae, P.R.Keeling, A.E.Smith

The Gross Structure Resonance near E(cm)=25 MeV in 12C + 12C Scattering

NUCLEAR REACTIONS 12C(12C, 8Be), E(cm)=25 MeV; measured average σ(θ), (Q-value) spectrum, 8Be(α)-, ααα-coin, angular correlations. 24Mg deduced resonance, J, π.

doi: 10.1016/0370-2693(87)90156-0
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1986FU07      Phys.Lett. 181B, 233 (1986)

B.R.Fulton, S.J.Bennett, C.A.Ogilvie, J.S.Lilley, D.W.Banes, W.D.M.Rae, S.C.Allcock, R.R.Betts, A.E.Smith

Symmetric Fission of 24Mg following Inelastic Scattering

NUCLEAR REACTIONS 12C(24Mg, 212C), (24Mg, 16O8Be), 4He(24Mg, 16O), E=180 MeV; measured total energy spectrum. 24Mg deduced symmetric fission. ΔE-E telescopes, coincidence method.

doi: 10.1016/0370-2693(86)90038-9
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1985FL06      Phys.Rev. C32, 1911 (1985)

N.R.Fletcher, W.D.M.Rae, A.E.Smith, S.C.Allcock, D.L.Gay

Search for Heavy-Ion Resonances in the Reactions 12C(20Ne, α) and 12C(20Ne, 8Be)

NUCLEAR REACTIONS 12C(20Ne, α), (20Ne, 8Be), E(cm)=12-15 MeV; measured σ(θ) vs E. 32S deduced resonances, J, π.

doi: 10.1103/PhysRevC.32.1911
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1985FO11      J.Phys.(London) G11, 1175 (1985)

H.T.Fortune, L.C.Bland, W.D.M.Rae

Location of the (1d5/2)(1d3/2) 4+ Level in 18O

NUCLEAR REACTIONS 16O(t, p), E=15 MeV; 17O(d, p), E=12 MeV; measured absolute σ(E(p), θ). 18O deduced levels, J, π.

doi: 10.1088/0305-4616/11/10/013
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1985RA12      Phys.Lett. 156B, 167 (1985)

W.D.M.Rae, S.C.Allcock, S.Marsh, B.R.Fulton

High-Spin α-Cluster Resonances in 16O

NUCLEAR REACTIONS 12C(12C, 16O), E=120 MeV; measured σ(E(16O)), α(12C)-coin, σ(θα, φα). 16O levels deduced decay characteristics, J, π, Γα0/Γα1.

doi: 10.1016/0370-2693(85)91502-3
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1985SM04      Nucl.Phys. A441, 701 (1985)

A.E.Smith, S.C.Allcock, W.D.M.Rae, B.R.Fulton, D.W.Banes

A Study of 19F by Inelastic Scattering on a 12C Target at 82 MeV and 144 MeV Using the Techniques of Resonant Particle Spectroscopy

NUCLEAR STRUCTURE 19F; calculated levels, B(λ). Shell model.

NUCLEAR REACTIONS 12C(19F, 15Nα), E=82, 144 MeV; measured dependence of α-correlation on emission angle. 19F levels deduced J. DWBA, strong absorption model analyses, shell model calculations.

doi: 10.1016/0375-9474(85)90444-0
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1985WI18      Nucl.Phys. A437, 65 (1985)

J.S.Winfield, N.A.Jelley, W.D.M.Rae, C.L.Woods

Spectroscopic-Factor Discrepancies in (9Be, 10B) For Different Ejectile Excitations

NUCLEAR REACTIONS 63Cu, 54Fe, 26,24Mg, 16O(9Be, 10B), 26Mg, 16O(9Be, 9Be), E=43 MeV; 40Ca(9Be, 10B), (9Be, 9Be), E=30, 45 MeV; measured σ(θ). 62Ni, 53Mn, 25,23Na, 15N, 39K levels deduced spectroscopic factors. Magnetic spectrometer, ΔE counter telescope.

doi: 10.1016/0375-9474(85)90227-1
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1984BH01      Phys.Lett. 136B, 149 (1984)

R.K.Bhowmik, W.D.M.Rae, B.R.Fulton

Spin Measurements and Reaction Mechanism in the Inelastic Scattering of 18O on 12C

NUCLEAR REACTIONS 12C(18O, 18O'), 12C(18O, α12C), E=82 MeV; measured σ(θ(α), θ(12C)), σ(E(rel)); deduced reaction mechanism. 18O levels deduced J. Strong absorption model, projectile breakup.

doi: 10.1016/0370-2693(84)91169-9
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1984RA07      Nucl.Phys. A420, 320 (1984)

W.D.M.Rae, R.K.Bhowmik

Reaction Mechanism and Spin Information in the Sequential Breakup of 18O at 82 MeV

NUCLEAR REACTIONS 12C(18O, α14C), (18O, α13C), (18O, α12C), (18O, α15N), E=82 MeV; measured (particle)(particle)(θ), σ(θ(18O), θ(α)). 18O levels deduced decay characteristics, J, π, sequential breakup in 14C+α channel. Strong absorption DWBA model analysis.

doi: 10.1016/0375-9474(84)90445-7
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1984RA10      Phys.Rev. C30, 158 (1984)

W.D.M.Rae, A.J.Cole, B.G.Harvey, R.G.Stokstad

Breakup of 16O and 20Ne at 9 MeV/Nucleon

NUCLEAR REACTIONS 12,13C, 28Si(16O, 16O'), (16O, 20Ne), E=140 MeV; 12C(20Ne, 20Ne), E=175 MeV; measured relative E spectra, α(12C)-, α(16O)-coin; deduced ejectile sequential breakup role.

doi: 10.1103/PhysRevC.30.158
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1984RA17      Nucl.Phys. A427, 142 (1984)

W.D.M.Rae, R.K.Bhowmik

Excitation of Anomalous α - 14C Resonances in the Inelastic Scattering of 18O on a 12C Target

NUCLEAR REACTIONS 12C(18O, α14C), E=82 MeV; measured σ(18O(θ), θα) vs emission angle. 18O levels deduced spins. Strong absorption model analysis.

doi: 10.1016/0375-9474(84)90142-8
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1983ME04      Phys.Lett. 121B, 111 (1983)

A.Menchaca-Rocha, M.E.Brandan, A.Dacal, A.Galindo, J.Mahoney, M.Murphy, W.D.M.Rae

Incomplete Momentum Transfer Components in 16O + 12C Fusion at 20 MeV/A

NUCLEAR REACTIONS 12C(16O, X), E=20 MeV/nucleon; measured σ(fragment E), fragment relative yield vs Z; deduced incomplete momentum transfer in fusion.

doi: 10.1016/0370-2693(83)90896-1
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1983NA04      Z.Phys. A311, 297 (1983)

W.J.Naude, H.S.Bradlow, O.Dietzsch, A.A.Pilt, W.D.M.Rae, D.Sinclair

Elastic Scattering of 20Ne on 24Mg

NUCLEAR REACTIONS 24Mg(20Ne, 20Ne), E=40 MeV; measured σ(θ); deduced elastic transfer mechanism, Sα. Optical model analysis. Surface barrier, position sensitive detectors, coincidence technique.


1981CO22      Phys.Rev.Lett. 47, 1705 (1981)

A.J.Cole, W.D.M.Rae, M.E.Brandan, A.Dacal, B.G.Harvey, R.Legrain, M.J.Murphy, R.G.Stokstad

12C + 12C Reaction Cross Section between 70 and 290 MeV Obtained from Elastic Scattering

NUCLEAR REACTIONS 12C(12C, 12C), E=120-290 MeV; measured σ(θ) vs momentum transfer; deduced σ(total), σ(reaction).

doi: 10.1103/PhysRevLett.47.1705
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1981GO02      Nucl.Phys. A351, 519 (1981)

N.S.Godwin, W.D.M.Rae, B.Cooke, A.Etchegoyen, N.J.Eyre, P.S.Fisher, G.Proudfoot, D.Sinclair

A Study of Three-Nucleon Transfer Reactions on 18O

NUCLEAR REACTIONS 18O(11B, 8Li), (12C, 9Be), E=115 MeV; 18O(13C, 10B), E=105 MeV; measured σ(E(8Li)), σ(E(9Be)), σ(E(10B)). Shell model, semiclassical reaction model. Enriched gas target.

doi: 10.1016/0375-9474(81)90186-X
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1981GO11      Nucl.Phys. A363, 493 (1981)

N.S.Godwin, W.D.M.Rae, B.Cooke, A.Etchegoyen, N.J.Eyre, P.S.Fisher, G.Proudfoot, D.Sinclair

A DWBA Analysis of Heavy-Ion Induced Three-Nucleon Transfer Reactions on 15N, 16O and 18O

NUCLEAR REACTIONS 15N, 16,18O(11B, 8Li), (12C, 9Be), E=115 MeV; 15N, 16,18O(13C, 10B), E=105 MeV; measured σ(θ). DWBA analysis. Enriched gas target.

doi: 10.1016/0375-9474(81)90270-0
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1981RA20      Phys.Lett. 105B, 417 (1981)

W.D.Rae, A.J.Cole, A.Dacal, R.Legrain, B.G.Harvey, J.Mahoney, M.J.Murphy, R.G.Stokstad, I.Tserruya

Coherent and Incoherent Processes in Projectile Breakup

NUCLEAR REACTIONS 12,13C, 28Si(16O, α12C), E=140 MeV; measured 12Cα-coin, total, relative energies of fragments; deduced coherent, incoherent projectile breakup.

doi: 10.1016/0370-2693(81)91195-3
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1981SH01      Phys.Rev.Lett. 46, 12 (1981)

A.C.Shotter, A.N.Bice, J.M.Wouters, W.D.Rae, J.Cerny

Observation of the Direct and Sequential Breakup of 7Li from 12C and 208Pb Targets at 70 MeV

NUCLEAR REACTIONS 12C, 208Pb(7Li, t), E=70 MeV; measured tα-coin, σ(θ(7Li')), σ(Et, θ). 7Li deduced direct, sequential breakup, α + t cluster structure of underlying level.

doi: 10.1103/PhysRevLett.46.12
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1980PR09      Nucl.Phys. A345, 278 (1980)

G.Proudfoot, H.S.Bradlow, P.S.Fisher, N.S.Godwin, J.King, D.Sinclair, W.D.M.Rae

Sequential Calculations for Heavy-Ion Induced Two-Nucleon Transfer on 14N, 15N and 16O

NUCLEAR REACTIONS 14N(13C, X), E=105 MeV; 14N(11B, 9Be), E=115 MeV; measured σ(θ). 15,16,17,18O, 19F deduced S. DWBA analysis, sequential transfer. Gas target.

doi: 10.1016/0375-9474(80)90425-X
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1980RA12      Phys.Rev.Lett. 45, 884 (1980)

W.D.Rae, R.G.Stokstad, B.G.Harvey, A.Dacal, R.Legrain, J.Mahoney, M.J.Murphy, T.J.M.Symons

Molecular Resonances and the Production of Fast α Particles in the Reaction of 16O with 12,13C Nuclei

NUCLEAR REACTIONS 12,13C(16O, α), E=140 MeV; measured α12C-coin; deduced no molecular resonance or final-state interaction between carbon ions. 16O levels deduced excitation, decay probabilities.

doi: 10.1103/PhysRevLett.45.884
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1979BR03      Nucl.Phys. A314, 171 (1979)

H.S.Bradlow, W.D.M.Rae, P.S.Fisher, N.S.Godwin, G.Proudfoot, D.Sinclair

A DWBA Analysis of Heavy Ion α-Transfer Reactions on 16O

NUCLEAR REACTIONS 16O(7Li, t), E=50, 68 MeV; 16O(11B, 7Li), (11B, 11B), E=115 MeV; 16O(7Li, 7Li), E=68 MeV; 20Ne(7Li, 7Li), E=68, 89 MeV; 16O(13C, 13C), (13C, 9Be), E=105 MeV; measured σ(θ). 20Ne levels deduced Sα. Optical model, DWBA analysis, cluster model. Enriched gas target.

doi: 10.1016/0375-9474(79)90561-X
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1979BR04      Nucl.Phys. A314, 207 (1979)

H.S.Bradlow, W.D.M.Rae, P.S.Fisher, N.S.Godwin, G.Proudfoot, D.Sinclair

Heavy Ion Induced α-Transfer on Targets of Mass 12 to 15

NUCLEAR REACTIONS 14,15N(11B, 7Li), E=115 MeV; 12,13C, 15N(13C, 9Be), E=105 MeV; 12C(7Li, t), E=68 MeV; 12C(7Li, 7Li), E=89 MeV; measured σ(θ). 19,18F, 16O levels deduced Sα. 17O deduced levels. Optical model, DWBA analysis, cluster model. Enriched gas target.

doi: 10.1016/0375-9474(79)90562-1
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1979GO17      Nucl.Phys. A331, 237 (1979)

N.S.Godwin, W.D.Rae, B.Cooke, N.J.Eyre, P.S.Fisher, G.Proudfoot, D.Sinclair

A Study of Three-Nucleon Transfer Reactions of 17O

NUCLEAR REACTIONS 17O(11B, 8Li), (12C, 9Be), E=115 MeV; 17O(13C, 10B), E=105 MeV; measured particle spectra. Shell model, semi-classical reaction model, enriched gas target.

doi: 10.1016/0375-9474(79)90311-7
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1979PR07      Nucl.Phys. A329, 271 (1979)

G.Proudfoot, W.D.M.Rae

Absolute Normalization in Heavy Ion Induced Two-Neutron Transfer Reactions on 12C

NUCLEAR REACTIONS 12C(16O, 15O), 12C(16O, 15N), 12C(16O, 14O), E=128 MeV; measured σ(θ). 13C, 14C, 13N deduced S, sequential transfer, cluster transfer. Optical model, shell model.

doi: 10.1016/0375-9474(79)90294-X
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1979RA10      Nucl.Phys. A319, 239 (1979)

W.D.M.Rae, N.S.Godwin, D.Sinclair, H.S.Bradlow, P.S.Fisher, J.D.King, A.A.Pilt, G.Proudfoot

Few-Nucleon Transfer Reactions on 15N and 16O

NUCLEAR REACTIONS 16O, 15N(13C, 10B), (13C, 11C), 16O(13C, 13C), (13C, 12C), (13C, 12B), E=105 MeV; 16O, 15N(11B, 8Li), (11B, 9Li), (11B, 9Be), (12C, 7Li), (12C, 8Li), (12C, 9Be), 15N(11B, 10Be), 16O(11B, 7Li), (11B, 10B), (11B, 10C), (11B, 11B), (11B, 11C), (11B, 12C), (12C, 12C), E=115 MeV; 16O(18O, 16O), E=126 MeV; measured σ(θ). 16,17O, 17F levels deduced S, parity. 18O deduced parity. Optical model, DWBA analysis. Weak coupling, shell, cluster models. Enriched gas targets.

doi: 10.1016/0375-9474(79)90184-2
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1976PI16      Nucl.Phys. A273, 189 (1976)

A.A.Pilt, D.J.Millener, H.Bradlow, O.Dietzsch, P.S.Fisher, W.J.Naude, W.D.M.Rae, D.Sinclair

Study of States in 19F and 20Ne via the (13C, 9Be) α-Transfer Reaction

NUCLEAR REACTIONS 15N, 16O(13C, 9Be), E=105 MeV; measured σ(E, θ). 19F, 20Ne deduced levels, relative spectroscopic amplitudes, suggested J, π values. Enriched gas targets. Shell-model calculation.

doi: 10.1016/0375-9474(76)90307-9
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