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Search: Author = J.S.Al-Khalili

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2021DI07      Phys.Rev. C 104, 034614 (2021)

M.J.Dinmore, N.K.Timofeyuk, J.S.Al-Khalili

Three-body optical potentials in (d, p) reactions and their influence on indirect study of stellar nucleosynthesis

NUCLEAR REACTIONS 26Al, 30P, 34Cl, 56Ni(d, p), E=12 MeV; calculated GRZ and KD03 σ and σ(θ), former using Giannini, Ricco, and Zucchiatti nonlocal optical potentials, and the latter from Johnson-Tandy potentials; deduced model uncertainties in total σ and σ(θ). 27Al, 57Ni(d, p), E=8.9, 12 MeV; calculated squared asymptotic normalization coefficients (ANCs) and proton widths (Γp) for mirror pairs: 27Al-27Si and 57Ni-57Cu. Adiabatic distorted-wave approximation (ADWA) with dominant contribution from the components of the three-body effects. Relevance to quantifying model uncertainties in ADWA calculations, and to important resonances contributing to nucleosynthesis in stellar environments via astrophysical (p, γ) reactions in rp process.

doi: 10.1103/PhysRevC.104.034614
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2020TI06      Phys.Rev. C 102, 064616 (2020)

N.K.Timofeyuk, M.J.Dinmore, J.S.Al-Khalili

Three-nucleon force contribution to the deuteron channel in (d, p) reactions

NUCLEAR REACTIONS 26Al(d, p), E=12 MeV; 40Ca(d, p), E=11.8, 12, 56 MeV; calculated adiabatic potential, deuteron s-wave and d-wave functions, monopole and quadrupole adiabatic effective potentials, absolute values of volume integrals and rms radii of effective interactions, differential σ(θ). Adiabatic distorted wave approximation (ADWA) for three-body model n+p+A of target, with four different three- nucleon interaction sets from local chiral effective field theory (EFT) at next-to-next-to-leading order.

doi: 10.1103/PhysRevC.102.064616
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2019DI09      Phys.Rev. C 99, 064612 (2019)

M.J.Dinmore, N.K.Timofeyuk, J.S.Al-Khalili, R.C.Johnson

Effects of an induced three-body force in the incident channel of (d, p) reactions

NUCLEAR REACTIONS 40Ca(d, p)41Ca, E=11.8, 20, 56 MeV; calculated differential σ(θ, E) using the adiabatic distorted-wave approximation (ADWA) with and without first-order contribution of induced three-body (I3B) force. Comparison with experimental data.

doi: 10.1103/PhysRevC.99.064612
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2013CU01      Phys.Rev. C 87, 054601 (2013)

E.S.Cunningham, J.S.Al-Khalili, R.C.Johnson

Effect of spin-spin interactions on nucleon-nucleus scattering

NUCLEAR REACTIONS 10B(p, p), E=200 MeV; calculated polarization transfer coefficient DNN as a function of angle using spin-spin interaction in the optical potential. Spin-spin tensors evaluated with DWBA. Folding model using realistic effective nucleon-nucleon interaction. Local and nonlocal spin-spin tensor interactions. Effect of parameters of the model used to describe the nuclear structure. Comparison with experimental data.

doi: 10.1103/PhysRevC.87.054601
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2011CU03      Phys.Rev. C 84, 041601 (2011)

E.S.Cunningham, J.S.Al-Khalili, R.C.Johnson

Role of the tensor exchange potential in nucleon-nucleus scattering

NUCLEAR REACTIONS 10B(p, p), E=200 MeV; calculated spin-spin tensor interactions, polarization transfer coefficient DNN. Distorted-wave Born approximation. Comparison with experimental data.

doi: 10.1103/PhysRevC.84.041601
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2010BI03      Phys.Lett. B 690, 15 (2010)

L.Bianco, R.D.Page, I.G.Darby, D.T.Joss, J.Simpson, J.S.Al-Khalili, A.J.Cannon, B.Cederwall, S.Eeckhaudt, S.Erturk, B.Gall, M.B.Gomez Hornillos, T.Grahn, P.T.Greenlees, B.Hadinia, K.Heyde, U.Jakobsson, P.M.Jones, R.Julin, S.Juutinen, S.Ketelhut, M.Labiche, M.Leino, A.-P.Leppanen, M.Nyman, D.O'Donnell, E.S.Paul, M.Petri, P.Peura, A.Puurunen, P.Rahkila, P.Ruotsalainen, M.Sandzelius, P.J.Sapple, J.Saren, C.Scholey, N.A.Smirnova, A.N.Steer, P.D.Stevenson, E.B.Suckling, J.Thomson, J.Uusitalo, M.Venhart

Discovery of 157W and 161Os

NUCLEAR REACTIONS 106Cd(58Ni, 3n), E=290, 310 MeV; measured reaction products; deduced α spectra, α-branching, T1/2, fine structure, ground state J, π.

RADIOACTIVITY 161Os(α), 157W(β+); measured decay products; deduced T1/2, β-branching. Comparison with shell model calculations.

doi: 10.1016/j.physletb.2010.04.056
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2010YA03      Few-Body Systems 47, 213 (2010)

A.Yakhelef, N.K.Timofeyuk, J.S.Al-Khalili, I.J.Thompson

Three-Body Spectrum of 18C and its Relevance to r-Process Nucleosynthesis

NUCLEAR STRUCTURE 16,17,18C; calculated energy levels, transition strengths, two-neutron separation energy.

NUCLEAR REACTIONS 17C(n, γ), E not given; calculated B(M1), astrophysical reaction rate, σ.

doi: 10.1007/s00601-010-0086-8
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2007AL08      Phys.Rev. C 75, 024608 (2007)

J.S.Al-Khalili, R.Crespo, R.C.Johnson, A.M.Moro, I.J.Thompson

Few-body multiple scattering calculations for 6He on protons

NUCLEAR REACTIONS 1H(α, α), E=699 MeV/nucleon; 1H(6He, 6He), E=717 MeV/nucleon; calculated elastic σ(θ). Multiple scattering expansion, comparison with data.

doi: 10.1103/PhysRevC.75.024608
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2007PA27      Phys.Rev. C 75, 061302 (2007)

R.D.Page, L.Bianco, I.G.Darby, J.Uusitalo, D.T.Joss, T.Grahn, R.-D.Herzberg, J.Pakarinen, J.Thomson, S.Eeckhaudt, P.T.Greenlees, P.M.Jones, R.Julin, S.Juutinen, S.Ketelhut, M.Leino, A.-P.Leppanen, M.Nyman, P.Rahkila, J.Saren, C.Scholey, A.Steer, M.B.Gomez Hornillos, J.S.Al-Khalili, A.J.Cannon, P.D.Stevenson, S.Erturk, B.Gall, B.Hadinia, M.Venhart, J.Simpson

α decay of 159Re and proton emission from 155Ta

RADIOACTIVITY 159Re(α) [from 106Cd(58Ni, X)]; 155Ta(p); measured Eα, Iα, Ep, Ip. deduced separation energies.

doi: 10.1103/PhysRevC.75.061302
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2006JO10      Phys.Lett. B 641, 34 (2006)

D.T.Joss, I.G.Darby, R.D.Page, J.Uusitalo, S.Eeckhaudt, T.Grahn, P.T.Greenlees, P.M.Jones, R.Julin, S.Juutinen, S.Ketelhut, M.Leino, A.-P.Leppanen, M.Nyman, J.Pakarinen, P.Rahkila, J.Saren, C.Scholey, A.Steer, A.J.Cannon, P.D.Stevenson, J.S.Al-Khalili, S.Erturk, M.Venhart, B.Gall, B.Hadinia, J.Simpson

Probing the limit of nuclear existence: Proton emission from 159Re

NUCLEAR REACTIONS 106Cd(58Ni, 4np), E=300 MeV; measured Eα, Iα, Ep, Ip, (recoil)α-coin following residual nucleus decay. Recoil-decay correlation technique.

RADIOACTIVITY 159Re(p) [from 106Cd(58Ni, 4np)]; measured Ep, T1/2; deduced ground-state configuration.

doi: 10.1016/j.physletb.2006.08.014
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2005AL17      Nucl.Phys. A751, 469c (2005)

J.S.Al-Khalili

The Thrill of Discovery: Nuclear Physics Research in the 21st Century

doi: 10.1016/j.nuclphysa.2005.02.048
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2005BA87      J.Phys.(London) G31, S1491 (2005)

G.C.Ball, T.Achtzehn, D.Albers, J.S.Al-Khalili, C.Andreoiu, A.Andreyev, S.F.Ashley, R.A.E.Austin, J.A.Becker, P.Bricault, S.Chan, R.S.Chakrawarthy, R.Churchman, H.Coombes, E.S.Cunningham, J.Daoud, M.Dombsky, T.E.Drake, B.Eshpeter, P.Finlay, P.E.Garrett, C.Geppert, G.F.Grinyer, G.Hackman, V.Hanemaayer, B.Hyland, G.A.Jones, K.A.Koopmans, W.D.Kulp, J.Lassen, J.P.Lavoie, J.R.Leslie, Y.Litvinov, J.A.Macdonald, C.Mattoon, D.Melconian, A.C.Morton, C.J.Osborne, C.J.Pearson, M.Pearson, A.A.Phillips, J.J.Ressler, F.Sarazin, M.A.Schumaker, J.Schwarzenberg, H.C.Scraggs, M.B.Smith, C.E.Svensson, J.J.Valiente-Dobon, J.C.Waddington, P.M.Walker, K.Wendt, S.J.Williams, J.L.Wood, E.F.Zganjar

High-resolution γ-ray spectroscopy: a versatile tool for nuclear β-decay studies at TRIUMF-ISAC

doi: 10.1088/0954-3899/31/10/019
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2005HO28      J.Phys.(London) G31, S1881 (2005)

D.J.Howell, J.A.Tostevin, J.S.Al-Khalili

Coupled channels calculations of 11Be breakup

NUCLEAR REACTIONS 12C(11Be, n10Be), E=67 MeV/nucleon; calculated σ(E, θ). Coupled discretized continuum channels method, comparison with data.

doi: 10.1088/0954-3899/31/10/093
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2005ZH17      Phys.Rev. C 71, 054004 (2005)

Q.Zhao, J.S.Al-Khalili, P.L.Cole

Vector meson photoproduction studied in its radiative decay channel

doi: 10.1103/PhysRevC.71.054004
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2004GA42      Eur.Phys.J. A 21, 185 (2004)

M.W.Gaber, C.Wilkin, J.S.Al-Khalili

Non-eikonal corrections for the scattering of spin-one particles

NUCLEAR REACTIONS 58Ni(d, d), E=400, 700 MeV; calculated σ(θ), analyzing powers, non-eikonal corrections.

doi: 10.1140/epja/i2003-10196-9
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2004SA46      Phys.Rev. C 70, 031302 (2004)

F.Sarazin, J.S.Al-Khalili, G.C.Ball, G.Hackman, P.M.Walker, R.A.E.Austin, B.Eshpeter, P.Finlay, P.E.Garrett, G.F.Grinyer, K.A.Koopmans, W.D.Kulp, J.R.Leslie, D.Melconian, C.J.Osborne, M.A.Schumaker, H.C.Scraggs, J.Schwarzenberg, M.B.Smith, C.E.Svensson, J.C.Waddington, J.L.Wood

Halo neutrons and the β decay of 11Li

RADIOACTIVITY 11Li(β-), (β-n) [from Ta(p, X)]; measured Eγ, Iγ, β-delayed neutron spectra. 10,11Be deduced levels, J, π, halo features.

doi: 10.1103/PhysRevC.70.031302
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2004ZH23      J.Phys.(London) G30, 1153 (2004)

Q.Zhao, J.S.Al-Khalili, R.C.Johnson

A quark model framework for the study of nuclear medium effects

NUCLEAR REACTIONS 2H(γ, π0), E=300 MeV; calculated σ(θ), medium effects. Quark model framework, comparison with data.

doi: 10.1088/0954-3899/30/9/014
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2002AL25      Eur.Phys.J. A 15, 115 (2002)

J.S.Al-Khalili

Structure and reactions of halo nuclei: An entangled approach

NUCLEAR STRUCTURE 6,7,8,9,10Li; calculated radii.

NUCLEAR REACTIONS 58Ni(8B, 7BeX), E=25.8 MeV; 12C(11Be, 11Be), E=10 MeV/nucleon; calculated σ(θ).

doi: 10.1140/epja/i2001-10237-5
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2002SU18      Phys.Rev. C66, 014614 (2002)

N.C.Summers, J.S.Al-Khalili, R.C.Johnson

Nonadiabatic Corrections to Elastic Scattering of Halo Nuclei

NUCLEAR REACTIONS 12C(6He, 6He), (11Be, 11Be), E=10 MeV/nucleon; calculated σ(θ), nonadiabatic corrections. Eikonal approximation, partial wave analysis, two-body projectile.

doi: 10.1103/PhysRevC.66.014614
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2002ZH06      Phys.Rev. C65, 032201 (2002)

Q.Zhao, J.S.Al-Khalili, C.Bennhold

Contributions of Vector Meson Photoproduction to the Gerasimov-Drell-Hearn Sum Rule

NUCLEAR REACTIONS 1n, 1H(γ, X), E=1-6 GeV; calculated ω and ρ meson production σ, σ(θ), contributions to sum rule.

doi: 10.1103/PhysRevC.65.032201
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2002ZH20      Phys.Rev. C65, 065204 (2002)

Q.Zhao, J.S.Al-Khalili, Z.-P.Li, R.L.Workman

Pion Photoproduction on the Nucleon in the Quark Model

NUCLEAR REACTIONS 1H(γ, π+), (γ, π0), E ≈ 200-700 MeV; 1n(γ, π-), (γ, π0), E ≈ 200-700 MeV; calculated σ, σ(θ), polarization observables. Quark model, comparison with data.

doi: 10.1103/PhysRevC.65.065204
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2001AL27      Nucl.Phys. A689, 551c (2001)

J.S.Al-Khalili

Validity of Spectator Core Model in Neutron Knock-Out Reactions

doi: 10.1016/S0375-9474(01)00902-2
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2001ZH18      Phys.Lett. 509B, 231 (2001)

Q.Zhao, B.Saghai, J.S.Al-Khalili

Non-Diffractive Mechanisms in the φ-Meson Photoproduction on Nucleons

NUCLEAR REACTIONS 1H(γ, pX), 1n(γ, nX), E ≈ 2-10 GeV; calculated φ meson production σ. Phenomenological quark model.

doi: 10.1016/S0370-2693(01)00432-4
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2001ZH36      Phys.Rev. C64, 052201 (2001)

Q.Zhao, J.S.Al-Khalili, C.Bennhold

Quark Model Predictions for K* Photoproduction on the Proton

NUCLEAR REACTIONS 1H(γ, X), E=1.8-3.4 GeV; calculated K* vector meson production σ, σ(θ). Quark model.

doi: 10.1103/PhysRevC.64.052201
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1999BR09      Phys.Rev. C59, 1560 (1999)

J.M.Brooke, J.S.Al-Khalili, J.A.Tostevin

Noneikonal Calculations for Few-Body Projectiles

NUCLEAR REACTIONS 12C(n, n), (d, d), (10Be, 10Be), (11Be, 11Be), E=10, 25, 50 MeV/nucleon; calculated σ(θ). Few-body Glauber model, exact partial wave phase shift.

doi: 10.1103/PhysRevC.59.1560
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1999RU07      Phys.Rev. C60, 027002 (1999)

S.Rugmai, J.S.Al-Khalili, R.C.Johnson, J.A.Tostevin

Three-Body Effects in the (d, 2He) Charge-Exchange Reaction

NUCLEAR REACTIONS 12C(d, 2p), E=270 MeV; calculated σ(θ); deduced three-body effects. Eikonal description, comparison with distorted wave approach.

doi: 10.1103/PhysRevC.60.027002
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1999TO01      Phys.Rev. C59, R5 (1999)

J.A.Tostevin, J.S.Al-Khalili

Calculations of Reaction Cross Sections for 19C at Relativistic Energies

NUCLEAR REACTIONS 12C(19C, X), E=960 MeV/nucleon; calculated reaction σ vs separation energy, radius. Few-body Glauber theory, comparison with optical limit approximation.

doi: 10.1103/PhysRevC.59.R5
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1998AL05      Phys.Rev. C57, 1846 (1998)

J.S.Al-Khalili, J.A.Tostevin

Few-Body Calculations of Proton-6,8He Scattering

NUCLEAR REACTIONS 1H(α, α), (6He, 6He), (8He, 8He), E ≈ 700 MeV/nucleon; analyzed σ(q2); deduced nuclear radius effects. Few-body calculations.

doi: 10.1103/PhysRevC.57.1846
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1998TO05      Nucl.Phys. A630, 340c (1998)

J.A.Tostevin, R.C.Johnson, J.S.Al-Khalili

Manifestation of Halo Size Scattering and Reactions

NUCLEAR REACTIONS 12C(6Li, X), (6He, X), E=800 MeV/nucleon; analyzed reaction σ; deduced projectile radius dependence. 12C(11Be, 11Be), E=49.3 MeV/nucleon; 12C(19C, 19C), E=30 MeV/nucleon; calculated σ(θ).

doi: 10.1016/S0375-9474(97)00772-0
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1998TO17      J.Phys.(London) G24, 1589 (1998)

J.A.Tostevin, J.S.Al-Khalili, J.M.Brooke, J.A.Christley

Sizes and Interactions of Halo Nuclei

doi: 10.1088/0954-3899/24/8/038
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1997AL05      Phys.Rev. C55, R1018 (1997)

J.S.Al-Khalili, J.A.Tostevin, J.M.Brooke

Beyond the Eikonal Model for Few-Body Systems

NUCLEAR REACTIONS 12C(11Be, 11Be), E=25, 49.3 MeV/nucleon; calculated σ(θ). Improved few-body Glauber model calculations.

doi: 10.1103/PhysRevC.55.R1018
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1997CH32      Nucl.Phys. A624, 275 (1997)

J.A.Christley, J.S.Al-Khalili, J.A.Tostevin, R.C.Johnson

Four-Body Adiabatic Model Applied to Elastic Scattering

NUCLEAR REACTIONS 12C(11Li, 11Li), E=55, 110, 220, 330, 637, 1100 MeV; calculated σ(θ). Four-body adiabatic, eikonal models compared, comparison with data for E=637 MeV.

doi: 10.1016/S0375-9474(97)00360-6
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1997JO16      Phys.Rev.Lett. 79, 2771 (1997)

R.C.Johnson, J.S.Al-Khalili, J.A.Tostevin

Elastic Scattering of Halo Nuclei

NUCLEAR REACTIONS 12C(11Be, 11Be), E=49.3 MeV/nucleon; calculated σ(θ), form factors. 12C(19C, 19C), E=30 MeV/nucleon; calculated form factor, σ(θ); deduced halo structure role.

doi: 10.1103/PhysRevLett.79.2771
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1997TO04      Nucl.Phys. A616, 418c (1997)

J.A.Tostevin, J.S.Al-Khalili

How Large are the Halos of Light Nuclei ( Question )

NUCLEAR REACTIONS 12C(11Li, X), (6He, X), E=800 MeV/nucleon; calculated reaction radii vs rms radii, hyperradii. Glauber theory, Faddeev three-body wavefunctions, static density approximation.

doi: 10.1016/S0375-9474(97)00111-5
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1997TO11      Phys.Rev. C56, R2929 (1997)

J.A.Tostevin, J.S.Al-Khalili, M.Zahar, M.Belbot, J.J.Kolata, K.Lamkin, D.J.Morrissey, B.M.Sherrill, M.Lewitowicz, A.H.Wuosmaa

Elastic and Quasielastic Scattering of 8He from 12C

NUCLEAR REACTIONS 12C(8He, 8He), (8He, 8He'), E=60 MeV/nucleon; measured σ(θ); deduced few-body correlations role. Eikonal few-body method. Quasielastic reaction.

doi: 10.1103/PhysRevC.56.R2929
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1996AL11      Phys.Lett. 378B, 45 (1996)

J.S.Al-Khalili, M.D.Cortina-Gil, P.Roussel-Chomaz, N.Alamanos, J.Barrette, W.Mittig, F.Auger, Y.Blumenfeld, J.M.Casandjian, M.Chartier, V.Fekou-Youmbi, B.Fernandez, N.Frascaria, A.Gillibert, H.Laurent, A.Lepine-Szily, N.A.Orr, V.Pascalon, J.A.Scarpaci, J.L.Sida, T.Suomijarvi

Elastic Scattering of 6He and Its Analysis within a Four-Body Eikonal Model

NUCLEAR REACTIONS 12C(6He, 6He), E=41.6 MeV/nucleon; measured σ(θ). Four-body eikonal model analysis.

doi: 10.1016/0370-2693(96)00336-X
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0244.


1996AL13      Phys.Rev.Lett. 76, 3903 (1996)

J.S.Al-Khalili, J.A.Tostevin

Matter Radii of Light Halo Nuclei

NUCLEAR REACTIONS 12C(11Li, X), (11Be, X), (8B, X), E=800 MeV/nucleon; calculated few-body adiabatic reaction σ, static density. 11Li, 11Be, 8B deduced matter radii related features. Static density model.

doi: 10.1103/PhysRevLett.76.3903
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1996AL24      Phys.Rev. C54, 1843 (1996)

J.S.Al-Khalili, J.A.Tostevin, I.J.Thompson

Radii of Halo Nuclei from Cross Section Measurements

NUCLEAR REACTIONS, ICPND 12C(10Be, X), (α, X), (9Li, X), (12Be, X), E=800 MeV/nucleon; 12C(11Li, X), E=200-800 MeV/nucleon; analyzed reaction σ; deduced core, halo matter rms radii. Static density, few-body models.

doi: 10.1103/PhysRevC.54.1843
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1996BU09      Phys.Rev. C53, 3009 (1996)

M.P.Bush, J.S.Al-Khalili, J.A.Tostevin, R.C.Johnson

Sensitivity of Reaction Cross Sections to Halo Nucleus Density Distributions

NUCLEAR REACTIONS 1H, 12C, 208Pb(11Li, X), E=800 MeV/nucleon; calculated reaction σ, transparency function vs model parameters ratio; deduced halo nucleus density distribution dependence. Optical limit Glauber model.

doi: 10.1103/PhysRevC.53.3009
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1996ZA04      Phys.Rev. C54, 1262 (1996)

M.Zahar, M.Belbot, J.J.Kolata, K.Lamkin, D.J.Morrissey, B.M.Sherrill, M.Lewitowicz, A.H.Wuosmaa, J.S.Al-Khalili, J.A.Tostevin, I.J.Thompson

Quasielastic Scattering of 9Li on 12C

NUCLEAR REACTIONS 12C(9Li, X), E=540 MeV; measured quasielastic σ(θ); calculated quasielastic σ(θ). 12C(11Li, X), E=637 MeV; analyzed quasielastic σ(θ); deduced effective interaction.

doi: 10.1103/PhysRevC.54.1262
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1995AI03      Nucl.Phys. A589, 307 (1995)

S.Ait-Tahar, J.S.Al-Khalili, Y.Nedjadi

A Relativistic Model for α-Nucleus Elastic Scattering

NUCLEAR REACTIONS 40Ca, 12C(α, α), E=104 MeV; 90Zr, 40Ca(α, α), E=141 MeV; 58Ni(α, α), E=139 MeV; calculated σ(θ). Relativistic model.

doi: 10.1016/0375-9474(95)00128-N
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1995AL01      Nucl.Phys. A581, 315 (1995)

J.S.Al-Khalili

Effect of the Breakup Channel on 11Li Elastic Scattering

NUCLEAR REACTIONS 12C(11Li, 11Li), E=57.9 MeV/nucleon; 28Si(11Li, 11Li), E=29 MeV/nucleon; analyzed σ(θ) data; deduced breakup channel coupling role.

doi: 10.1016/0375-9474(94)00431-L
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1995AL02      Nucl.Phys. A581, 331 (1995)

J.S.Al-Khalili, I.J.Thompson, J.A.Tostevin

Evaluation of an Eikonal Model for 11Li-Nucleus Elastic Scattering

NUCLEAR REACTIONS 12C, 40Ca, 208Pb(11Li, 11Li), E=30-600 MeV/nucleon; 12C(11Li, 11Li'), E=637 MeV; calculated σ(θ). Eikonal model.

doi: 10.1016/0375-9474(94)00432-M
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1995TH04      Nucl.Phys. A588, 59c (1995)

I.J.Thompson, J.S.Al-Khalili, J.M.Bang, B.V.Danilin, V.D.Efros, F.M.Nunes, J.S.Vaagen, M.V.Zhukov, and the Russian-Nordic-British Theory (RNBT) Collaboration

Structure and Reactions of the Li and Be Halo Nuclei

NUCLEAR REACTIONS 12C(14Be, 14Be), (12Be, 12Be), E=57 MeV/nucleon; analyzed data; deduced rms matter radius role. Glauber, optical models.

NUCLEAR STRUCTURE 11Li, 11,12,14Be; analyzed halo characteristics; deduced intruder state role. 14Be; calculated binding energies, rms radii, selected channels weights, Serber widths.

doi: 10.1016/0375-9474(95)00099-M
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1994AL02      Phys.Rev. C49, 386 (1994)

J.S.Al-Khalili, J.A.Tostevin

Dynamic Polarization Potential for 11Li Scattering

NUCLEAR REACTIONS 12C(11Li, 11Li), E=637 MeV; calculated dynamic polarization potential parameters. Glauber few-body model.

doi: 10.1103/PhysRevC.49.386
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1993AL05      J.Phys.(London) G19, 403 (1993)

J.S.Al-Khalili, M.B.Barbaro, C.Wilkin

An Analysis of Eta-Production via the p6Li → (Eta)7Be Reaction

NUCLEAR REACTIONS 6Li(p, π+), E=201-800 MeV; 6Li(p, d), E=698 MeV; 7Li(p, d), E=800 MeV; analyzed data; deduced empirical form factors, extrapolation to eta-production point in 6Li+p reaction. Semi-phenomenological model.

doi: 10.1088/0954-3899/19/3/008
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1993TH01      Phys.Rev. C47, R1364 (1993)

I.J.Thompson, J.S.Al-Khalili, J.A.Tostevin, J.M.Bang

Quasielastic Scattering of 11Li using Realistic Three-Body Wave Functions

NUCLEAR REACTIONS 12C(11Li, 11Li), (11Li, X), E=60 MeV/nucleon; calculated elastic, quasielastic σ(θ). Realistic three-body wave functions, four-body Glauber approximation.

doi: 10.1103/PhysRevC.47.R1364
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1992AL10      Nucl.Phys. A546, 622 (1992)

J.S.Al-Khalili, R.C.Johnson

A Three-Body Glauber Model for Polarized Deuteron Scattering at Intermediate Energies

NUCLEAR REACTIONS 58Ni(polarized d, d), E=400, 700 MeV; calculated σ(θ), vector, tensor analyzing power vs θ. Parameter free Glauber model.

doi: 10.1016/0375-9474(92)90548-X
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1990AL01      Phys.Rev. C41, R806 (1990)

J.S.Al-Khalili, J.A.Tostevin, R.C.Johnson

Effects of Singlet Breakup on Deuteron Elastic Scattering at Intermediate Energies

NUCLEAR REACTIONS 58Ni(polarized d, d), E=400 MeV; calculated σ(θ), tensor analyzing power; deduced singlet breakup contribution.

doi: 10.1103/PhysRevC.41.R806
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1990AL18      Nucl.Phys. A513, 43 (1990)

J.S.Al-Khalili, E.D.Cooper

An Alternative Non-Relativistic Optical Potential Parameterization for the Proton-Nucleus Interaction

NUCLEAR REACTIONS 40Ca(p, p), E=200, 350 MeV; calculated potential parameters, Perey factor vs r. 40Ca(d, d), E=400, 700 MeV; calculated local equivalent potential parameters vs r. 58Ni(polarized d, d), E=400, 700 MeV; calculated σ(θ), analyzing power vs θ. Nonlocal parametrization.

doi: 10.1016/0375-9474(90)90341-I
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1990AL26      Nucl.Phys. A514, 649 (1990)

J.S.Al-Khalili, J.A.Tostevin, R.C.Johnson

Singlet Channel Coupling in Deuteron Elastic Scattering at Intermediate Energies

NUCLEAR REACTIONS 58Ni(polarized d, d), E=200-700 MeV; calculated σ(θ), analyzing power, rotation parameter vs θ.

doi: 10.1016/0375-9474(90)90015-E
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1990AL37      Phys.Lett. 252B, 327 (1990)

J.S.Al-Khalili

Application of the Cluster-Folding Model to Polarised 6Li Scattering at Intermediate Energies

NUCLEAR REACTIONS 40Ca(polarized d, d), E=700 MeV; analyzed σ(θ), analyzing power vs θ. 40Ca(α, α), E=1.37 GeV; calculated σ(θ); deduced model parameters. 40Ca(polarized 6Li, 6Li), E=2.1 GeV; analyzed σ(θ), vector, tensor analyzing power data. Schrodinger equivalent Dirac optical potentials, α+d cluster model.

doi: 10.1016/0370-2693(90)90546-I
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1988AL15      J.Phys.(London) G14, L103 (1988)

J.S.Al-Khalili, J.A.Tostevin, R.C.Johnson, M.Kawai

The Momentum-Dependent T(p) Tensor Interaction in Intermediate-Energy Deuteron Scattering

NUCLEAR REACTIONS 58Ni(polarized d, d), E=400 MeV; calculated tensor analyzing power vs θ, potential form factors. Pauli-induced breakup.

doi: 10.1088/0305-4616/14/5/007
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