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NSR database version of April 27, 2024.

Search: Author = F.D.Santos

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2004BR08      Phys.Rev. C 69, 024608 (2004)

B.Braizinha, C.R.Brune, A.M.Eiro, B.M.Fisher, H.J.Karwowski, D.S.Leonard, E.J.Ludwig, F.D.Santos, I.J.Thompson

Resonant and direct components in the ³He(d, p)⁴He reaction at low energies

NUCLEAR REACTIONS ³He(polarized d, p), E=0.52, 0.89, 1.49 MeV; measured σ(θ=0°), analyzing power; deduced scattering matrix elements.

doi: 10.1103/PhysRevC.69.024608
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0978.

2001BR23      Nucl.Phys. A689, 369c (2001)

B.Braizinha, A.M.Eiro, F.D.Santos

The ¹²C(α, γ)¹⁶O Reaction at Astrophysical Energies

NUCLEAR REACTIONS ¹²C(α, γ), E(cm)=0-4 MeV; analyzed astrophysical S-factor, multipole components; deduced parameters, resonance contributions.

doi: 10.1016/S0375-9474(01)00857-0
Citations: PlumX Metrics

2000HE12      J.Phys.(London) G26, 1217 (2000)

J.Henriques de Jesus, J.P.Pinto, F.D.Santos

Effects of Variable Nucleon Energy in the Relativistic Analysis of Deuteron-Nucleus Scattering

NUCLEAR REACTIONS ²⁴Mg, ⁴⁰Ca, ⁵⁸Ni(d, d), E=200, 400, 700 MeV; calculated σ(θ), vector and tensor analyzing powers; deduced effects of variable nucleon-nucleus interaction energy. Comparisons with data.

doi: 10.1088/0954-3899/26/8/309
Citations: PlumX Metrics

1999PI16      Europhys.Lett. 47, 668 (1999)

J.P.Pinto, A.Amorim, F.D.Santos

Relativistic Deuteron Structure Function at Large Q²

NUCLEAR STRUCTURE ²H; calculated deep inelastic unpolarized structure function.

doi: 10.1209/epl/i1999-00441-9
Citations: PlumX Metrics

1999VE11      Phys.Rev. C60, 064003 (1999)

K.D.Veal, C.R.Brune, W.H.Geist, H.J.Karwowski, E.J.Ludwig, E.E.Bartosz, P.D.Cathers, T.L.Drummer, K.W.Kemper, A.M.Eiro, F.D.Santos, B.Kozlowska, H.J.Maier, I.J.Thompson

Determination of the Asymptotic D- to S-State Ratio for ⁶Li via (⁶Li(pol), d) Transfer Reactions

NUCLEAR REACTIONS ⁴⁰Ca, ⁵⁸Ni(polarized ⁶Li, d), E=34 MeV; measured deuteron spectra, σ(E, θ), Ay(θ), tensor analyzing powers. ⁶Li deduced asymptotic D- to S-state ratio. DWBA analysis.

doi: 10.1103/PhysRevC.60.064003
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0607.

1998VE03      Phys.Rev.Lett. 81, 1187 (1998)

K.D.Veal, C.R.Brune, W.H.Geist, H.J.Karwowski, E.J.Ludwig, A.J.Mendez, E.E.Bartosz, P.D.Cathers, T.L.Drummer, K.W.Kemper, A.M.Eiro, F.D.Santos, B.Kozlowska, H.J.Maier, I.J.Thompson

Deformation Effects in ⁶Li

NUCLEAR REACTIONS ⁵⁸Ni(polarized ⁶Li, d), E=34 MeV; analyzed σ(θ), A(y)(θ), A(zz)(θ), A(xz)(θ). ⁶Li deduced asymptototic D- to S-state ratio. DWBA analysis.

doi: 10.1103/PhysRevLett.81.1187
Citations: PlumX Metrics

1997PI05      Phys.Rev. C55, 2577 (1997)

J.P.Pinto, F.D.Santos, A.Amorim

Eikonal Approximation to Deuteron-Nucleus Scattering at Intermediate Energies

NUCLEAR REACTIONS ⁴⁰Ca(polarized d, d), E=700 MeV; analyzed σ(θ), tensor analyzing power vs θ. Eikonal approximation, integral representation.

doi: 10.1103/PhysRevC.55.2577
Citations: PlumX Metrics

1996PI02      Phys.Rev. C53, 2376 (1996)

J.P.Pinto, A.Amorim, F.D.Santos

Microscopic Relativistic Model for Deuteron-Nucleus Scattering

NUCLEAR REACTIONS ⁴⁰Ca(polarized d, d), E=400, 700 MeV; analyzed σ(θ), vector, tensor analyzing power vs θ. Microscopic relativistic model.

doi: 10.1103/PhysRevC.53.2376
Citations: PlumX Metrics

1994SA18      Phys.Lett. 325B, 267 (1994)

F.D.Santos, A.Arriaga

Full Determination of Transition Matrix Elements in the d(pol)(p(pol), pp)n Reaction

NUCLEAR REACTIONS ²H(polarized p, 2p), E not given; calculated transition matrix elements; deduced d helicity amplitudes dependence. Collinear geometry.

doi: 10.1016/0370-2693(94)90008-6
Citations: PlumX Metrics

1993CR01      Phys.Rev. C47, 2690 (1993)

E.R.Crosson, S.K.Lemieux, E.J.Ludwig, W.J.Thompson, M.Bisenberger, R.Hertenberger, D.Hofer, H.Kader, P.Schiemenz, G.Graw, A.M.Eiro, F.D.Santos

Probing α-Particle Wave Functions Using (d(pol), α) Reactions

NUCLEAR REACTIONS ⁵⁰Ti, ⁵⁸Ni(polarized d, α), E=16, 22 MeV; measured σ(θ), vector, tensor analyzing power vs θ; deduced α-particle D-state role. Exact finite-range DWBA analysis.

doi: 10.1103/PhysRevC.47.2690
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1993CR04      Phys.Rev. C48, 1770 (1993)

E.R.Crosson, E.J.Ludwig, M.Bisenberger, R.Hertenberger, D.Hofer, H.Kader, P.Schiemenz, G.Graw, A.M.Eiro, F.D.Santos, B.A.Brown

Configuration Mixing in ⁵⁶Co and ⁴⁶Sc Using (d(pol), α) Reactions

NUCLEAR REACTIONS ⁵⁸Ni, ⁴⁸Ti(polarized d, α), E=22 MeV; measured σ(θ), analyzing power vs θ. ⁵⁶Co, ⁴⁶Sc levels deduced L-mixing ratios.

doi: 10.1103/PhysRevC.48.1770
Citations: PlumX Metrics

1992AM05      Phys.Lett. 297B, 31 (1992)

A.Amorim, F.D.Santos

Relativistic Impulse Approximation for Deuteron Scattering

NUCLEAR REACTIONS ⁴⁰Ca(polarized d, d), E=700 MeV; analyzed σ(θ), vector, tensor analyzing power vs θ. Relativistic impulse approximation.

doi: 10.1016/0370-2693(92)91064-G
Citations: PlumX Metrics

1992CR01      Phys.Rev. C45, R492 (1992)

E.R.Crosson, R.K.Das, S.K.Lemieux, E.J.Ludwig, W.J.Thompson, M.Bisenberger, R.Hertenberger, D.Hofer, H.Kader, P.Schiemenz, G.Graw, A.M.Eiro, F.D.Santos

Probing α-Particle Wave Functions by (d, α) Tensor Analyzing Powers

NUCLEAR REACTIONS ⁵⁸Ni(polarized d, α), E=22 MeV; ⁵⁰Ti(polarized d, α), E=16 MeV; measured σ(θ), analyzing power vs θ; deduced optical model parameters. ⁴He deduced D-state parameters. DWBA analysis, realistic interactions.

doi: 10.1103/PhysRevC.45.R492
Citations: PlumX Metrics

1991AM01      Phys.Rev. C44, 2100 (1991)

A.Amorim, F.D.Santos

From Dirac Phenomenology to Deutron-Nucleus Elastic Scattering at Intermediate Energies

NUCLEAR REACTIONS ⁵⁸Ni, ⁴⁰Ca(polarized d, d), E=400, 700 MeV; analyzed σ(θ), vector analyzing power vs θ. Global nucleon-nucleus Dirac optical potentials.

doi: 10.1103/PhysRevC.44.2100
Citations: PlumX Metrics

1990EI01      J.Phys.(London) G16, 1139 (1990)

A.M.Eiro, F.D.Santos

Non-Spherical Components of Light Nuclei

NUCLEAR REACTIONS, ICPND ²H(polarized d, γ), E=0.8-14.7 MeV; compiled astrophysical S-factor vs E other data analyses. ⁴⁰Ca, ³¹P(d, t), ⁴⁰Ca, ³¹P, ⁴He(d, ³He), E not given; ²⁰⁸Pb(polarized d, t), E=12.3 MeV; ²⁰⁸Pb(polarized d, p), E=9 MeV; ⁹⁰Zr(polarized d, p), E=5.5 MeV; ¹¹⁹Sn(polarized d, t), E=12 MeV; ⁸⁹Y(d, α), E not given; compiled data analyses. ^2,3H, ^3,4He deduced D-state components method dependence.

doi: 10.1088/0954-3899/16/8/010
Citations: PlumX Metrics

1990LU10      J.Phys.(Paris), Colloq.C-6, 439 (1990)

E.J.Ludwig, C.M.Bhat, T.B.Clegg, E.R.Crosson, H.J.Karwowski, G.Graw, P.Schiemenz, R.Hertenberger, H.Kader, D.Hofer, M.Bisenberger, A.M.Eiro, F.D.Santos

D-State Parameter Determinations for ³He and ⁴He

NUCLEAR REACTIONS ³²S(polarized d, ³He), E=16 MeV; ⁵⁸Ni(polarized d, α), E=22 MeV; measured σ(θ), analyzing power vs θ. ^3,4He deduced asymptotic D- to S-state ratio, D₂ parameter.

1990SA40      J.Phys.(London) G16, 1909 (1990)

F.D.Santos

Large Entrance Channel Spin-2 Amplitudes in the ⁶Li(d, α)⁴He Reaction

NUCLEAR REACTIONS ⁶Li(polarized d, α), E=8-10 MeV; analyzed tensor analyzing power features; deduced mechanisms for large spin-2 amplitude generation.

doi: 10.1088/0954-3899/16/12/015
Citations: PlumX Metrics

1990SA47      J.Phys.(Paris), Colloq.C-6, 443 (1990)

F.D.Santos, I.J.Thompson, A.M.Eiro

⁶Li D-State Effects in the ⁶Li(d(pol), α)⁴He Reaction

NUCLEAR REACTIONS ⁶Li(polarized d, α), E=10 MeV; analyzed tensor analyzing power data. ⁶Li deduced D-state component.

1989CR01      Phys.Rev. C39, 305 (1989)

R.Crespo, A.M.Eiro, F.D.Santos

D-State Effects in the Radiative Capture Reaction d + α → ⁶Li + γ

NUCLEAR REACTIONS, ICPND ⁴He(polarized d, γ), E(cm) ≈ 2-10 MeV; calculated σ(θ), capture σ(E), tensor analyzing power vs θ; deduced ⁶Li D-state role. Direct capture model.

doi: 10.1103/PhysRevC.39.305
Citations: PlumX Metrics

1989CR04      J.Phys.(London) G15, 637 (1989)

R.Crespo, F.D.Santos

Medium Effects in Deuteron Elastic Scattering

NUCLEAR REACTIONS ²⁰⁸Pb(polarized d, d), E=56 MeV; analyzed σ(θ), polarization observables vs θ; deduced medium effects role. Brueckner-Hartree-Fock calculations of optical model.

doi: 10.1088/0954-3899/15/5/016
Citations: PlumX Metrics

1989SA17      J.Phys.(London) G15, 1275 (1989)

F.D.Santos, J.L.Yun

The ²H(d, γ)⁴He Reaction and Primordial Nucleosynthesis

NUCLEAR REACTIONS ²H(d, γ), E not given; analyzed reaction rate; deduced influence on light element abundances in early universe.

doi: 10.1088/0954-3899/15/8/022
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1988AR11      Phys.Rev. C37, 2312 (1988)

A.Arriaga, A.M.Eiro, F.D.Santos, J.E.Ribeiro

²H(d, γ)⁴He Reaction from a Microscopic Point of View

NUCLEAR REACTIONS ²H(d, γ), (polarized d, γ), E=1-15 MeV; calculated σ(θ), tensor analyzing power; deduced deuteron D-state effects role. ⁴He deduced asymptotic D/S state ratio.

doi: 10.1103/PhysRevC.37.2312
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1988PI01      Phys.Rev. C37, 1 (1988)

W.K.Pitts, H.O.Meyer, L.C.Bland, J.D.Brown, R.C.Byrd, M.Hugi, H.J.Karwowski, P.Schwandt, A.Sinha, J.Sowinski, I.J.van Heerden, A.Arriaga, F.D.Santos

¹H(d(pol), γ)³He Reaction at E(d) = 95 MeV

NUCLEAR REACTIONS, MECPD ¹H(polarized d, γ), E=95 MeV; measured σ(θ), analyzing power vs θ. ³He deduced D- to S- state asymptotic normalization ratio.

doi: 10.1103/PhysRevC.37.1
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0625.

1986KA27      Nucl.Phys. A457, 15 (1986)

B.C.Karp, E.J.Ludwig, J.E.Bowsher, B.L.Burks, T.B.Clegg, F.D.Santos, A.M.Eiro

Alpha-Particle D-State and Configuration-Mixing Effects in the ⁸⁹Y(d, α)⁸⁷Sr Reaction

NUCLEAR REACTIONS ⁸⁹Y(polarized d, α), E=9, 12, 16 MeV; measured σ(θ), vector, tensor analyzing power vs θ. ⁸⁹Y(polarized d, d), E=12 MeV; measured σ(θ), vector analyzing power vs θ. ⁸⁷Sr(α, α), E=19.5 MeV; measured σ(θ). ⁸⁷Sr levels deduced L, J, configuration mixing, α-particle D-state parameter. Finite range DWBA.

doi: 10.1016/0375-9474(86)90517-8
Citations: PlumX Metrics

1986SA16      Phys.Lett. 175B, 110 (1986)

F.D.Santos

Relativistic Spin-1 Dynamics and Deuteron-Nucleus Elastic Scattering

NUCLEAR REACTIONS ²H(p, p), (n, n), E not given; analyzed elastic scattering processes; deduced spin-orbit potential model dependence. Dirac approach compared to folding model.

doi: 10.1016/0370-2693(86)90697-0
Citations: PlumX Metrics

1986WE07      Phys.Rev. C34, 32 (1986)

H.R.Weller, P.Colby, J.Langenbrunner, Z.D.Huang, D.R.Tilley, F.D.Santos, A.Arriaga, A.M.Eiro

⁴He D-State Effects in the ²H(d, γ)⁴He Reaction at Low Energies

NUCLEAR REACTIONS, ICPND ²H(d, γ), E=0.7-14.9 MeV; measured Eγ, Iγ, γ(θ), σ(E). ⁴He deduced asymptotic D-to-S state ratio.

doi: 10.1103/PhysRevC.34.32
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0387.

1985SA04      Phys.Rev. C31, 707 (1985)

F.D.Santos, A.Arriaga, A.M.Eiro, J.A.Tostevin

⁴He D-State Effects in the ²H(d(pol), γ)⁴He Reaction

NUCLEAR REACTIONS ²H(polarized d, γ), E=9.7 MeV; calculated tensor analyzing power vs θ; deduced D-state role. ⁴He deduced D- to S-state ratio. Wave function input from resonating group phase shifts.

doi: 10.1103/PhysRevC.31.707
Citations: PlumX Metrics

1985SA18      Phys.Rev. C32, 338 (1985)

F.D.Santos, B.C.Karp, J.E.Bowsher, E.J.Ludwig, A.M.Eiro

Determination of Two-Nucleon Spectroscopic Amplitudes from (d, α) Analyzing Powers

NUCLEAR REACTIONS ⁸⁹Y(d, α), E=9, 12, 16 MeV; measured σ(θ), vector, tensor analyzing power vs θ. ⁸⁷Sr levels deduced L, J, mixing amplitudes. Finite-range DWBA, S-, D-state admixture, neutron, proton configurations involved.

doi: 10.1103/PhysRevC.32.338
Citations: PlumX Metrics

1984AR07      Phys.Rev. C29, 1945 (1984)

A.Arriaga, F.D.Santos

³He D-State Effects in the ¹H(d(pol), γ)³He Reaction

NUCLEAR REACTIONS ¹H(polarized d, γ), E ≈ 1-20 MeV; calculated tensor analyzing power vs θ. ³He deduced asymptotic, D-to S-state ratio.

doi: 10.1103/PhysRevC.29.1945
Citations: PlumX Metrics

1984KA33      Phys.Rev.Lett. 53, 1619 (1984)

B.C.Karp, E.J.Ludwig, W.J.Thompson, F.D.Santos

α-Particle D-State Components from (d, α) Analyzing Powers

NUCLEAR REACTIONS ⁸⁹Y(polarized d, α), E=9, 12, 16 MeV; measured σ(θ), analyzing power vs θ. ⁴He deduced D-state parameter. Exact finite-range DWBA analysis.

doi: 10.1103/PhysRevLett.53.1619
Citations: PlumX Metrics

1983SA42      Prog.Theor.Phys.(Kyoto) 70, 1679 (1983)

F.D.Santos

L Mixing and D-State Effects in (d, α) Reactions

NUCLEAR REACTIONS ³⁶Ar, ³²S(polarized d, α), E=16 MeV; calculated vector, tensor analyzing power vs θ; deduced sensitivity to α-particle D-state effects. ³⁴Cl, ³⁰P levels deduced L-mixing effects. DWBA method.

doi: 10.1143/PTP.70.1679
Citations: PlumX Metrics

1982SA12      Phys.Rev. C25, 3243 (1982)

F.D.Santos, S.A.Tonsfeldt, T.B.Clegg, E.J.Ludwig, Y.Tagishi, J.F.Wilkerson

α-Particle D-State Effects in (d, α) Reactions

NUCLEAR REACTIONS ³²S, ^36,38Ar(polarized d, α), E=16 MeV; analyzed tensor analyzing power data ; deduced α-particle D-state effects. DWBA, Jackson-Riska model D-to S-state ratio.

doi: 10.1103/PhysRevC.25.3243
Citations: PlumX Metrics

1981LI23      Phys.Rev. C24, 1852 (1981)

P.W.Lisowski, R.C.Byrd, G.Mack, W.Tornow, R.L.Walter, T.B.Clegg, F.D.Santos

Polarization Transfer in (d(pol), n(pol)) Reactions on Light Nuclei at θ = 0°

NUCLEAR REACTIONS ¹²C, ¹⁴N, ¹⁶O, ²⁸Si(polarized d, n), E=5-15 MeV; measured polarization transfer. ¹²C(d, n), E=6-14 MeV; measured σ(θ=0°). DWBA analysis.

doi: 10.1103/PhysRevC.24.1852
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1415.

1981SA16      Phys.Lett. 101B, 219 (1981)

F.D.Santos, A.M.Goncalves

Analyzing Powers of Heavy Ion Induced Transfer Reactions

NUCLEAR REACTIONS ⁵⁸Ni(polarized ⁷Li, ⁶Li), E=20.3 MeV; analyzed σ(θ), iT₁₁(θ). Semiclassical model, DWBA analysis.

doi: 10.1016/0370-2693(81)90298-7
Citations: PlumX Metrics

1981SA20      Phys.Rev. C24, 156 (1981)

F.D.Santos, A.M.Goncalves

Strong j-Dependent Effects in (⁷Li(pol), ⁶Li) Reactions

NUCLEAR REACTIONS ⁵⁸Ni(polarized ⁷Li, ⁶Li), E=20.3 MeV; calculated σ(θ), vector, tensor analyzing power vs θ; deduced j-dependent effects. DWBA analysis.

doi: 10.1103/PhysRevC.24.156
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1981SA27      Phys.Rev. C24, 1379 (1981)

F.D.Santos

Coulomb Effects on Charged Particle Exchange Singularities

NUCLEAR REACTIONS ^1,3H, ³He(d, d), E=0-60 MeV; calculated exchange amplitude Coulomb correction factor. ³H, ³He deduced asymptotic D- to S-state ratio.

doi: 10.1103/PhysRevC.24.1379
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1979SA02      Phys.Rev. C19, 238 (1979)

F.D.Santos, A.M.Eiro, A.Barroso

N + d Clustering of Three-Nucleon Systems: D-State Effects in (d, t) and (d, ³He) Reactions

NUCLEAR STRUCTURE ³H; calculated S, D states of overlap integral with d; deduced zero-range normalization constant, D-state parameter for (d, t), (d, ³He).

doi: 10.1103/PhysRevC.19.238
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1977RO17      Nucl.Phys. A289, 269 (1977)

S.Roman, A.K.Basak, J.B.A.England, J.M.Nelson, N.E.Sanderson, F.D.Santos, A.M.Eiro

³He D-State Effects in (d, ³He) Reactions

NUCLEAR REACTIONS ²⁷Al(polarized d, ³He), E=12.4 MeV; measured iT₁₁, T₂₀, T₂₂(θ); deduced ³He d-state contribution. Natural target.

doi: 10.1016/0375-9474(77)90032-X
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1976SA04      Phys.Rev. C13, 1145 (1976)

F.D.Santos

1- and j-Dependent Effect in (d, p) Reactions

NUCLEAR REACTIONS ¹²C, ¹⁶O, ⁴⁰Ca, ⁵²Cr, ²⁸Si, ⁹⁰Zr, ⁵⁴Fe(polarized d, p), E=6-13.3 MeV; calculated A(θ). Surface reaction model.

doi: 10.1103/PhysRevC.13.1145
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1975KN07      Phys.Rev.Lett. 35, 1570 (1975)

L.D.Knutson, B.P.Hichwa, A.Barroso, A.M.Eiro, F.D.Santos, R.C.Johnson

Effects of the Triton D State in (d, t) Reactions

NUCLEAR REACTIONS ¹¹⁸Sn(d, t), E=12.0 MeV; ²⁰⁸Pb(d, t), E=12.3 MeV; measured polarization parameters T₂₀, T₂₁, T₂₂.

doi: 10.1103/PhysRevLett.35.1570
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1974SA11      Phys.Lett. 51B, 14 (1974)

F.D.Santos

Transparency to Vector Polarization Transfer in Deuteron Stripping Reactions

NUCLEAR REACTIONS ¹²C, ⁴⁰Ca(d, p); calculated P(θ).

doi: 10.1016/0370-2693(74)90138-5
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1974SA20      Nucl.Phys. A236, 90 (1974)

F.D.Santos

Polarization Transfer in Deuteron Stripping Reactions

NUCLEAR REACTIONS ¹²C, ²⁴Mg, ²⁸Si, ⁴⁰Ca(polarized d, p), E=12.3 MeV; calculated P(θ).

doi: 10.1016/0375-9474(74)90223-1
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1973JO10      Nucl.Phys. A208, 221 (1973)

R.C.Johnson, F.D.Santos, R.C.Brown, A.A.Debenham, G.W.Greenlees, J.A.R.Griffith, O.Karban, D.C.Kocher, S.Roman

Vector and Tensor Analysing Power of (d, p) Reactions and Deuteron D-State Effects

NUCLEAR REACTIONS ⁹Be, ¹²C, ¹⁶O, ¹⁹F, ²⁵Mg, ²⁸Si, ⁴⁰Ca(polarized d, p), E=12.3 MeV; measured analyzing powers iT₁₁(θ), T₂₀(θ), T₂₂(θ), deduced importance of d-state effects. ¹⁰Be, ¹³C, ¹⁷O, ²⁰F, ²⁶Mg, ²⁹Si, ⁴¹Ca deduced level J. Enriched ²⁵Mg, ⁴⁰Ca targets.

doi: 10.1016/0375-9474(73)90371-0
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1971JO22      Particles Nucl. 2, 285 (1971)

R.C.Johnson, F.D.Santos

Deuteron D-State Effects in (d, p) and (p, d) Reactions

NUCLEAR REACTIONS ⁴⁰Ca, ⁸⁸Sr(d, p), E=12, 11 MeV; ¹⁶O, ⁴⁸Ca, ⁵⁶Fe(p, d), E=30, 18, 18.5 MeV; ²⁰⁶Pb, ²⁸Si, ^50,52Cr(d, p), ⁹⁰Zr(d, p), E=10, 13, 7.5, 8.0, 15 MeV; ⁶⁶Zn(d, n), E=10 MeV; ¹¹⁶Sn, ¹¹⁴Sn(p, d), E=30, 20.7 MeV; analyzed σ(θ), d-state deuteron effects.DWBA.