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2000MB01      Eur.Phys.J. A 9, 313 (2000)

G.Mairle, P.Grabmayr

A Phenomenological Spin-Orbit and Nuclear Potential for ²⁰⁸Pb

NUCLEAR STRUCTURE ^207,208,209Pb, ²⁰⁷Tl, ²⁰⁹Bi; calculated single particle levels, mean field densities, radii; deduced optical model potential for ²⁰⁸Pb. Comparison with experimental values. Role of spin-orbit term discussed.

NUCLEAR REACTIONS ²⁰⁸Pb(d, ³He), (d, t), (³He, d), (d, p), E=20-52 MeV; calculated σ(θ), spectroscopic factors. DWBA calculations.

doi: 10.1007/s100500070016
Citations: PlumX Metrics

1995MA16      Z.Phys. A350, 285 (1995)

G.Mairle

The Shape of the Nuclear Spin-Orbit Potential

NUCLEAR STRUCTURE ²⁰⁸Pb; calculated proton, neutron spin-orbit potentials.

doi: 10.1007/BF01291184
Citations: PlumX Metrics

1993MA16      Phys.Rev. C47, 2113 (1993)

G.Mairle, M.Seeger, M.Ermer, P.Grabmayr, A.Mondry, G.J.Wagner

Global Properties of Proton-Hole Strengths in Mass 54 to 70 Nuclei

NUCLEAR REACTIONS ⁶⁶Zn(polarized d, ³He), E=52 MeV; measured σ(θ), iT₁₁(θ); deduced model parameters. ⁶⁵Cu deduced levels, J, π, C²S.

NUCLEAR STRUCTURE ^54,56,58Fe, ^58,60,62,64Ni, ^64,66Zn, ⁷⁰Ge; calculated proton Fermi surface parameters.

doi: 10.1103/PhysRevC.47.2113
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1993MA18      Phys.Lett. 304B, 39 (1993)

G.Mairle

Scaling of Measured Nuclear Spin-Orbit Splittings

NUCLEAR STRUCTURE ¹²C, ¹⁶O, ^40,48Ca, ⁹⁰Zr, ¹¹⁶Sn, ¹⁴⁰Ce, ¹⁴⁴Sm, ²⁰⁸Pb; A ≤ 200; analyzed proton-, neutron spin-orbit splittings; deduced scaling.

doi: 10.1016/0370-2693(93)91396-5
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1993MA50      Nucl.Phys. A565, 543 (1993)

G.Mairle, M.Seeger, H.Reinhardt, T.Kihm, K.T.Knopfle, C.L.Wen

The Distribution of Proton-Hole Strengths in the (2s, 1d)-Shell of ³⁵Cl, ³⁷Cl and ³⁹Cl

NUCLEAR REACTIONS ^36,38,40Ar(polarized d, ³He), E=52 MeV; measured σ(θ), iT₁₁(θ). ^35,37,39Cl deduced levels, J, π, spectroscopic factors, proton occupancies, single-particle energies, spreading widths. ³⁹Cl deduced mass excess. Enriched ^36,38Ar gas targets. DWBA analysis.

doi: 10.1016/0375-9474(93)90044-X
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1992MA28      Nucl.Phys. A543, 558 (1992)

G.Mairle, M.Seeger, M.Ermer, P.Grabmayr, A.Mondry, G.J.Wagner

The ⁶⁰Ni(d(pol), ³He)⁵⁹Co Reaction and the Proton Strengths Distributions in Even Nickel Isotopes

NUCLEAR REACTIONS ⁶⁰Ni(polarized d, ³He), E=52 MeV; measured σ(θ), iT₁₁(θ). ⁵⁹Co deduced levels, J, π, spectroscopic factors. ^58,60,62,64Ni deduced proton occupation numbers, single-particle energies, spreading widths. Different proton stripping, pick-up experiments data analyzed. DWBA analysis. Enriched ⁶⁰Ni target.

doi: 10.1016/0375-9474(92)90279-S
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1992SE03      Nucl.Phys. A539, 223 (1992)

M.Seeger, Th.Kihm, K.T.Knopfle, G.Mairle, U.Schmidt-Rohr

Study of Proton Hole States in ⁶³Cu and ⁶³Co (II). The γ-Decay of Proton Hole States

NUCLEAR REACTIONS ⁶⁴Zn, ⁶⁴Ni(d, ³He), E=31 MeV; measured (³He)γ-coin, DSA. ⁶³Cu, ⁶³Co deduced levels, γ-branching, T_1/2. Enriched targets, Ge(Li) detectors. Phonon-hole model calculations.

doi: 10.1016/0375-9474(92)90268-O
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1991SE09      Nucl.Phys. A533, 1 (1991)

M.Seeger, Th.Kihm, K.T.Knopfle, G.Mairle, U.Schmidt-Rohr, J.Hebenstreit, D.Paul, P.von Rossen

Study of Proton-Hole States in ⁶³Cu and ⁶³Co (I). Spectroscopy of (d, ³He) Reactions at E(d) = 52 MeV

NUCLEAR REACTIONS ⁶⁴Zn, ⁶⁴Ni(d, ³He), (polarized d, ³He), E=52 MeV; measured σ(E(³He)), σ(θ), iT₁₁(θ). ⁶³Cu, ⁶³Co deduced levels, J, π, spectroscopic factors. Enriched target. Parametrized 2s_1/2 proton single-particle energies for 16 ≤ A ≤ 66.

doi: 10.1016/0375-9474(91)90817-P
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1990WA16      Yad.Fiz. 51, 1521 (1990); Sov.J.Nucl.Phys. 51, 959 (1990)

G.Wagner, P.Grabmayr, M.V.Evlanov, T.Kim, K.Knopfle, G.Mairle, V.M.Pugach, G.Siegert

Energy and Angle Correlations of Products of the Reactions of ²⁸Si(⁶Li, αc)X at Energy 156 MeV

NUCLEAR REACTIONS ²⁸Si(⁶Li, αX), E=156 MeV; measured σ(θα, Eα, fragment θ) for X=α, p, d, t, ³He; deduced reaction mechanism. Quasifree scattering model.

1988KH04      Nucl.Phys. A481, 253 (1988)

S.Khan, G.Mairle, K.T.Knopfle, Th.Kihm, L.-K.Pao, P.Grabmayr, G.J.Wagner, L.Friedrich

Hole-Strength Distributions from the ³⁴S(d(pol), ³He)³³P and ³⁴S(d(pol), t)³³S Reactions

NUCLEAR REACTIONS ³⁴S(polarized d, ³He), (polarized d, t), E=52 MeV; measured σ(θ), iT₁₁(θ); deduced systematics of single particle states for A=28-40. ³³P, ³³S deduced levels, J, π, T, spectroscopic factors, occupation numbers summed (S⁺), (S^-) Gamow-Teller strength. Enriched target.

doi: 10.1016/0375-9474(88)90496-4
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1988MA53      Nucl.Phys. A490, 371 (1988)

G.Mairle, K.T.Knopfle, M.Seeger

Total Gamow-Teller Strengths from Measured Ground-State Correlations

NUCLEAR REACTIONS ^16,18O, ^20,22Ne, ^24,26Mg, ^28,30Si, ^36,38,40Ar, ^{40,42,44,46,48}Ca, ^46,48,50Ti, ^52,54Cr, ⁵⁴Fe, ⁵⁸Ni, ⁹⁰Zr(p, n), (n, p); analyzed one-nucleon transfer σ data; deduced ground-state occupation numbers, total Gamow-Teller strengths.

doi: 10.1016/0375-9474(88)90511-8
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1987GR21      Nucl.Phys. A469, 285 (1987)

P.Grabmayr, G.Mairle, U.Schmidt-Rohr, G.P.A.Berg, J.Meissburger, P.von Rossen, J.L.Tain

Proton Particle-Hole States in ²⁰⁸Pb

NUCLEAR REACTIONS ²⁰⁹Bi(d, ³He), ²⁰⁸Pb(d, ³He), E=45 MeV; measured σ(θ). ²⁰⁸Pb deduced levels, J, π, L, C²S. Enriched targets. DWBA analysis.

doi: 10.1016/0375-9474(87)90111-4
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1987NU01      Nucl.Phys. A465, 365 (1987)

J.Nurzynski, T.Kihm, K.T.Knopfle, G.Mairle, H.Clement

Reorientation Effects for 52 MeV Vector Polarized Deuterons

NUCLEAR REACTIONS ^20,22Ne, ²⁶Mg, ²⁸Si, ^32,34S, ^36,40Ar(polarized d, d), (polarized d, d'), E=52 MeV; measured σ(θ), iT₁₁(θ); deduced optical model parameters. ^20,22Ne, ²⁶Mg, ²⁸Si, ^32,34S, ^36,40Ar levels deduced β₂. Natural ²⁸Si, ³²S, ⁴⁰Ar targets, ^20,22Ne, ²⁶Mg, ³⁴S, ³⁶Ar enriched targets.

doi: 10.1016/0375-9474(87)90353-8
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1987PU02      Izv.Akad.Nauk SSSR, Ser.Fiz. 51, 1904 (1987); Bull.Acad.Sci.USSR, Phys.Ser. 51, No.11, 27 (1987)

V.M.Pugach, V.A.Kiva, W.Wagner, V.Bechtold, P.Grabmayr, G.Zigert, T.Kim, G.Mairle, L.Friedrich

Determination of Spin of the Deep-Lying Proton-Hole States in the Reaction ⁵⁸Ni(d(pol), ³He)⁵⁷Co

NUCLEAR REACTIONS ⁵⁸Ni(polarized d, ³He), E=52 MeV; measured σ(E(³He), θ(³He)), analyzing power. ⁵⁷Co levels deduced possible J. Enriched target, ΔE-E telescope.

1986MA55      Z.Phys. A325, 243 (1986)

G.Mairle, P.Grabmayr

Experimental Constraints on Size and Phase of Proton and Neutron Contributions to the Isoscalar 1⁺ State in ²⁰⁸Pb

NUCLEAR REACTIONS ²⁰⁹Bi(d, ³He), E=45 MeV; measured σ(E(³He)), σ(θ). ²⁰⁸Pb deduced level, J, π, C²S, neutron, proton size, phase contributions to isoscalar B(M1).

1986PF01      Nucl.Phys. A455, 381 (1986)

A.Pfeiffer, G.Mairle, K.T.Knopfle, T.Kihm, G.Seegert, P.Grabmayr, G.J.Wagner, V.Bechtold, L.Friedrich

Study of the (d(pol), ³He) Reaction on ⁸⁴Kr and ⁸⁶Kr and the Lowest Moments of the Proton Strength Distributions in the Zr Region

NUCLEAR REACTIONS ^84,86Kr(polarized d, ³He), E=52 MeV; measured σ(θ), iT₁₁(θ). ^83,85Br levels deduced J, π. ^84,86Kr, ^86,88Sr, ^90,92,94,96Zr, ^{92,94,96,98,100}Mo; analyzed data; deduced single particle energy, spreading width systematics.

doi: 10.1016/0375-9474(86)90313-1
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0827.

1985KH04      Phys.Lett. 156B, 155 (1985)

S.Khan, Th.Kihm, K.T.Knopfle, G.Mairle, V.Bechtold, L.Friedrich

The Mass of ³⁵P and Spin-Parity Assignments for Excited ³⁵P States

NUCLEAR REACTIONS ³⁶S(d, ³He), (polarized d, ³He), E=52 MeV; measured σ(E(³He)), σ(θ), iT₁₁(θ). ³⁵P deduced mass excess, levels, J, π, C²S.

doi: 10.1016/0370-2693(85)91499-6
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1985MA46      Z.Phys. A322, 173 (1985)

G.Mairle

Systematic Properties of Proton Single-Particle Energies

NUCLEAR STRUCTURE A=30-100; calculated proton single particle energies. Proton pickup, stripping data input.

doi: 10.1007/BF01412033
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1984KI11      Z.Phys. A318, 205 (1984)

T.Kihm, G.Mairle, P.Grabmayr, K.T.Knopfle, G.J.Wagner, V.Bechtold, L.Friedrich

Spins and Parities of Hole States in ²⁵Na and ²⁵Mg

NUCLEAR REACTIONS ²⁶Mg(polarized d, ³He), (d, ³He), (d, t), E=52 MeV; measured σ(θ), σ(E(³He)), σ(Et). ²⁵Na deduced levels, J, π, C²S. ²⁵Mg deduced IAS, J, π, S. Local, zero-range DWBA analysis.

doi: 10.1007/BF01413470
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1984SE13      J.Phys.(Paris), Colloq.C4, 85 (1984); See 1984Se21

G.Seegert, A.Pfeiffer, P.Grabmayr, T.Kihm, K.T.Knopfle, G.Mairle, G.J.Wagner, V.Bechtold, L.Friedrich

Study of Deeply-Bound Hole States in the Zr-Region via the (d(pol), ³He) Reaction

1984SE21      J.Phys.(Paris), Colloq.C-4, 85 (1984)

G.Seegert, A.Pfeiffer, P.Grabmayr, T.Kihm, K.T.Knopfle, G.Mairle, G.J.Wagner, V.Bechtold, L.Friedrich

Study of Deeply-Bound Hole States in the Zr-Region via the (d(pol), ³He) Reaction

NUCLEAR REACTIONS ⁸⁶Kr, ^90,92Zr, ⁹²Mo(polarized d, ³He), E=52 MeV; measured σ(E(³He), θ(³He)), σ(θ(³He)). ⁸⁶Kr, ^90,92Zr, ⁹²Mo deduced 1f_7/2 hole state centroid energies, average Γ, spectroscopic factors. ⁸⁵Br deduced 1f_7/2 strength distribution.

1984WA19      Yad.Fiz. 40, 1396 (1984)

G.Wagner, A.Vdovin, P.Grabmayr, T.Kim, G.Mairle, V.Pugach, G.Siegert, Ch.Stoyanov

Fragmentation of Deep Hole States in the Reaction ⁵⁸Ni(d, ³He)⁵⁷Co at Deuteron Energy 52 MeV

NUCLEAR REACTIONS ⁵⁸Ni(d, ³He), E=52 MeV; measured σ(θ); deduced optical model parameters. ⁵⁷Co levels deduced S, d_3/2, d_5/2 single particle strength functions, deep hole state fragmentation.

1983MA07      Phys.Lett. 121B 307 (1983); Priv.Comm. (February 1983)

G.Mairle, K.Schindler, P.Grabmayr, G.J.Wagner, U.Schmidt-Rohr, G.A.P.Berg, W.Hurlimann, S.A.Martin, J.Meissburger, J.G.H.Romer, B.Styczen, J.L.Tain

Spectroscopic Results from a High-Resolution Study of Proton Particle-Hole States in ²⁰⁸Pb

NUCLEAR REACTIONS ²⁰⁹Bi(d, ³He), E=45 MeV; measured σ(θ), σ(E(³He)). ²⁰⁸Pb levels deduced J, π, C²S, configuration. High resolution magnetic spectrometer. Local, zero-range DWBA analysis.

doi: 10.1016/0370-2693(83)91375-8
Citations: PlumX Metrics

1982MA25      Nucl.Phys. A382, 173 (1982)

G.Mairle, G.J.Wagner, P.Grabmayr, K.T.Knopfle, Liu Ken Pao, H.Riedesel, K.Schindler, V.Bechtold, L.Friedrich, P.Ziegler

Spin Determination of States with Stretched Configurations in ¹⁶N and ³²P Via the (d(pol), α) Reaction at 52 Mev

NUCLEAR REACTIONS ¹²C, ¹⁸O, ³⁴S(polarized d, α), E=52 MeV; measured σ(θ), iT₁₁(θ). ³²P, ¹⁶N deduced levels, J, π. Enriched targets.

doi: 10.1016/0375-9474(82)90130-0
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1981MA14      Nucl.Phys. A363, 413 (1981)

G.Mairle, G.J.Wagner, K.T.Knopfle, Liu Ken Pao, H.Riedesel, V.Bechtold, L.Friedrich

Deformation of 1p Shells in (2s, 1d) Shell Nuclei from a Systematic Study of (d(pol), ³He) Reactions

NUCLEAR REACTIONS ¹²C, ¹⁴N, ^16,18O, ²²Ne, ²⁸Si(polarized d, ³He); E=52 MeV; measured iT₁₁(E(³He), θ). ¹⁷N, ¹⁷O, ²¹F, ²¹Ne deduced levels, J, π, S. Enriched targets. DWBA, Nilsson model analyses.

doi: 10.1016/0375-9474(81)90266-9
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1981MA24      Z.Phys. A301, 157 (1981)

G.Mairle, Liu Ken Pao, G.J.Wagner, K.T.Knopfle, H.Riedesel

A Comparative Spectroscopic Investigation of ²¹Ne and ²¹F by Pickup Reactions

NUCLEAR REACTIONS ²²Ne(d, t), (d, ³He), E=52 MeV; measured σ(θ, Et), σ(θ, E(³He)). ²¹Ne, ²¹F deduced levels, L, J, π, T, S. Enriched target. DWBA analysis.

doi: 10.1007/BF01419246
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1980MA10      Nucl.Phys. A339, 61 (1980)

G.Mairle, K.T.Knopfle, H.Riedesel, G.J.Wagner, V.Bechtold, L.Friedrich

The Optical Potential for Vector-Polarized Deuterons of 52 MeV

NUCLEAR REACTIONS ¹²C, ¹⁶O, ²⁰Ne, ²⁸Si, ³²S, ⁴⁰Ar, ⁵⁸Ni, ⁹⁰Zr, ¹⁹⁷Au(polarized d, d), E=52 MeV; measured iT₁₁(θ); deduced optical model parameters. Enriched targets.

doi: 10.1016/0375-9474(80)90242-0
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1980ST28      Z.Phys. A297, 307 (1980)

A.Stuirbrink, G.J.Wagner, K.T.Knopfle, L.K.Pao, G.Mairle, H.Riedesel, K.Schindler, V.Bechtold, L.Friedrich

Spin Determination of Deeply-Bound Hole States from (d(pol), ³He) Reactions

NUCLEAR REACTIONS ⁹⁰Zr(polarized d, ³He), E=52 MeV; measured σ(θ). ⁸⁹Y levels deduced L, j-transfer, C²S, configuration.

doi: 10.1007/BF01422789
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1979DO06      Phys.Lett. 82B, 357 (1979)

P.Doll, G.J.Wagner, H.Breuer, K.T.Knopfle, G.Mairle, H.Riedesel

Strong Exhaustion of 1g₉/₂ Strength by Deeply-Bound Proton-Hole States in Pm Isotopes

NUCLEAR REACTIONS ^144,148,152Sm(d, ³He), E=52 MeV; measured σ(E(³He), θ). ^143,147,151Pm deduced level, L, C²S, J-transfer. Local, zero-range DWBA calculations.

doi: 10.1016/0370-2693(79)90241-7
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1979DO12      J.Phys.(London) G5, 1421 (1979)

P.Doll, G.Mairle, H.Breuer, K.T.Knopfle, T.Tohei, G.J.Wagner

On Positive-Parity States of ⁴⁵Sc, ⁴⁷Sc and ⁴⁹Sc

NUCLEAR REACTIONS ^46,48,50Ti(d, ³He), E=52 MeV; measured σ(E(³He), θ). ^45,47,49Sc deduced levels, 2s-, 1d-hole strength distributions. Enriched targets.

doi: 10.1088/0305-4616/5/10/017
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1978BE14      Phys.Lett. 72B, 169 (1978); see also 77Be70

V.Bechtold, L.Friedrich, P.Doll, K.T.Knopfle, G.Mairle, G.J.Wagner

Spins of Proton Hole States from Analyzing Powers of (d, γ) Reactions at 52 MeV

NUCLEAR REACTIONS ¹⁶O, ²⁸Si, ⁴⁰Ca(polarized d, ³He), E=52 MeV; measured A(θ), σ(θ). ¹⁵N, ²⁷Al, ³⁹K levels deduced J.

doi: 10.1016/0370-2693(77)90693-1
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1978MA16      Nucl.Phys. A299, 39 (1978)

G.Mairle, G.J.Wagner, P.Doll, K.T.Knopfle, H.Breuer

The Particle-Hole Spectra of ¹⁶O and ¹⁶N as Observed in Pick-up Reactions from ¹⁷O

NUCLEAR REACTIONS ¹⁷O(d, t), (d, ³He), E=52 MeV; measured σ(θ). ¹⁶O, ¹⁶N deduced levels, L, J, π, T, S. Enriched targets.

doi: 10.1016/0375-9474(78)90207-5
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1978RI03      Phys.Rev.Lett. 41, 377 (1978)

H.Riedesel, K.T.Knopfle, H.Breuer, P.Doll, G.Mairle, G.J.Wagner

Is There an Isoscalar 'Giant' Quadrupole Resonance in ¹²C (Question)

NUCLEAR REACTIONS ¹²C(α, α'), (α, 2α), (α, pα), E=104 MeV; measured σ, αα(θ), pα(θ). ¹²C giant resonance region deduced E2 strength.

doi: 10.1103/PhysRevLett.41.377
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1977BE70      Phys.Lett. 72B, 169 (1977)

V.Bechtold, L.Friedrich, P.Doll, K.T.Knopfle, G.Mairle, G.J.Wagner

Spins of Proton Hole States from Analyzing Powers of (d, τ) Reactions at 52 MeV

NUCLEAR REACTIONS ¹⁶O, ²⁸Si, ⁴⁰Ca(polarized d, ³He), E=52 MeV; measured A(θ), σ(θ). ¹⁵N, ²⁷Al, ³⁹K levels deduced J.

doi: 10.1016/0370-2693(77)90693-1
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1977MA10      Nucl.Phys. A280, 97 (1977)

G.Mairle, K.T.Knopfle, P.Doll, J.Breuer, G.J.Wagner

The (d, t) and (d, τ) Reactions on ¹⁸O and the 1p Spin-Orbit Splitting

NUCLEAR REACTIONS ¹⁸O(d, t), ¹⁸O(d, ³He), E=52 MeV; measured σ(Et, θ)σ(E(³He), θ). ¹⁷O, ¹⁷N deduced levels, L, J, π, T, S. Enriched target.

doi: 10.1016/0375-9474(77)90296-2
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1977WA11      Phys.Rev. C16, 1271 (1977)

G.J.Wagner, K.T.Knopfle, G.Mairle, P.Doll, H.Hafner, J.L.C.Ford, Jr.

Strong Effect of Isospin Mixing in ¹⁶O

NUCLEAR REACTIONS ¹⁷O(d, ³He), (d, t), E=52 MeV; ¹⁷O(³He, α), E=36 MeV; measured σ(θ); deduced relative population of states. ¹⁶O levels deduced T-mixing.

doi: 10.1103/PhysRevC.16.1271
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1976DO05      Nucl.Phys. A263, 210 (1976)

P.Doll, G.J.Wagner, K.T.Knopfle, G.Mairle

The Quasihole Aspect of Hole Strength Distribution in Odd Potassium and Calcium Isotopes

NUCLEAR REACTIONS ^40,42,44,48Ca(d, ³He), ^40,44Ca(d, t), E=52 MeV; measured σ(θ). ^39,41,43,47K, ^39,43Ca deduced levels, J, π, L, T_1/2, S. Enriched targets.

doi: 10.1016/0375-9474(76)90169-X
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1975HS01      Nucl.Phys. A243, 380 (1975)

S.T.Hsieh, K.T.Knopfle, G.Mairle, G.J.Wagner

The Spectra of Mass 15, 16 and 17 Nuclei

NUCLEAR STRUCTURE ^15,16,17O; calculated levels. ¹⁵N, ^15,16,17O; calculated S. ¹⁵O, ¹⁵N, ¹⁶O; calculated γ-width.

doi: 10.1016/0375-9474(75)90285-7
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1975MA41      Nucl.Phys. A253, 253 (1975)

G.Mairle, G.J.Wagner

The Decrease of Ground-State Correlations from ¹²C to ¹⁴C

NUCLEAR REACTIONS ^12,13,14C(d, ³He), E=52 MeV; measured σ(E(³He), θ). ^11,12,13B deduced levels, spectroscopic factors. Enriched ^13,14C targets.

doi: 10.1016/0375-9474(75)90480-7
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1975SC41      Z.Phys. A275, 241 (1975)

U.Schwinn, G.Mairle, G.J.Wagner, C.Ramer

Proton Pick-up from Nuclei in the Middle of the 1p Shell

NUCLEAR REACTIONS ⁹Be, ^10,11B(d, ³He), E=52 MeV; measured σ(E(³He), θ). ⁸Li, ^9,10Be levels deduced S. ¹⁰Be deduced level.

doi: 10.1007/BF01409291
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1975WA17      Phys.Lett. 57B, 413 (1975)

G.J.Wagner, P.Doll, K.T.Knopfle, G.Mairle

Lifetime of Nuclear Hole States Caused by Phonon-Hole Coupling

NUCLEAR REACTIONS ^36,38,40Ar, ^40,42,44,48Ca(d, ³He), E=52 MeV; measured σ(E(³He), θ). ^35,37,39Cl, ^39,41,43,47K levels deduced spreading width.

doi: 10.1016/0370-2693(75)90256-7
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1974DO12      Nucl.Phys. A230, 329 (1974)

P.Doll, H.Mackh, G.Mairle, G.J.Wagner

Comparative Spectroscopy with the (d, τ) Reaction on Even Ar Isotopes

NUCLEAR REACTIONS ^36,38Ar(d, ³He), E=52 MeV; measured σ(E(³He), θ). ^35,37Cl deduced levels, S, J, π. Enriched targets.

doi: 10.1016/0375-9474(74)90311-X
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1974KN07      Nucl.Phys. A233, 317 (1974)

K.T.Knopfle, P.Doll, G.Mairle, G.J.Wagner

Investigation of 1p-2h States in ³⁹K with the ³⁸Ar(³He, d)³⁹K Reaction

NUCLEAR REACTIONS ³⁸Ar(³He, d), E=24 MeV; measured σ(E(³He), θ). ³⁹K deduced levels, L, π, J, T, S. Enriched ³⁸Ar target.

doi: 10.1016/0375-9474(74)90459-X
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1974MA23      Phys.Lett. 50B, 252 (1974)

G.Mairle, G.J.Wagner

1p Hole-States in ¹⁶O and ¹⁶N and the Mass Dependence of the 1p Spin-Orbit Splitting

NUCLEAR REACTIONS ¹⁷O(d, t), (d, ³He), E=52 MeV; measured σ(E, Et, θ), σ(E, E(³He), θ). ¹⁶O, ¹⁶N deduced levels, t, J, π, S.

doi: 10.1016/0370-2693(74)90552-8
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1974MA34      Z.Phys. 269, 353 (1974)

H.Mackh, G.Mairle, G.J.Wagner

Proton Shell Structure of Mass 28-32 Nuclei

NUCLEAR REACTIONS ^28,29,30Si, ³¹P, ³²S(d, ³He), E=52 MeV; measured σ(E(³He), θ). ^27,28,29Al, ³⁰Si, ³¹P levels deduced L, S.

doi: 10.1007/BF01668607
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1973MA21      Z.Phys. 258, 321 (1973)

G.Mairle, G.J.Wagner

On Mirror States of Negative Parity in Mass 15 Nuclei

NUCLEAR REACTIONS ¹⁶O(d, ³He), (d, t), E=52 MeV; measured σ(E(³He), Et, θ). ¹⁵N, ¹⁵O deduced levels, J, π.

doi: 10.1007/BF01392441
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1972MA33      Z.Phys. 251, 404 (1972)

G.Mairle, G.J.Wagner

The ⁴⁶Ti(d, τ)⁴⁵Sc Reaction. Evidence for f₅/₂ Single Proton Configurations in the Ground State of ⁴⁶Ti

NUCLEAR REACTIONS ⁴⁶Ti(d, ³He), E=52 MeV; measured σ(E(³He), θ). ⁴⁵Sc deduced levels, J, π, S.

doi: 10.1007/BF01391734
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1971HA48      Z.Phys. 246, 418 (1971)

D.Hartwig, G.T.Kaschl, G.Mairle, G.J.Wagner

A Study of ¹⁷N Levels and T=3/2 Multiplets in Mass 17 Nuclei

NUCLEAR REACTIONS ¹⁸O(d, ³He), E=52 MeV; measured σ(E(³He), θ). ¹⁷N deduced levels, L(p), J, π.

doi: 10.1007/BF02115806
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1971KA35      Nucl.Phys. A178, 275 (1971)

G.Kaschl, G.Mairle, H.Mackh, D.Hartwig, U.Schwinn

The ¹⁵N(d, tau)¹⁴C Reaction and High-Lying T = 1 States in Mass-14 Nuclei: A Determination of 1p²₁/₂ and 1p₁/₂1p₁/₂ Diagonal Matrix Elements

NUCLEAR REACTIONS ¹⁵N(d, ³He), E=52 MeV; measured σ(E(³He), θ). ¹⁴C deduced levels, L, J, π, S. Enriched target.

doi: 10.1016/0375-9474(71)90205-3
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1971KR04      Nucl.Phys. A165, 353 (1971)

E.Kramer, G.Mairle, G.Kaschl

Proton Pick-up from the Magnesium Isotopes: ^24,25,26Mg(d, t)^23,24,25Na

NUCLEAR REACTIONS ^24,25,26Mg(d, ³He), E=52 MeV; measured σ(θ). ^23,24,25Na deduced levels, J, L, π, S. Enriched ²⁴Mg, ²⁵Mg, ²⁶Mg targets.

doi: 10.1016/0375-9474(71)90765-2
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1970KA31      Nucl.Phys. A155, 417 (1970)

G.T.Kaschl, G.J.Wagner, G.Mairle, U.Schmidt-Rohr

Proton Pick-up from ¹⁹F, ²⁰Ne and ²²Ne

NUCLEAR REACTIONS ¹⁹F, ^20,22Ne(d, ³He), E=52 MeV; measured σ(E(³He), θ). ¹⁸O, ^19,21F deduced levels, L, J, π, S. Enriched Ne targets.

doi: 10.1016/0375-9474(70)90904-8
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF1131.

1969KA22      Nucl.Phys. A136, 286 (1969)

G.T.Kaschl, G.Mairle, U.Schmidt-Rohr, G.J.Wagner, P.Turek

Proton Pick-up from the 2s-1d and 1p Shells of ³²S

NUCLEAR REACTIONS ³²S(d, ³He) ³¹P, E = 52 MeV; measured σ(E(³He), θ). ³¹P deduced levels J, π, L(p), S.

doi: 10.1016/0375-9474(69)90054-2
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1969MA26      Nucl.Phys. A134, 180 (1969)

G.Mairle, G.T.Kaschl, H.Link, H.Mackh, U.Schmidt-Rohr, G.J.Wagner, P.Turek

Proton Separation Energies Derived from the (d, ³He) Reaction on f-p Shell Nuclei at 52 MeV

NUCLEAR REACTIONS ⁴⁵Sc, ⁵⁴Fe, ^58,60Ni, ^63,65Cu(d, ³He), E = 52 MeV; measured σ(E(³He), θ). ⁴⁴Ca, ⁵³Mn, ^57,59Co, ^62,64Ni deduced levels, L, J, π, S. Enriched targets.

doi: 10.1016/0375-9474(69)90691-5
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1969WA01      Nucl.Phys. A125, 80(1969)

G.J.Wagner, G.Mairle, U.Schmidt-Rohr, P.Turek

Proton Pick-up from the 1p and 2s-1d Shells of ²⁷Al

NUCLEAR REACTIONS ²⁷Al(d, ³He)²⁶Mg, Ed=52 MeV; measured σ(E(³He), θ). ²⁶Mg deduced levels, S.

doi: 10.1016/0375-9474(69)90830-6
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1969WA03      Nucl.Phys. A129, 469 (1969)

G.J.Wagner, G.T.Kaschl, G.Mairle, U.Schmidt-Rohr, P.Turek

Levels of ³⁹Cl Studied by the ⁴⁰Ar(d, ³He)³⁹Cl Reaction at 52 MeV

NUCLEAR REACTIONS ⁴⁰Ar(d, ³He), E=52 MeV; measured σ(E(³He), θ). ³⁹Cl deduced levels, L, J, π. Natural target.

doi: 10.1016/0375-9474(69)90680-0
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1262.

1968HI01      Nucl.Phys. A106, 161 (1968)

F.Hinterberger, G.Mairle, U.Schmidt-Rohr, P.Turek, G.J.Wagner

Single Nucleon Pick-up from ¹²C and ¹⁴N with 52 MeV Deuterons

NUCLEAR REACTIONS ¹⁴N(d, ³He), ¹⁴N(d, t), ¹²C(d, ³He), E = 52 MeV; measured σ(E(³He), θ), σ(Et, θ). ¹¹B, ¹³C, ¹³N deduced levels, J, π, S. Natural targets.

doi: 10.1016/0375-9474(67)90835-4
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1968HI09      Nucl.Phys. A115, 570 (1968)

F.Hinterberger, G.Mairle, U.Schmidt-Rohr, G.J.Wagner, P.Turek

Inelastic Scattering of 52 MeV Deuterons

NUCLEAR REACTIONS ¹²C, ¹⁴N, ^20,22Ne, ²⁷Al, ²⁸Si, ³²S, ⁴⁰Ar, ⁴⁸Ti, ⁵⁴Fe, ^58,64Ni, ²⁰⁸Pb, ²⁰⁹Bi(d, d'), E = 52 MeV; measured σ(Ed, θ). ¹²C, ¹⁴N, ^20,22Ne, ²⁷Al, ²⁸Si, ³²S, ⁴⁰Ar, ⁴⁸Ti, ⁵⁴Fe, ^58,64Ni, ²⁰⁸Pb, ²⁰⁹Bi deduced deformation parameters β(L). Enriched targets.

doi: 10.1016/0375-9474(68)90750-1
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1968HI14      Nucl.Phys. A111, 265 (1968)

F.Hinterberger, G.Mairle, U.Schmidt-Rohr, G.J.Wagner, P.Turek

Elastic scattering of 52 MeV deuterons

NUCLEAR REACTIONS ¹H(d, d), ³He(d, d), ⁴He(d, d), ¹²C(d, d), ¹⁴N(d, d), ¹⁶O(d, d), ²⁰Ne(d, d), ²²Ne(d, d), ²⁴Mg(d, d), ²⁷Al(d, d), ²⁸Si(d, d), ³²S(d, d), ⁴⁰Ar(d, d), ⁴⁸Ti(d, d), ⁵⁰Ti(d, d), ⁵⁴Fe(d, d), ⁵⁸Ni(d, d), ⁶⁴Ni(d, d), ⁸⁹Y(d, d), ⁹³Nb(d, d), ¹⁰³Rh(d, d), ¹⁴⁰Ce(d, d), ¹⁸¹Ta(d, d), ¹⁹⁷Au(d, d), ²⁰⁸Pb(d, d), ²⁰⁹Bi(d, d), ²³⁸U(d, d), E=52 MeV; measured products, Eπ, Iπ; deduced σ(θ). Data were imported from EXFOR entry D0225.

doi: 10.1016/0375-9474(68)90122-X
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0225.

1967HI09      Z.Physik 202, 236 (1967)

F.Hinterberger, G.Mairle, U.Schmidt-Rohr, P.Turek, G.J.Wagner

Shell Structure Studies in the Titanium Region with 52 MeV Deuterons

NUCLEAR REACTIONS ⁴⁸Ti(d, d'), E=52 MeV; ^48,50Ti, ⁵¹V(d, ³He), E=52 MeV; measured σ(θ), σ(E(³He), θ). ^47,49Sc, ⁵⁰Ti deduced levels, L, J, π, S.

doi: 10.1007/BF01331212
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1966DU03      Z.Naturforsch. 21a, 969 (1966)

B.Duelli, G.Mairle, U.Schmidt-Rohr, P.Turek, G.Wagner

Kernreaktionen durch Deuteronen von 52 MeV

NUCLEAR STRUCTURE ¹⁰⁴Rh, ⁹²Nb, ⁸⁹Y, ⁹⁰Y, ¹⁰³Rh, ¹⁰²Rh, ¹⁹⁸Au; measured not abstracted; deduced nuclear properties.

1966DU08      Phys.Letters 23, 485 (1966)

B.Duelli, F.Hinterberger, G.Mairle, U.Schmidt-Rohr, P.Turek, G.Wagner

Elastic Scattering of 52 MeV Deuterons

NUCLEAR REACTIONS ¹²C, ¹⁶O, ²⁴Mg, ²⁸Si, ^48,50Ti, ⁶⁴Ni, ⁸⁹Y, ⁹³Nb, ¹⁰³Rh, ¹⁴⁰Ce, ¹⁸¹Ta, ¹⁹⁷Au, ²⁰⁸Pb, ²⁰⁹Bi, ²³⁸U(d, d), E=52 MeV; measured σ(θ); deduced optical model parameters.

doi: 10.1016/0031-9163(66)90784-0
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1965JA13      Nucl.Phys. 70, 383 (1965)

R.Jahr, G.Mairle

Elastic and Inelastic Scattering of Deuterons on Ne, Ar and Kr

NUCLEAR REACTIONS Ne, Kr(d, d'), E = 11.6 MeV; Ar(d, d'), E = 10.6, 11.6 MeV; measured σ(E, θ). ⁴⁰Ar deduced levels, J, π. Natural targets.

doi: 10.1016/0029-5582(65)90534-1
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