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1994SA52      Nucl.Instrum.Methods Phys.Res. A337, 387 (1994)

P.Savard, L.-A.Hamel, J.-P.Martin, P.Taras

An a-Si:H gas microstrip detector

RADIOACTIVITY 55Fe(EC); measured K X-ray spectra; deduced detector resolution features. An a-Si:H gas microstrip detector.

doi: 10.1016/0168-9002(94)91107-X
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1993HA19      Nucl.Phys. A561, 251 (1993)

B.Haas, V.P.Janzen, D.Ward, H.R.Andrews, D.C.Radford, D.Prevost, J.A.Kuehner, A.Omar, J.C.Waddington, T.E.Drake, A.Galindo-Uribarri, G.Zwartz, S.Flibotte, P.Taras, I.Ragnarsson

Studies of Superdeformation in the Gadolinium Nuclei

NUCLEAR REACTIONS 120,122,124Sn(28Si, xn), (29Si, xn), (30Si, xn), E=155 MeV; measured Eγ, Iγ, γγ-coin, DCO ratios. 145,146,147,148,149Gd deduced, γ-multipliplicities, J, π, levels, superdeformed bands. Compton-suppressed hyperpure Ge detector array, 4π-bismuth germanate ball. Cranked shell-model-Strutinsky calculations.

doi: 10.1016/0375-9474(93)90153-O
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1992RA17      Nucl.Phys. A545, 665 (1992)

D.C.Radford, H.R.Andrews, G.C.Ball, D.Horn, D.Ward, F.Banville, S.Flibotte, S.Monaro, S.Pilotte, P.Taras, J.K.Johansson, D.Tucker, J.C.Waddington, M.A.Riley, G.B.Hagemann, I.Hamamoto

Multiple Band Structure and Band Termination in 157Ho Towards Complete High-Spin Spectroscopy

NUCLEAR REACTIONS 124Sn(37Cl, 4n), E=155, 165 MeV; measured Eγ, γγ-coin, Iγ(θ, φ). 157Ho deduced levels, Iγ, J, π, rotational band characteristics, band-mixing interaction strengths.

doi: 10.1016/0375-9474(92)90298-X
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1992VI03      Phys.Lett. 278B, 407 (1992)

J.P.Vivien, D.Balouka, B.Haas, H.R.Andrews, D.C.Radford, D.Ward, V.P.Janzen, D.Prevost, J.C.Waddington, S.Flibotte, S.Pilotte, P.Taras, A.Galindo-Uribarri, H.Kluge, S.Aberg

Radiation Originating from Unresolved Superdeformed States in 149Gd

NUCLEAR REACTIONS 124Sn(30Si, xn), E=155 MeV; measured correlated γγ-coincidence matrix, Iγ. 149Gd deduced unresolved superdeformed states.

doi: 10.1016/0370-2693(92)90576-P
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1991FL02      Nucl.Phys. A530, 187 (1991)

S.Flibotte, B.Haas, F.Banville, J.Gascon, P.Taras, H.R.Andrews, D.C.Radford, D.Ward, J.C.Waddington

High-Spin States in 149Gd

NUCLEAR REACTIONS 124Sn(30Si, 5n), E=150 MeV; measured Eγ, Iγ, γγ-coin, Iγ(θ), oriented nuclei. 149Gd deduced levels, J, δ. Enriched targets, Compton-suppressed hyperpure Ge detector array, 4π BGO ball. Deformed Woods-Saxon potential calculations.

doi: 10.1016/0375-9474(91)90762-U
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1991FL03      Nucl.Phys. A531, 205 (1991)

S.Flibotte, B.Haas, P.Taras, H.R.Andrews, D.C.Radford, D.Ward

Spin Dependence of the Giant Dipole Resonance in Gd Isotopes

NUCLEAR REACTIONS 124Sn(30Si, xn), E=150 MeV; measured Eγ, Iγ, γγ-coin, spin orientation, γ(θ). 148,149,150Gd deduced deformation. Enriched targets, Compton-suppressed hyperpure Ge detector array, 4π BGO ball.

doi: 10.1016/0375-9474(91)90578-T
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1991WA20      Nucl.Phys. A529, 315 (1991)

D.Ward, V.P.Janzen, H.R.Andrews, D.C.Radford, G.C.Ball, D.Horn, J.C.Waddington, J.K.Johansson, F.Banville, J.Gascon, S.Monaro, N.Nadon, S.Pilotte, D.Prevost, P.Taras, R.Wyss

Gamma-Ray Spectroscopy of 126Ba

NUCLEAR REACTIONS 96Zr(34S, 4n), E=155 MeV; 116Sn(13C, 3n), E=56 MeV; measured Eγ, Iγ, γγ-coin, Iγ-spin orientation correlation, DCO ratios. 126Ba deduced levels, J, δ. Enriched targets, Compton-suppressed hyperpure Ge detector array, 4π-bismuth germanate ball. Cranked shell model calculations, total routhian surface calculations.

doi: 10.1016/0375-9474(91)90798-B
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1990HA25      Phys.Lett. 245B, 13 (1990)

B.Haas, J.P.Vivien, S.K.Basu, F.A.Beck, Ph.Benet, T.Byrski, D.Curien, G.Duchene, C.Gehringer, H.Kluge, J.C.Merdinger, P.Romain, D.Santos, S.Flibotte, J.Gascon, P.Taras, E.Bozek, K.Zuber

Feeding of the Superdeformed Yrast Band in 149Gd

NUCLEAR REACTIONS 124Sn(30Si, 5n), E=150-160 MeV; measured γ-spectra. 149Gd deduced superdeformed yrast band relative Iγ.

doi: 10.1016/0370-2693(90)90156-Z
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1990HA31      Phys.Rev. C42, R1817 (1990)

B.Haas, D.Ward, H.R.Andrews, G.C.Ball, T.E.Drake, S.Flibotte, A.Galindo-Uribarri, V.P.Janzen, J.K.Johansson, H.Kluge, J.Kuehner, A.Omar, S.Pilotte, D.Prevost, J.Rodriguez, D.C.Radford, P.Taras, J.P.Vivien, J.C.Waddington, S.Aberg

Observation of Excited Proton and Neutron Configurations in the Superdeformed 149Gd Nucleus

NUCLEAR REACTIONS 124Sn(30Si, 5n), E=155 MeV; 124Sn(31P, 5n), E=156 MeV; measured γ-spectra, γγ-coin. 149Gd deduced levels, J, π, superdeformed band structure.

doi: 10.1103/PhysRevC.42.R1817
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1990PI11      Nucl.Phys. A514, 545 (1990)

S.Pilotte, S.Flibotte, S.Monaro, N.Nadon, D.Prevost, P.Taras, H.R.Andrews, D.Horn, V.P.Janzen, D.C.Radford, D.Ward, J.K.Johansson, J.C.Waddington, T.E.Drake, A.Galindo-Uribarri, R.Wyss

Rotational Bands and Shape Changes in 124Ba

NUCLEAR REACTIONS 94Zr(34S, 4n), E=145 MeV; 110Cd(16O, 2n), E=60 MeV; measured Eγ, Iγ, γγ-coin, Iγ(θ), oriented nuclei. 124Ba deduced levels, J, π, δ. Enriched target, Compton-suppressed Ge detector array, 4π bismuth germanate ball. Total routhian surface calculations, cranked shell-model.

doi: 10.1016/0375-9474(90)90155-F
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1989JO04      Phys.Rev.Lett. 63, 2200 (1989)

J.K.Johansson, H.R.Andrews, T.Bengtsson, A.Djaafri, T.E.Drake, S.Flibotte, A.Galindo-Uribarri, D.Horn, V.P.Janzen, J.A.Kuehner, S.Monaro, N.Nadon, S.Pilotte, D.Prevost, D.C.Radford, I.Ragnarsson, P.Taras, A.Tehami, J.C.Waddington, D.Ward, S.Aberg

Multiple Superdeformed Bands in 153Dy

NUCLEAR REACTIONS 124Sn(34S, 5n), E not given; measured γγγ-coin, sum spectra. 153Dy deduced levels, J, π, moment of inertia, band structure, deformation, superdeformation features.

doi: 10.1103/PhysRevLett.63.2200
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1989TA12      Phys.Lett. 222B, 357 (1989)

P.Taras, S.Flibotte, J.Gascon, B.Haas, S.Pilotte, D.C.Radford, D.Ward, H.R.Andrews, F.Banville, J.K.Johansson, J.C.Waddington

Additional Superdeformed States in the Continuum of 149Gd

NUCLEAR REACTIONS 124Sn(30Si, 5n), E=150 MeV; analyzed data. 149Gd deduced levels, J, π, superdeformation.

doi: 10.1016/0370-2693(89)90323-7
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1988GA03      Z.Phys. A329, 139 (1988)

J.Gascon, F.Beck, T.Byrski, G.Duchene, B.Haas, J.C.Merdinger, A.Nourreddine, P.Taras, J.P.Vivien

Moderately Deformed Bands in the Continuum of 144Gd

NUCLEAR REACTIONS 74Ge(72Ge, 2n), E=270 MeV; measured Eγ, Iγ, DSA. 144Gd deduced continuum band structure, transition γ-multipolarity, T1/2, J.


1988HA02      Phys.Rev.Lett. 60, 503 (1988)

B.Haas, P.Taras, S.Flibotte, F.Banville, J.Gascon, S.Cournoyer, S.Monaro, N.Nadon, D.Prevost, D.Thibault, J.K.Johansson, D.M.Tucker, J.C.Waddington, H.R.Andrews, G.C.Ball, D.Horn, D.C.Radford, D.Ward, C.St.Pierre, J.Dudek

Superdeformed Band up to Spin ≈ (127/2) in 149Gd

NUCLEAR REACTIONS 124Sn(30Si, 5n), E=150 MeV; measured Eγ, Iγ, Doppler shift fraction. 149Gd deduced levels, J, π, moment of inertia superdeformed band quadrupole moment.

doi: 10.1103/PhysRevLett.60.503
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1988RA19      Phys.Lett. 209B, 177 (1988)

G.-E.Rathke, R.V.F.Janssens, M.W.Drigert, I.Ahmad, K.Beard, R.R.Chasman, U.Garg, M.Hass, T.L.Khoo, H.-J.Korner, W.C.Ma, S.Pilotte, P.Taras, F.L.H.Wolfs

A Superdeformed Band in 151Dy

NUCLEAR REACTIONS 122Sn(34S, 5n), E=174.5 MeV; measured γγ-coin, γ multiplicity, Eγ, Iγ. 151Dy deduced levels, J, π, γ-branching, deformation, superdeformation features.

doi: 10.1016/0370-2693(88)90928-8
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1988TA20      Phys.Rev.Lett. 61, 1348 (1988)

P.Taras, S.Flibotte, J.Gascon, B.Haas, S.Pilotte, D.C.Radford, D.Ward, H.R.Andrews, G.C.Ball, F.Banville, S.Cournoyer, D.Horn, J.K.Johansson, S.Monaro, N.Nadon, D.Prevost, C.Pruneau, D.Thibault, D.M.Tucker, J.C.Waddington

Feeding of Discrete-Line Superdeformed Bands at Very High Spin

NUCLEAR REACTIONS 124Sn(30Si, 4n), (30Si, 5n), (30Si, 6n), (30Si, xn), E=140-160 MeV; measured γ yields, γ sum spectra, multiplicities. 149Gd deduced superdeformed band features.

doi: 10.1103/PhysRevLett.61.1348
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1987GA09      Nucl.Phys. A467, 539 (1987)

J.Gascon, P.Taras, D.C.Radford, D.Ward, H.R.Andrews, F.Banville

Change in Triaxiality in 159Tm

NUCLEAR REACTIONS 128Te(35Cl, xn), E=150 MeV; measured recoil distance, Eγ, Iγ. 158,159Tm deduced levels, J, π, T1/2, B(E2), B(M1), transition quandrupole moments, nuclear shape.

doi: 10.1016/0375-9474(87)90544-6
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1987GA12      Nucl.Phys. A470, 230 (1987)

J.Gascon, F.Banville, P.Taras, D.Ward, T.K.Alexander, H.R.Andrews, G.C.Ball, D.Horn, D.C.Radford, J.C.Waddington, A.Christy

Constant Transition Quadrupole Moments in 174Os up to Spin 20(h-bar)

NUCLEAR REACTIONS 51V(127I, 4n), E ≈ 610 MeV; measured Eγ, Iγ, recoil distance. 174Os deduced levels, J, π, T1/2, yrast level transition quadrupole moments, B(E2).

doi: 10.1016/0375-9474(87)90130-8
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1987GA14      Nucl.Phys. A472, 558 (1987)

J.Gascon, P.Taras, P.van Esbroek, H.R.Andrews, D.C.Radford, D.Ward, A.Christy

Shape Variations of 174W below the i13/2 Neutron Backbend

NUCLEAR REACTIONS 159Tb(19F, 4n), E=85 MeV; measured Eγ, Iγ, recoil distance. 174W deduced levels, T1/2, J, π, B(λ), transition quadrupole moment.

doi: 10.1016/0375-9474(87)90045-5
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1987NO06      Phys.Rev. C36, 2687 (1987)

A.Nourreddine, J.P.Vivien, F.A.Beck, T.Byrski, G.Duchene, C.Gehringer, B.Haas, J.C.Merdinger, J.Gascon, P.Taras

Simultaneous Population of Large and Small Deformation Bands at very High Spin in 152Dy

NUCLEAR REACTIONS 74Ge(80Se, 2n), E=285 MeV; 76Ge(80Se, 4n), E=320 MeV; measured DSA, Eγ, Iγ. 152Dy deduced levels, T1/2, high spin continuum states average quadrupole moment.

doi: 10.1103/PhysRevC.36.2687
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1986HA28      Nucl.Phys. A456, 317 (1986)

E.Hammaren, O.Hausser, H.R.Andrews, P.Taras, A.Larabee

136Xe(13C, 4nγ) Reaction Study of 145Nd

NUCLEAR REACTIONS 136Xe(13C, 4nγ), E=49-60 MeV; measured E(γ), I(γ)(E), I(γ)(θ), γγ-, energy-coin. 145Nd deduced levels, J, π. Pulsed beam, enriched solid 136Xe target, Ge(Li) detectors.

doi: 10.1016/0375-9474(86)90396-9
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1985HO17      Nucl.Phys. A441, 344 (1985)

D.Horn, I.S.Towner, O.Hausser, D.Ward, H.R.Andrews, M.A.Lone, J.F.Sharpey-Schafer, N.Rud, P.Taras

Single-Particle States at very High Spin in the Light Dysprosium Isotopes

NUCLEAR REACTIONS 124Sn(32S, xn), E=150, 163 MeV; measured γγ-coin, recoil distance. 150,151,152Dy deduced levels, J, π, T1/2, B(λ). Pulsed beam, Compton suppressed Ge(Li) detectors, NaI(Tl) array, plunger. Shell model, effective interactions.

NUCLEAR STRUCTURE 148,149,150,151,152Dy; calculated level, B(λ). Shell model, effective interactions.

doi: 10.1016/0375-9474(85)90037-5
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1985TA02      Nucl.Phys. A435, 294 (1985)

P.Taras, O.Hausser, H.R.Andrews, D.Ward, M.A.Deleplanque, R.M.Diamond, A.O.Macchiavelli, F.S.Stephens

Neutron Alignment at High Spin in 156Dy

NUCLEAR REACTIONS 24Mg(136Xe, 4n), E=600, 620 MeV; measured I(γ)(θ, H). 156Dy deduced average g. Enriched targets, transient field IMPAC technique.

doi: 10.1016/0375-9474(85)90315-X
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1984HA06      Nucl.Phys. A412, 141 (1984)

O.Hausser, H.R.Andrews, D.Horn, M.A.Lone, P.Taras, P.Skensved, R.M.Diamond, M.A.Deleplanque, E.L.Dines, A.O.Macchiavelli, F.S.Stephens

Transient Magnetic Fields for Large-Z Atoms Recoiling through Gadolinium

NUCLEAR REACTIONS 207Pb, 232Th, U(58Ni, 58Ni'), E=222, 230 MeV; 207Pb(136Xe, 136Xe'), E=610 MeV; measured γ(58Ni)-, γ(136Xe)-coin, Coulomb excitation, Iγ(θγ, H), transient field effect in 232Th, 238U at high spin; deduced 207Pb recoil transient magnetic field velocity dependence in Gd at 77(K). Transient field IMPAC technique.

doi: 10.1016/0375-9474(84)90389-0
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1984HA39      Phys.Lett. 144B, 341 (1984)

O.Hausser, D.Ward, H.R.Andrews, P.Taras, B.Haas, M.A.Deleplanque, R.M.Diamond, E.L.Dines, A.O.Macchiavelli, R.McDonald, F.S.Stephens, C.V.Stager

Spin Precession of Unresolved High-Spin States in 153-156Dy

NUCLEAR REACTIONS 26Mg(132Xe, xn), E=645 MeV; 24Mg(136Xe, xn), E=610 MeV; measured γγ-coin, summed spectra, γ(θ), oriented nuclei. 153,154,155,156Dy deduced high-spin collectivities, average g, γ-multiplicity. Fast Dy recoils in ferromagnetic gadolinium.

doi: 10.1016/0370-2693(84)91274-7
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1983HA24      Nucl.Phys. A406, 339 (1983)

O.Hausser, H.R.Andrews, D.Ward, N.Rud, P.Taras, R.Nicole, J.Keinonen, P.Skensved, C.V.Stager

Large Transient Magnetic Fields for Rare-Earth Ions Recoiling in Gadolinium and γ-Factors of High-Spin States in 156,158,160Gd

NUCLEAR REACTIONS 169Tm, Gd(34S, 34S'γ), E=58, 70, 80, 90, 100, 108, 115, 125, 130 MeV; 169Tm, Gd(63Cu, 63Cu'γ), E=230 MeV; measured (34S'γ)-, (63Cu'γ)-coin, Iγ(θ, H); deduced velocity dependence of transient magnetic field in Gd at 80 K. 156,158,160Gd levels deduced g. Ge(Li) detectors, natural targets, transient field IMPAC technique.

doi: 10.1016/0375-9474(83)90466-9
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1983HO09      Phys.Rev.Lett. 50, 1447 (1983)

D.Horn, O.Hausser, I.S.Towner, H.R.Andrews, M.A.Lone, P.Taras

Identification of Single-Particle Configurations at very High Spin in 150-152Dy

NUCLEAR STRUCTURE 148,149,150,151,152Dy; calculated levels, B(λ) ratios. Shell model.

NUCLEAR REACTIONS 124Sn(32S, xn), E=163 MeV; measured γγ-coin. 150,151,152Dy deduced levels, J, π, configurations, γ-branching, B(λ) ratios. Shell model.

doi: 10.1103/PhysRevLett.50.1447
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1983WA07      Nucl.Phys. A397, 161 (1983)

D.Ward, H.R.Andrews, B.Haas, P.Taras, N.Rud

Continuous Gamma Radiation Feeding High-Spin Isomers in 148,149,151,152Dy and 147Gd

NUCLEAR REACTIONS 120,122,124Sn(32S, xn), E=132-165 MeV; 124Sn(28Si, 5n), E=130-156 MeV; measured γγ-coin, γ(θ). 148,149,151,152Dy, 147Gd deduced continuum Eγ, γ-multipolarity, multiplicity spectra, average neutron kinetic energies. Pulsed beams, Ge(Li), NaI(Tl) array detectors, NaI(Tl) compton shielding crystal.

doi: 10.1016/0375-9474(83)90083-0
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1982AN10      Nucl.Phys. A383, 509 (1982)

H.R.Andrews, O.Hausser, D.Ward, P.Taras, R.Nicole, J.Keinonen, P.Skensved, B.Haas

Calibration of the Transient Magnetic Field for Rare-Earth Nuclei in Iron: Application to g-factors of high spin states in 152,154Sm

NUCLEAR REACTIONS 152,154Sm, Gd, 156Gd, Dy, 169Tm, 174Yb(63Cu, 63Cu'), E=154, 230 MeV; 152,154Sm, Gd, 156Gd, Dy, 169Tm, 174Yb(79Br, 79Br'), (81Br, 81Br'), E=200, 240 MeV; measured (63Cu)γ-, (79Br)γ-coin, γ(θ, H); deduced transient field calibration, Z, velocity dependence. 152,154Sm levels deduced g. Natural, enriched targets, Ge(Li) detectors, transient field IMPAC technique.

doi: 10.1016/0375-9474(82)90088-4
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1982BA46      Nucl.Phys. A389, 93 (1982)

O.Bakander, C.Baktash, J.Borggreen, J.B.Jensen, J.Kownacki, J.Pedersen, G.Sletten, D.Ward, H.R.Andrews, O.Hausser, P.Skensved, P.Taras

Co-Existence of Spherical and Oblate Configurations in 147Gd

NUCLEAR REACTIONS 135Ba(16O, 4n), E=77-84 MeV; 124Sn(28Si, 5n), E=128-140 MeV; measured γγ-coin, Iγ(θ), I(ce). 147Gd deduced levels, J, π, isomer T1/2, reduced transition probabilities. Pulsed beam, Ge(Li), Si(Li) detectors, NaI(Tl) array, mini-orange spectrometer.

doi: 10.1016/0375-9474(82)90293-7
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1982HA22      Nucl.Phys. A379, 287 (1982)

O.Hausser, H.E.Mahnke, T.K.Alexander, H.R.Andrews, J.F.Sharpey-Schafer, M.L.Swanson, D.Ward, P.Taras, J.Keinonen

Quadrupole Moments of Yrast Isomers in 144, 147, 148Gd

NUCLEAR REACTIONS 120,124Sn(28Si, xn), E=108-144 MeV; measured Iγ(θ, H, t) vs T. 144,147,148Gd levels deduced quadrupole moment, tentative J, deformation. Pulsed beam, Ge(Li) detectors, recoil implantation into Gd.

doi: 10.1016/0375-9474(82)90394-3
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1982TR01      Nucl.Phys. A378, 141 (1982)

W.Trautmann, J.F.Sharpey-Schafer, H.R.Andrews, B.Haas, O.Hausser, P.Taras, D.Ward

Measurement of the Linear Polarization of Continuum Gamma Rays from (32S, xn) Reactions to Prolate and Oblate Rare-Earth Nuclei

NUCLEAR REACTIONS 130Te, 124Sn(32S, xn), E=150 MeV; measured Eγ, Iγ, linear polarization, γ(θ). 156,158Er, 151,152Dy deduced γ-multipolarity, collective γ-ray continuum. Pulsed beam, NaI(Tl), Ge(Li) detectors, three-Ge(Li) polarimeter, NaI(Tl) array.

doi: 10.1016/0375-9474(82)90387-6
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1981HA17      Nucl.Phys. A362, 254 (1981)

B.Haas, D.Ward, H.R.Andrews, O.Hausser, A.J.Ferguson, J.F.Sharpey-Schafer, T.K.Alexander, W.Trautmann, D.Horn, P.Taras, P.Skensved, T.L.Khoo, R.K.Smither, I.Ahmad, C.N.Davids, W.Kutschera, S.Levenson, C.L.Dors

Yrast Isomers and very High Spin States in 148, 149, 151, 152Dy and 147Gd

NUCLEAR REACTIONS 120,122,124Sn(32S, xn), (34S, xn), E=129-165 MeV; 124Sn(28Si, 5n), E=110-149 MeV; 142Nd(12C, xn), E=56-61 MeV; measured γγ-coin, γγ(θ), γ(θ), γ(θ, t), linear polarization, recoil. 148,149,151,152Dy, 147Gd deduced levels, J, π, δ, T1/2, E2 transition strengths. Pulsed beam, Ge(Li) detectors, NaI(Tl) array, plunger, polarimeter.

doi: 10.1016/0375-9474(81)90680-1
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1981RU02      Phys.Lett. 100B, 17 (1981)

N.Rud, D.Ward, H.R.Andrews, P.Taras, J.Keinonen

Evidence for Enhanced transition Rates in the Feeding of High Spin States in 147Gd

NUCLEAR REACTIONS 124Sn(28Si, 5n), E=130, 145 MeV; measured γ-multiplicity, σ(Eγ), γ(θ). 147Gd deduced strectched E2 transition to quasiparticle yrast states, average B(E2), average entry spin J.

doi: 10.1016/0370-2693(81)90276-8
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1981RU05      Phys.Lett. 101B, 35 (1981)

N.Rud, D.Ward, H.R.Andrews, O.Hausser, P.Taras, J.Keinonen, M.Neiman, R.M.Diamond, F.S.Stephens

Average g-Factors for High Spin States in 156Dy

NUCLEAR REACTIONS 24Mg(136Xe, 4n), E=544, 570, 650 MeV; measured γ-multiplicities, γγ(θ, H) in Fe. 156Dy deduced average g in high-spin region.

doi: 10.1016/0370-2693(81)90483-4
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1981TA24      Phys.Lett. 107B, 35 (1981)

P.Taras, G.C.Ball, W.G.Davies, H.R.Andrews, B.Haas

Evidence for Alpha-Cluster Structure at 12.9 MeV CM in the 12C + 16O System

NUCLEAR REACTIONS 12C(16O, 12C), E(cm)=12.2-13.5 MeV; measured σ(θ) vs E, σ(E(12C)). 28Si resonance deduced J, π, Γ, α-cluster structure.

doi: 10.1016/0370-2693(81)91141-2
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1981WA16      Nucl.Phys. A365, 173 (1981)

D.Ward, H.R.Andrews, A.J.Ferguson, O.Hausser, N.Rud, P.Skensved, J.Keinonen, P.Taras

Average g-Factors for High-Spin States in 78Kr

NUCLEAR REACTIONS 16,18O(65Cu, 2np), (63Cu, 2np), E=190-210 MeV; measured γ(θ, B) in polarized Fe. 78Kr levels deduced g. Enriched targets, transient field perturbed angular correlation technique.

doi: 10.1016/0375-9474(81)90394-8
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1980AN27      Phys.Rev.Lett. 45, 1835 (1980)

H.R.Andrews, O.Hausser, D.Ward, P.Taras, N.Rud, B.Haas, R.M.Diamond, D.Fossan, H.Kluge, M.Nieman, C.Roulet, F.S.Stephens

g Factors of High-Spin States in 160Dy and 170,174Yb Measured by the Transient Magnetic Field Interaction

NUCLEAR REACTIONS 160Dy, 170,174Yb(86Kr, 86Kr'), E=350 MeV; measured (86Kr)γ-coin, multiple coulomb excitation, recoil in Fe, γ(θ, H). 160Dy, 170,174Yb deduced g for high-spin states.

doi: 10.1103/PhysRevLett.45.1835
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1980HA02      Phys.Rev.Lett. 44, 132 (1980)

O.Hausser, H.-E.Mahnke, J.F.Sharpey-Schafer, M.L.Swanson, P.Taras, D.Ward, H.R.Andrews, T.K.Alexander

Quadrupole Moment of a High-Spin Yrast Trap in 147Gd

NUCLEAR REACTIONS 124Sn(28Si, 5nγ), E=144 MeV; measured γ(θ, t), oriented nuclei, quadrupole interactions. 147Gd levels deduced quadrupole moments, quasiparticle configuration, β. Pulsed beam.

doi: 10.1103/PhysRevLett.44.132
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1980HA52      Hyperfine Interactions 8, 271 (1980)

O.Hausser, D.Ward, T.K.Alexander, H.R.Andrews, W.J.L.Buyers, H.-E.Mahnke, J.F.Sharpey-Schafer, P.Skensved, M.L.Swanson, P.Taras

The Electric Field Gradient for Gd in Gadolinium Metal

NUCLEAR REACTIONS 120Sn(28Si, 4n), E=130 MeV; measured γ(θ, H), recoil in Gd host. 144Gd deduced temperature dependence of electric field gradient in Gd above Curie point. 156,158,160Gd(α, α'), E=6 MeV; measured Coulomb excitation, Iγ; deduced electric field gradient for Gd in Gd.


1979HA15      Phys.Rev.Lett. 42, 1451 (1979)

O.Hausser, P.Taras, W.Trautmann, D.Ward, T.K.Alexander, H.R.Andrews, B.Haas, D.Horn

g Factors of High-Spin Yrast Traps in 146,147Gd

NUCLEAR REACTIONS 120,122,124Sn(28Si, xn), E=108-144 MeV; 144Sm(α, xn), E=30 MeV; measured γγ(θ, H, t) in Sn, Sm, Pb. 144,146,147,148Gd levels deduced T1/2, g, configuration. Paramagnetic correction, pulsed beam. Enriched targets.

doi: 10.1103/PhysRevLett.42.1451
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1979HA28      Phys.Lett. 84B, 178 (1979)

B.Haas, H.R.Andrews, O.Hausser, D.Horn, J.F.Sharpey-Schafer, P.Taras, W.Trautmann, D.Ward, T.L.Khoo, R.K.Smither

Single Particle Nature of the Yrast Line at High Angular Momentum in 152Dy

NUCLEAR REACTIONS 122Sn(34S, 4nγ), 124Sn(32S, 4nγ), E=150 MeV; measured γγ-coin, γγ(t), γ-linear polarization, DSA, RDM. 152Dy deduced levels, branching ratios, transition probabilities, T1/2, J, π.

doi: 10.1016/0370-2693(79)90278-8
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1979MA37      Phys.Lett. 88B, 48 (1979)

H.-E.Mahnke, T.K.Alexander, H.R.Andrews, O.Hausser, P.Taras, D.Ward, E.Dafni, G.D.Sprouse

Quadrupole Moments of the 12+ States in 206Pb and 200Pb

NUCLEAR REACTIONS 204,198Hg(α, 2n), E=33 MeV; measured γ(θ, H, t). 206,200Pb levels deduced quadrupole moments, T1/2, B(E2).

doi: 10.1016/0370-2693(79)90110-2
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1979ST13      Nucl.Phys. A327, 295 (1979)

J.Styczen, E.Bozek, T.Pawlat, Zb.Stachura, F.A.Beck, C.Gehringer, B.Haas, J.C.Merdinger, N.Schulz, P.Taras, M. Toulemonde, J.P.Vivien, A.Muller-Arnke

High-Spin States in 50Ti, 52Cr and 54Fe

NUCLEAR REACTIONS 48Ca, 50Ti, 52Cr(α, 2nγ), E=24-33 MeV; measured Eγ, σ(E, θγ), linear polarization, γγ-coin, σ(θγ, t). 50Ti, 52Cr, 54Fe deduced levels, J, π, δ, T1/2. Enriched targets.

doi: 10.1016/0375-9474(79)90261-6
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1979TA05      Phys.Rev. C19, 1557 (1979)

P.Taras, G.R.Rao

Spin of the 12.8 MeV c.m. Resonance in the 12C + 16O System

NUCLEAR REACTIONS 12C(16O, α), E(cm)=12.80-13.01 MeV; measured σ(θα). 28Si resonance deduced J, π.

doi: 10.1103/PhysRevC.19.1557
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1979TA18      Can.J.Phys. 57, 1775 (1979)

P.Taras, B.Haas, J.C.Merdinger, J.Styczen

Search for Isomers in Nuclei Near N = 50

NUCLEAR REACTIONS 58,60,61,62,64Ni, Co, Cu(16O, X), E=42 MeV; measured Eγ, Iγ, γ(t). 74Kr deduced no new isomer.

doi: 10.1139/p79-246
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1979TR08      Phys.Rev.Lett. 43, 991 (1979)

W.Trautmann, J.F.Sharpey-Schafer, H.R.Andrews, B.Haas, O.Hausser, P.Taras, D.Ward

Linear Polarization of the Continuum γ Rays Feeding High-Spin Yrast States in 151,152Dy and 156-158Er

NUCLEAR REACTIONS 124Sn(32S, 5n), (32S, 4n), 130Te(32S, 4n), (32S, 5n), (32S, 6n), E=150 MeV; measured continuum γ-linear polarization, σ(Eγ), Iγ(θ). 156,157,158Er levels deduced E2 cascade involving high-spin yrast states. 151,152Dy levels deduced collective rotational character of high-spin yrast states.

doi: 10.1103/PhysRevLett.43.991
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1979WA15      Nucl.Phys. A330, 225 (1979)

D.Ward, O.Hausser, H.R.Andrews, P.Taras, P.Skensved, N.Rud, C.Broude

Measurement of g-Factors in 170Yb, 172Yb and 174Yb by Transient Field Interaction at High Recoil Velocities

NUCLEAR REACTIONS 169Tm, 170,172,174Yb(40Ca, 40Ca'γ), E=168 MeV; measured (40Ca', γ)coin, γ(θ, H). 170,172,174Yb deduced g-factors. Enriched targets. Enhanced transient field. IMPAC technique.

doi: 10.1016/0375-9474(79)90547-5
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1978AZ01      Phys.Rev. C17, 443 (1978)

G.Azuelos, G.R.Rao, P.Taras

35Cl(p, n)35Ar Threshold Energy and its Relation to the Vanishing Cabibbo Angle

NUCLEAR REACTIONS 27Al, 35Cl(p, n), E=threshold; measured yields; deduced Q. 35Ar deduced Eβ, Q, Cabibbo angle.

doi: 10.1103/PhysRevC.17.443
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1978HA17      Phys.Rev.Lett. 40, 1313 (1978)

B.Haas, F.A.Beck, C.Gehringer, J.C.Merdinger, N.Schulz, P.Taras, M.Toulemonde, J.P.Vivien, J.Styczen, E.Bozek, Z.Stachura, T.Pawlat, A.Muller-Arnke

High-Spin Neutron Particle-Hole States in Even N = 28 Isotones

NUCLEAR REACTIONS 48Ca, 50Ti, 52Cr(α, 2nγ), E=27-33 MeV; measured σ(E, Eγ, θ), γγ-coin, γγ(θ), linear polarization, γ(t). 50Ti deduced levels, J, π, λ, δ, B(λ). 52Cr deduced configuration mixing.

doi: 10.1103/PhysRevLett.40.1313
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1978RA15      Phys.Rev. C18, 1085 (1978)

G.R.Rao, G.Azuelos, J.C.Kim, J.P.Martin, P.Taras

39K(p, n)39Ca Threshold Energy and the Gamow-Teller Interaction in 39Ca

NUCLEAR REACTIONS 39K(p, n), E=7.480-7.530 MeV; measured β+ yields; deduced Q. 39Ca deduced Gamow-Teller interaction.

RADIOACTIVITY 39Ca; measured Eβ; deduced Q.

doi: 10.1103/PhysRevC.18.1085
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1978TA11      Phys.Rev.Lett. 41, 840 (1978)

P.Taras, G.R.Rao, G.Azuelos

Fine Structure in the Fusion Cross Section for 16O + 12C

NUCLEAR REACTIONS 12C(16O, X), E=28.5-35 MeV; measured σ(E, Eγ).

doi: 10.1103/PhysRevLett.41.840
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1977TA03      Phys.Rev. C15, 834 (1977)

P.Taras, G.Rao, N.Schulz, J.P.Vivien, B.Haas, J.C.Merdinger, S.Landsberger

Resonance at E(c.m.) = 12.8 MeV in the 12C + 16O System

NUCLEAR REACTIONS 12C(16O, n), E(cm)=10.7-15.9 MeV; 12C(16O, p), (16O, d), (16O, α), (16O, 16O), E=12.43-13.93 MeV; measured σ. 28Si deduced resonance, J, π.

doi: 10.1103/PhysRevC.15.834
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1977TA10      Nucl.Phys. A289, 165 (1977)

P.Taras, D.Ward, H.R.Andrews, J.S.Geiger, R.L.Graham, W.McLatchie

Electromagnetic Properties of the Ground State Rotational Band in 169Tm

NUCLEAR REACTIONS 169Tm(32S, 32S'γ), E=130, 140 MeV; measured recoil distance, DSA, 32S'γ(θ), Eγ, Iγ. 169Tm levels deduced transitions, δ, T1/2, B(λ), γ-branching.

doi: 10.1016/0375-9474(77)90527-9
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1976HA07      Phys.Lett. 61B, 141 (1976)

B.Haas, J.Chevallier, A.Knipper, J.Styczen, P.Taras

Deformation Systematics for the Positive Parity States in the 1f7/2 Shell

NUCLEAR STRUCTURE 41,43,45,47Ca, 41,43,45,47Sc, 43,45,47,49,51V, 43,45,47,49Ti, 45,47,49,51,53Mn, 47,49,51,53,55Co, 47,49,51,53Fe, 47,49,51Cr, 49,51,53,55Ni; calculated relative static energy vs deformation.

doi: 10.1016/0370-2693(76)90609-2
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1976ME09      Nucl.Phys. A260, 307 (1976)

J.C.Merdinger, A.Chevallier, L.Courdier, B.Haas, J.Styczen, P.Taras

Mesures des Vies Moyennes des Niveaux de 41K Alimentes par les Reactions 39K(t, p) et 27Al(16O, 2p)

NUCLEAR REACTIONS 39K(t, pγ), E=3.0 MeV; 27Al(16O, 2pγ), (16O, npγ), E=34 MeV; measured Eγ, recoil distance, DSA. 41K, 41Ca deduced levels, T1/2, J. Natural targets. Si, Ge(Li) detectors.

doi: 10.1016/0375-9474(76)90032-4
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1976ST05      Nucl.Phys. A262, 317 (1976)

J.Styczen, J.Chevallier, B.Haas, N.Schulz, P.Taras, M.Toulemonde

Survey of Electromagnetic Properties of Positive Parity States in Odd 1f7/2 Shell Nuclei

NUCLEAR STRUCTURE 43,45,47Sc, 45Ti, 47,49V; calculated quadrupole moment, g ratios, band mixing; analyzed B(M1), B(E2).

doi: 10.1016/0375-9474(76)90624-2
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1975HA04      Nucl.Phys. A238, 253 (1975)

B.Haas, P.Taras, J.C.Merdinger, R.Vaillancourt

Yrast States in 48Cr and Reaction Mechanism of the 34S + 16O Reaction at E(lab) = 30-36 MeV

NUCLEAR REACTIONS 34S(16O, 2n), E=30-36 MeV; measured γγ-, nγ-coin, recoil distance, σ(E, Eγ), σ(Eγ, θ). 48Cr levels deduced, J, π, 3He, γ-mixing, deformation. Reaction mechanism, σ(E). Possible backbending effect. Enriched targets. Ge(Li), NE213 detectors.

doi: 10.1016/0375-9474(75)90352-8
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1975HA22      Nucl.Phys. A246, 141 (1975)

B.Haas, P.Taras, J.Styczen

Negative Parity States of the Cross-Conjugate Nuclei 47V-49Cr, 47Ti-49V in the Strong Coupling Model

NUCLEAR STRUCTURE 47,49V, 47,49Ti; calculated levels, μ, quadrupole moment, B(M1), B(E2), T1/2, γ-mixing, branching ratios.

doi: 10.1016/0375-9474(75)90568-0
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1975HA47      Phys.Rev. C12, 1865 (1975)

B.Haas, A.Chevallier, J.Chevallier, C.Gehringer, J.C.Merdinger, N.Schulz, J.Styczen, P.Taras, M.Toulemonde, J.P.Vivien

Magnetic Moment of the d3/2 Hole State in 45Ti

NUCLEAR REACTIONS 42Ca(α, n), E=9.0 MeV; measured γ(θ, H, t). 45Ti level deduced g. Enriched target. Ge(Li) detectors.

doi: 10.1103/PhysRevC.12.1865
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1975TA04      Nucl.Instrum.Methods 123, 73 (1975)

P.Taras, B.Haas

Spin Assignments Following Heavy-Ion Induced Reactions

NUCLEAR REACTIONS 34S(16O, pn), (16O, n2p), (16O, pα), (16O, 2p), (16O, nα), (16O, 2n), E=30-36 MeV; measured σ(E). 48V, 48Cr levels deduced J.

doi: 10.1016/0029-554X(75)90080-4
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1975VA15      Can.J.Phys. 53, 2534 (1975)

R.Vaillancourt, B.Haas, P.Taras

Proprietes des Niveaux de l'37Ar entre 2.7 et 3.8 MeV d'Energie d'Excitation

NUCLEAR REACTIONS 34S(α, nγ), E=10.5 MeV; measured linear polarization, σ(Eγ, θ), nγ-coin. 37Ar deduced levels, J, π, δ, γ-branching.

doi: 10.1139/p75-308
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1975WA14      Izv.Akad.Nauk SSSR, Ser.Fiz. 39, 37 (1975); Bull.Acad.Sci.USSR, Phys.Ser. 39, No.1, 30 (1975)

D.Ward, H.R.Andrews, G.J.Costa, J.S.Geiger, R.L.Graham, P.Taras

Values of the Lifetimes of States Having a High Nuclear Spin for Which Back Bending Is Observed. The Possibility of Measuring g-Factors by the Method of Varying the Flight of Recoil Nuclei in Vacuum

NUCLEAR REACTIONS 110Pd(24Mg, 4n), E=103 MeV; 115In(19F, 4n), E=86 MeV; measured Eγ, Iγ, σ(Eγ, θ), γγ-coin, recoil distance.


1974DE12      Nucl.Phys. A225, 1 (1974)

W.Dehnhardt, S.J.Mills, M.Muller-Veggian, U.Neumann, D.Pelte, G.Poggi, B.Povh, P.Taras

Yrast Cascades in Even-Mass Ce Isotopes

NUCLEAR REACTIONS 118,120,122,124Sn(16O, 4nγ), E=68-76 MeV; measured Eγ, Iγ(θ), γγ coin. 130,132,134,136Ce deduced levels, J, T1/2. Enriched targets.

doi: 10.1016/0375-9474(74)90361-3
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1974HA05      Can.J.Phys. 52, 49 (1974)

B.Haas, P.Taras

Band Mixing in the 2s-1d Shell: Application to 23Na

NUCLEAR STRUCTURE 23Na; calculated levels, T1/2, γ-mixing, μ, quadrupole moment.

doi: 10.1139/p74-007
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1974HA33      Phys.Rev.Lett. 33, 105 (1974)

B.Haas, P.Taras

Negative-Parity Band in 48V

NUCLEAR REACTIONS 34S(16O, pn), E=30-36 MeV; measured Eγ, Iγ, γ(θ), γγ-, nγ-coin. 48V deduced levels, J, π, γ-branching, mixing ratios, negative π band.

doi: 10.1103/PhysRevLett.33.105
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1974HA53      Phys.Lett. 52B, 146 (1974)

B.Haas, P.Taras, J.Styczen, J.Chevallier

Band Mixing in 49Cr and 47V: Importance of a Correct Treatment of Hole Excitations and the J2 Term

NUCLEAR STRUCTURE 47V, 49Cr; calculated levels.

doi: 10.1016/0370-2693(74)90073-2
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1974HA66      Nucl.Phys. A236, 405 (1974)

B.Haas, P.Taras, J.C.Merdinger, R.Vaillancourt

Mean Lifetimes of Levels in 48V

NUCLEAR REACTIONS 34S(16O, npγ), E=34 MeV; measured recoil distance, DSA; deduced reaction feeding time. 48V levels deduced T1/2, π, transition strengths. Enriched targets, Ge(Li) detector.

doi: 10.1016/0375-9474(74)90263-2
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1974TA15      Nucl.Phys. A232, 99 (1974)

P.Taras, B.Haas, R.Vaillancourt

Nuclear Spectroscopy in 48V via the 34S(16O, pn)48V Reaction

NUCLEAR REACTIONS 34S(16O, X), E=34 MeV; measured σ(Eγ, θ), γγ-coin, nγ-coin; 34S(16O, npγ), E=30-36 MeV; measured σ(E, Eγ). 48V deduced levels, J, π, γ-branching ratios, γ-mixing.

doi: 10.1016/0375-9474(74)90647-2
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1973VE05      Can.J.Phys. 51, 1039 (1973)

M.J.Verucchi, R.Vaillancourt, C.Cardinal, P.Taras

Mean Lifetime of the 1612 keV Level in 37Ar

NUCLEAR REACTIONS 34S(α, n), E=7.9 MeV; measured recoil-distance, Eγ. 37Ar level deduced T1/2.


1972TA10      Can.J.Phys. 50, 1182 (1972)

P.Taras, A.Turcotte, R.Vaillancourt

Study of Low-Lying Levels in 37Ar

NUCLEAR REACTIONS 35Cl(p, nγ), E=3.98, 4.17, 4.38, 4.81 MeV; 34S(α, nγ), E=8.00, 8.50, 8.60 MeV; measured σ(E;Eγ, θ(γ)), γ-linear polarization. 37Ar deduced levels, J, π, γ-mixing, γ-branching.

doi: 10.1139/p72-163
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1972TA25      Phys.Lett. 41B, 295 (1972)

P.Taras, W.Dehnhardt, S.J.Mills, M.Veggian, J.C.Merdinger, U.Neumann, B.Povh

High-Spin Yrast States in 132C

NUCLEAR REACTIONS 120Sn(16O, 4nγ), E=68-76 MeV; measured σ(E;Eγ, θ(γ), θ(γγ)), γγ-coin. 132Ce deduced high-J yrast states, J.

doi: 10.1016/0370-2693(72)90582-5
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1972TU06      Nucl.Instrum.Methods 105, 445 (1972)

A.Turcotte, P.Taras

Analysis of Gamma-Ray Linear Polarization Spectra Obtained with a NaI Compton Polarimeter

NUCLEAR REACTIONS 34S(α, nγ);E=8.6 MeV; measured linear polarization. 37Ar deduced γ-ray mixing ratios.

doi: 10.1016/0029-554X(72)90336-9
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1971TA02      Can.J.Phys. 49, 328 (1971)

P.Taras

Gamma-Ray Linear Polarization and Angular Distribution Formulas in Terms of Phase-Defined Reduced Matrix Elements

NUCLEAR REACTIONS 35Cl(p, p'γ), E=3.115 MeV; measured nothing; analyzed Iγ(θ), γ-linear polarization data. 35Cl level deduced J, γ-mixing.

doi: 10.1139/p71-039
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1971TA08      Can.J.Phys. 49, 1215 (1971)

P.Taras, A.Turcotte, R.Vaillancourt, J.Matas

Properties of the 1.410 and 1.612 MeV Levels in 37Ar and the 1.727 MeV Level in 37Cl

NUCLEAR REACTIONS 37Cl(p, p'γ), (p, nγ), E=3.98, 4.17, 4.38, 4.81 MeV; measured σ(Eγ, θ(γ)), γ-linear polarization. 37Cl, 37Ar levels deduced J, π, γ-mixing.

doi: 10.1139/p71-146
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1970TA02      Can.J.Phys. 48, 603 (1970)

P.Taras, J.Matas

Properties of the 2.645, 2.693, 3.001, and 3.162 MeV Levels in 35Cl

NUCLEAR REACTIONS 35Cl(p, p'γ), E=4.2-5.2 MeV; measured σ(E;Eγ, θ(γ)), γ-linear polarization. 35Cl deduced levels, branching ratios, J, π, γ-mixing, transition strengths.

doi: 10.1139/p70-078
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1970TA09      Nucl.Instrum.Methods 77, 10 (1970)

P.Taras, J.Matas

Analysis of Linear Polarization Measurements of Unresolved Gamma Rays

NUCLEAR REACTIONS 35Cl(p, p'γ), E=5.11 MeV; measured γ-linear polarization. 35Cl transitions deduced γ-mixing.

doi: 10.1016/0029-554X(70)90578-1
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1969TA13      Can.J.Phys. 47, 1605 (1969)

P.Taras, J.Matas

Properties of the 1.763 MeV Level in 35Cl

NUCLEAR REACTIONS 35Cl(p, p'γ), E = 3.05-3.37 MeV; measured σ(E;Eγ, θ(γ)), γ linear polarization. 35Cl level deduced J, π, γ-mixing.

doi: 10.1139/p69-204
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1968TA14      Nucl.Instr.Methods 62, 117 (1968)

P.Taras

Interpretation of the Isotropic Gamma-Ray Angular Distribution for a Final State of Spin 3/2

doi: 10.1016/0029-554X(68)90627-7
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1967TA08      Phys.Rev. 164, 1386 (1967)

P.Taras, L.W.Oleksiuk, R.E.Azuma, J.D.Prentice

Properties of Some Levels of Cl35

NUCLEAR STRUCTURE 35Cl; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.164.1386
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1967TA13      Nucl.Instr.Methods 54, 153 (1967)

P.Taras

Theoretical Angular Distribution Curves for Reactions with Entrance Channel Spin 1/2

NUCLEAR STRUCTURE 35Cl levels deduced γ-mixing, J from Iγ(θ) analysis.

doi: 10.1016/S0029-554X(67)80026-0
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1966AZ01      Phys.Rev.Letters 17, 659 (1966)

R.E.Azuma, L.W.Oleksiuk, J.D.Prentice, P.Taras

Properties of the 3.16-MeV Level of Cl35

NUCLEAR STRUCTURE 35Cl; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.17.659
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1966TA03      Can.J.Phys. 44, 1563 (1966)

P.Taras

35Cl and the Unified Model

NUCLEAR STRUCTURE 35Cl; measured not abstracted; deduced nuclear properties.

doi: 10.1139/p66-129
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Note: The following list of authors and aliases matches the search parameter P.Taras: , P.J.TARAS