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NSR database version of April 11, 2024.

Search: Author = T.H.Kruse

Found 38 matches.

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1981BA01      Nucl.Phys. A351, 63 (1981)

F.T.Baker, A.Scott, R.C.Styles, T.H.Kruse, K.Jones, R.Suchannek

182,184,186W(α, α') Reactions at Eα = 24 MeV

NUCLEAR REACTIONS 182,184,186W(α, α'), E=24 MeV; measured σ(Eα', θ); deduced optical model parameters. 182,184,186W deduced β2, β4 charge, density quadrupole, hexadecapole moments. 184W deduced β3. Enriched targets. Rotational-vibrational model.

doi: 10.1016/0375-9474(81)90545-5
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0890.


1981BA49      Nucl.Phys. A371, 68 (1981)

F.T.Baker, M.A.Grimm, Jr., A.Scott, R.C.Styles, T.H.Kruse, K.Jones, R.Suchannek

192Os(α, α') Reaction at Eα = 24 MeV and the IBA Model

NUCLEAR REACTIONS 192Os(α, α), (α, α'), E=24 MeV; measured σ(θ), σ(Eα', θ). 192Os deduced B(E4), deformation parameter β4. Enriched target. Interacting boson model, coupled-channels analysis.

doi: 10.1016/0375-9474(81)90745-4
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0839.


1978BA20      Phys.Rev. C17, 1559 (1978)

F.T.Baker, A.Scott, R.M.Ronningen, T.H.Kruse, R.Suchannek, W.Savin

192Pt(α, α') Reaction at E = 24 MeV

NUCLEAR REACTIONS 192Pt(α, α'), E=24 MeV; measured σ(Eα', θ). 192Pt levels deduced β, relative signs of matrix elements. Coupled channels analysis. Enriched target.

doi: 10.1103/PhysRevC.17.1559
Citations: PlumX Metrics


1978RO02      Phys.Rev.Lett. 40, 364 (1978)

R.M.Ronningen, F.T.Baker, A.Scott, T.H.Kruse, R.Suchannek, W.Savin, J.H.Hamilton

Evidence for a Nonrotational Interpretation of [0+ m(E4) 4+] in 180Hf

NUCLEAR REACTIONS 180Hf(α, α'), E=21, 24 MeV; measured σ(Eα', θ). 180Hf levels deduced β2, β4.

doi: 10.1103/PhysRevLett.40.364
Citations: PlumX Metrics


1977BA58      Phys.Lett. 70B, 167 (1977)

F.T.Baker, A.Scott, R.M.Ronningen, T.H.Kruse, R.Suchannek, W.Savin, J.H.Hamilton

Sensitivity of (α, α') Cross Sections to Excited-State Quadrupole Moments

NUCLEAR REACTIONS 180Hf(α, α'), E=21, 24 MeV; measured σ(Eα', θ). 180Hf level deduced β.

doi: 10.1016/0370-2693(77)90512-3
Citations: PlumX Metrics


1976BA06      Nucl.Phys. A258, 43 (1976)

F.T.Baker, T.H.Kruse, W.Hartwig, I.Y.Lee, J.X.Saladin

Nuclear Shapes of the Transitional Nuclei 186,188,190,192Os

NUCLEAR REACTIONS 186,188,190,192Os(α, α'), E=13-24 MeV, θlab=130°; measured σ(E, Eα'). 186,188,190,192Os deduced β2 charge, mass deformations, 186,188,192Os deduced β4 charge, mass deformations. 192Os(α, α'), E=24 MeV; measured σ(Eα', θ). 192Os deduced optical model parameters. Enriched targets.

doi: 10.1016/0375-9474(76)90526-1
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0894.


1976BA23      Phys.Rev.Lett. 37, 193 (1976)

F.T.Baker, A.Scott, T.H.Kruse, W.Hartwig, E.Ventura, W.Savin

Experimental Determination of the Signs of E2 Interference Terms for 192Os and 194Pt

NUCLEAR REACTIONS 192Os, 194Pt(α, α'), E=12-24 MeV; analyzed data. 192Os, 194Pt deduced sign of interference term.

doi: 10.1103/PhysRevLett.37.193
Citations: PlumX Metrics


1976BA35      Nucl.Phys. A266, 337 (1976)

F.T.Baker, A.Scott, T.H.Kruse, W.Hartwig, E.Ventura, W.Savin

Nuclear Shapes of the Transitional Nuclei 194,196,198Pt

NUCLEAR REACTIONS 194,196,198Pt(α, α'), E=14-24 MeV, θlab=127.5°; measured σ(E, e'). 194,196,198Pt deduced β2, β4 charge, mass deformations. 194Pt deduced sign of interference term.

doi: 10.1016/0375-9474(76)90362-6
Citations: PlumX Metrics


1975BA03      Phys.Rev. C11, 262 (1975)

F.T.Baker, W.Hartwig, T.H.Kruse, E.Ventura

Coulomb-Nuclear Interference for the (d, d') Reaction on Isotopes of Nd

NUCLEAR REACTIONS 142,144,146,148,150Nd(d, d'), E=5-16 MeV; measured σ(E, Ed'); deduced deformation parameters β2. Enriched targets.

doi: 10.1103/PhysRevC.11.262
Citations: PlumX Metrics


1975BA09      Phys.Rev. C11, 1051 (1975)

F.T.Baker, T.H.Kruse, W.Hartwig, M.E.Williams, W.Savin

Coulomb-Nuclear Interference for the 58Ni(14N, 14N') Reaction

NUCLEAR REACTIONS 58Ni(14N, 14N), E=30-48 MeV; measured σ(E), first 2+ state at θ(lab)=59°. 58Ni(14N, 14N), E=41 MeV; measured σ(θ). Enriched target.

doi: 10.1103/PhysRevC.11.1051
Citations: PlumX Metrics


1974BA78      Nucl.Phys. A235, 428 (1974)

F.T.Baker, T.H.Kruse, M.E.Williams, W.Savin

Coulomb-Nuclear Interference for Inelastic Deuteron Scattering

NUCLEAR REACTIONS 54,56Fe, 60Ni, 114Cd, 152Sm, 192Os(d, d'), E=3-16 MeV; measured σ(E, Ed'). 54,56Fe, 60Ni, 114Cd, 152Sm, 192Os levels deduced deformation lengths βL R. Enriched targets.

doi: 10.1016/0375-9474(74)90203-6
Citations: PlumX Metrics


1973BA28      Part.Nucl. 5, 29 (1973)

F.T.Baker, T.H.Kruse, J.L.Matthews, M.E.Williams

90Zr(d, d') Reaction at E = 15 MeV

NUCLEAR REACTIONS 90Zr(d, d'), E=15 MeV; measured σ(θ). Deduced β(L), L.


1973BA39      Phys.Rev.Lett. 31, 721 (1973)

F.T.Baker, T.H.Kruse, M.E.Williams, W.Savin

Observation of Nuclear Structure Dependence of the Phase of the (d, d') Form Factor

NUCLEAR REACTIONS 54,56Fe, 60Ni, 114Cd, 138Ba, 144,150,152Sm, 192Os(d, d'); measured σ(E). 138Ba, 144,150Sm deduced levels, J, π, deformation parameters.

doi: 10.1103/PhysRevLett.31.721
Citations: PlumX Metrics


1973WI16      Nucl.Phys. A213, 317 (1973)

M.E.Williams, T.H.Kruse, P.Goode, F.T.Baker, J.L.Matthews, W.Savin

Neutron Correlations in the 41K Ground State and T = 1 2p-2h States in 40K

NUCLEAR REACTIONS 41K(p, d), (d, t), E=15 MeV; measured σ(θ). 40K levels deduced L, S.

doi: 10.1016/0375-9474(73)90153-X
Citations: PlumX Metrics


1972BA61      Phys.Lett. 40B, 355 (1972)

F.T.Baker, T.H.Kruse, M.E.Williams, J.L.Matthews, W.Savin

The Phase and Shape of the Form Factor for Inelastic 3He Scattering

NUCLEAR REACTIONS 114Cd(3He, 3He), (3He, 3He'), E=10-17 MeV; measured σ(E;θ); deduced nuclear/Coulomb excitation interference, form factor.

doi: 10.1016/0370-2693(72)90818-0
Citations: PlumX Metrics


1972FE06      Nucl.Phys. A187, 123 (1972)

J.A.Fenton, T.H.Kruse, N.Williams, M.E.Williams, R.N.Boyd, W.Savin

Two-Hole Strengths in 38K from the 39K(3He, α)38K Reaction

NUCLEAR REACTIONS 39K(3He, α)38K, E=21.09 MeV; measured σ(θ(α)), Q. 38K deduced levels, J, π, L(n), T, S. Natural target.

doi: 10.1016/0375-9474(72)90078-4
Citations: PlumX Metrics


1969BA50      Phys.Letters 30B, 621 (1969)

G.Bassani, T.H.Kruse, N.Saunier, G.Souchere

The 13C(6Li, t)16O Reaction at 20 MeV

NUCLEAR REACTIONS 13C(6Li, t), E = 20 MeV; measured σ(Et, θ). 16O deduced levels.

doi: 10.1016/0370-2693(69)90075-6
Citations: PlumX Metrics


1968MA34      Phys.Rev. 174, 1429 (1968)

W.Makofske, W.Savin, H.Ogata, T.H.Kruse

Elastic and Inelastic Proton Scattering from Even Isotopes of Cd, Sn, and Te

NUCLEAR REACTIONS 110,112,114,116Cd, 112,116,118,120,122,124Sn, 126,128,130Te(p, p'), E=16 MeV; measured σ(θ).

doi: 10.1103/PhysRev.174.1429
Citations: PlumX Metrics


1967MA23      Phys.Letters 25B, 322 (1967)

W.Makofske, M.Slagowitz, W.Savin, H.Ogata, T.H.Kruse, T.Tamura

Scattering of 16-MeV Protons from Even Tin Isotopes

NUCLEAR REACTIONS 112,114,116,118,120,122,124Sn(p, p'), E=16 MeV; measured σ(θ). Coupled-channel analysis.

doi: 10.1016/0370-2693(67)90082-2
Citations: PlumX Metrics


1963NI05      Phys.Rev. 132, 2212 (1963)

N.Nikolic, L.J.Lidofsky, T.H.Kruse

Scattering of Protons from C12 in the Energy Range of 5-6 MeV

NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.132.2212
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2362.


1962NE02      Phys.Rev. 125, 639 (1962)

M.Nessin, T.H.Kruse, K.E.Eklund

Nuclear Electric Monopole Transitions in O16, Ca40, Ge72, and Zr90

NUCLEAR STRUCTURE 16O, 90Zr, 91Nb, 73As, 72Ge, 40Ca; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.125.639
Citations: PlumX Metrics


1961BE19      Phys.Rev. 123, 262 (1961)

N.Benczer-Koller, M.Nessin, T.H.Kruse

Nuclear Electric Monopole Transition in Ca42

NUCLEAR STRUCTURE 42Ca; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.123.262
Citations: PlumX Metrics


1961NI01      Bull.Am.Phys.Soc. 6, No.1, 25, I9 (1961)

N.M.Nikolic, L.J.Lidofsky, T.H.Kruse

Excited States of N13 Around 7 MeV

NUCLEAR STRUCTURE 13N; measured not abstracted; deduced nuclear properties.


1961NI08      Cu(Pnpl)-211, 20 (1961)

N.Nikolic, J.Silverstein, T.H.Kruse

Proton Scattering from C12

NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.


1960BE07      Bull.Am.Phys.Soc. 5, No.4, 248, 16 (1960)

N.Benczer-Koller, M.Nessin, T.H.Kruse

Nuclear Electric Monopole Transition in Ca42

NUCLEAR STRUCTURE 42Ca; measured not abstracted; deduced nuclear properties.


1960KR02      Phys.Rev. 119, 289 (1960)

T.H.Kruse, R.D.Bent, L.J.Lidofsky

Gamma Radiations of Na23 and Ne20

NUCLEAR STRUCTURE 20Ne, 23Na; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.119.2890
Citations: PlumX Metrics


1960NE01      Bull.Am.Phys.Soc. 5, No.1, 66, UA2 (1960)

M.Nessin, T.H.Kruse

Nuclear Electric Monopole Transition in Ge72 and Zr90

NUCLEAR STRUCTURE 72Ge, 90Zr, 16O, 40Ca; measured not abstracted; deduced nuclear properties.


1960NE18      CU(PNPL)-205, p.20 (1960)

M.Nessin, T.H.Kruse

Nuclear Electric Monopole Transitions

NUCLEAR STRUCTURE 207Bi, 72Ge, 90Zr, 40Ca; measured not abstracted; deduced nuclear properties.


1959KR66      Thesis, Columbia University (1959); CU-181 (1959)

T.H.Kruse

Gamma Radiations of Na23 and Ne20


1959KR67      CU-174, p.25 (1959)

T.H.Kruse, R.D.Bent, L.J.Lidofsky

Gamma-Rays from Na23 + p: Na23 States


1959NE21      Bull.Am.Phys.Soc. 4, No.4, 278, U6 (1959)

M.Nessin, K.E.Eklund, T.H.Kruse

Electric Monople Internal Conversion in Ca40 and O16


1959NE25      Bull.Am.Phys.Soc. 4, No.1, 18, EA11 (1959)

M.Nessin, K.E.Eklund, T.H.Kruse

Search for Double Gamma Emission from the First Excited State of Ca40


1959NE28      CU(PNPL)-199, p.23 (1959)

M.Nessin, T.H.Kruse

O+ → O+ Nuclear Electric Monopole Transitions


1958BE15      Phys.Rev. 109, 1240 (1958)

R.D.Bent, T.H.Kruse

Compound States Formed in the Reaction Ca40(p, p'e+e-)

doi: 10.1103/PhysRev.109.1240
Citations: PlumX Metrics


1958KR67      Bull.Am.Phys.Soc. 3, No.3, 200, P11 (1958)

T.H.Kruse, R.D.Bent, L.J.Lidofsky

Gamma Rays from Na23 + p


1958KR70      Phys.Rev. 112, 931 (1958)

T.H.Kruse, R.D.Bent

Search for Electric Monopole Pairs from the 7.6-MeV State of C12

doi: 10.1103/PhysRev.112.931
Citations: PlumX Metrics


1957BE48      Bull.Am.Phys.Soc. 2, No.4, 179, D10 (1957)

R.D.Bent, T.H.Kruse, L.J.Lidofsky

Excitation Function for the Reaction Ca40(p, p'π) and Levels in Sc41


1957BE61      Phys.Rev. 108, 802 (1957)

R.D.Bent, T.H.Kruse

Gamma-Emitting States in O16 Below 12 MeV

doi: 10.1103/PhysRev.108.802
Citations: PlumX Metrics


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