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Search: Author = S.D.Bloom

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2001GO25      Nucl.Instrum.Methods Phys.Res. A462, 545 (2001)

C.D.Goodman, M.Bhattacharya, M.B.Aufderheide, S.D.Bloom, P.Zupranski

Data Analysis Techniques for Extracting Gamow-Teller Strengths from 0° (p, n) Data

NUCLEAR REACTIONS 7Li, 13C, 23Na(p, n), E=120, 160 MeV; analyzed neutron spectra; deduced Gamow-Teller matrix elements.

doi: 10.1016/S0168-9002(00)01317-6
Citations: PlumX Metrics


1996AU05      Phys.Rev. C53, 3139 (1996)

M.B.Aufderheide, S.D.Bloom, G.J.Mathews, D.A.Resler

Importance of (n, p) Reactions for Stellar Beta Decay Rates

NUCLEAR STRUCTURE 54,56Mn, 58Co, 59Fe; calculated Gamow-Teller resonances; deduced newly calibrated stellar β-decay rates related features. Data from (n, p) reactions considered.

doi: 10.1103/PhysRevC.53.3139
Citations: PlumX Metrics


1996RE06      Phys.Rev. C53, 2505 (1996)

M.T.Ressell, G.J.Mathews, M.B.Aufderheide, S.D.Bloom, D.A.Resler

Strange Neutral Currents in Nuclei

NUCLEAR STRUCTURE 50,52,54,56,58,60,62,64,66Fe, 56Ni, 28Si, 24Mg, 20Ne, 14N, 12C; calculated total neutral current Gamow-Teller transition strength change, strength function. Shell model, finite contribution from polarized strange quark sea.

doi: 10.1103/PhysRevC.53.2505
Citations: PlumX Metrics


1994AU01      Phys.Rev. C49, 678 (1994)

M.B.Aufderheide, S.D.Bloom, D.A.Resler, C.D.Goodman

Comparison of Gamow-Teller Strength in 37Ar and 37K and 37Cl Neutrino Cross Sections

NUCLEAR STRUCTURE 37Ar; analyzed Gamow-Teller transition strength; deduced 37Cl(ν, X) reaction σ for solar, supernova, μ+-decay neutrinos. 37K level deduced β--delayed proton emission suppression features. Shell model.

doi: 10.1103/PhysRevC.49.678
Citations: PlumX Metrics


1993AU02      Phys.Rev. C47, 2961 (1993)

M.B.Aufderheide, S.D.Bloom, D.A.Resler, G.J.Mathews

Implications of the Recent 59Co(n, p)59Fe Experiment for Stellar Electron Capture Rates

NUCLEAR REACTIONS 59Co(p, n), E not given; calculated Gamow-Teller transition strength; deduced stellar electron capture rate (in 59Co) implications. Shell model.

NUCLEAR STRUCTURE 59Co, 59Fe; calculated levels. 60Co; calculated Gamow-Teller transition strengths. 59,60Co; calculated stellar electron capture rate vs temperature. Shell model.

doi: 10.1103/PhysRevC.47.2961
Citations: PlumX Metrics


1993AU06      Phys.Rev. C48, 1677 (1993)

M.B.Aufderheide, S.D.Bloom, D.A.Resler, G.J.Mathews

Shell-Model Calculations of Gamow-Teller Strength in 51V, 54Fe, and 59Co

NUCLEAR REACTIONS 51V, 54Fe, 59Co(p, n), (n, p), E not given; calculated normalized Gamow-Teller transition strength; deduced quenching reaction dependence. Shell model.

doi: 10.1103/PhysRevC.48.1677
Citations: PlumX Metrics


1993RE14      Phys.Rev. D48, 5519 (1993)

M.T.Ressell, M.B.Aufderheide, S.D.Bloom, K.Griest, G.J.Mathews, D.A.Resler

Nuclear Shell Model Calculations of Neutralino-Nucleus Cross Sections for 29Si and 73Ge

NUCLEAR REACTIONS 29Si, 73Ge(X, X), E not given; calculated neutralino scattering matrix elements; deduced non-nuclear uncertainities. Shell model target wave functions.

NUCLEAR STRUCTURE 29Si, 73Ge; calculated levels, spectroscopic factors, g factors. Shell model target wave functions.

doi: 10.1103/PhysRevD.48.5519
Citations: PlumX Metrics


1992AU05      Phys.Rev. C46, 2251 (1992)

M.B.Aufderheide, S.D.Bloom, D.A.Resler, C.D.Goodman

Gamow-Teller Strength in A = 37 Nuclei

NUCLEAR STRUCTURE A=37; analyzed Gamow-Teller transition strength from 37Ca(β+) decay, 37Cl(p, n) reaction data; deduced branching ratios sum possible values range, relevance to solar, supernova ν σ of 37Cl.

doi: 10.1103/PhysRevC.46.2251
Citations: PlumX Metrics


1992CA05      Phys.Rev. C45, 1145 (1992)

J.A.Carr, S.D.Bloom, F.Petrovich, R.J.Philpott

Fragmentation of Stretched Spin Strength in N = Z sd-Shell Nuclei

NUCLEAR STRUCTURE 20Ne, 24Mg, 28Si, 32S, 36Ar; calculated levels transition strengths, stretched states spin strength fragmentation. Effective interactions.

doi: 10.1103/PhysRevC.45.1145
Citations: PlumX Metrics


1992GO13      Phys.Rev.Lett. 69, 2445 (1992)

C.D.Goodman, M.B.Aufderheide, S.D.Bloom, D.A.Resler

Comment on ' Is the Weak Axial-Vector Current Renormalized in Nuclei ( Question ) '

NUCLEAR STRUCTURE 37K, 37Ar; analyzed Gamow-Teller transition strength data; deduced β-decay, (p, n) reaction probe consistency evidence.

doi: 10.1103/PhysRevLett.69.2445
Citations: PlumX Metrics


1990GO12      Phys.Rev. C42, 1150 (1990)

C.D.Goodman, J.Rapaport, S.D.Bloom

Comment on ' Testing ' the Gamow-Teller Sum Rule

doi: 10.1103/PhysRevC.42.1150
Citations: PlumX Metrics


1989CA07      Phys.Rev.Lett. 62, 2249 (1989); Erratum Phys.Rev.Lett. 63, 918 (1989)

J.A.Carr, S.D.Bloom, F.Petrovich, R.J.Philpott

Fragmentation of Stretched Spin Strength in 28Si

NUCLEAR STRUCTURE 28Si; calculated stretched states fragmentation, spectroscopic factors, M6 transition strength function. Large basis.

doi: 10.1103/PhysRevLett.62.2249
Citations: PlumX Metrics


1987BL24      Can.J.Phys. 65, 684 (1987)

S.D.Bloom, G.J.Mathews, J.A.Becker

Gamow-Teller Strength Function for 90Zr(n, p)90Y

NUCLEAR REACTIONS 90Zr(n, p), E not given; calculated Gamow-Teller strength function. Exciton model.

NUCLEAR STRUCTURE 90Y; calculated energy levels. Exciton model.

doi: 10.1139/p87-098
Citations: PlumX Metrics


1986TA01      Phys.Rev. C33, 296 (1986)

K.Takahashi, G.J.Mathews, S.D.Bloom

Shell-Model Calculation of 99Tc Beta Decay in Astrophysical Environments

NUCLEAR STRUCTURE 99Tc; calculated β-decay Gamow-Teller matrix elements, T1/2 at stellar temperature, s-process survival. 97Mo; calculated levels, β-decay log ft. 97Nb, 99Ru; calculated levels. Shell model.

doi: 10.1103/PhysRevC.33.296
Citations: PlumX Metrics


1986WA25      J.Phys.(London) G12, 1017 (1986)

E.K.Warburton, J.W.Olness, C.J.Lister, J.A.Becker, S.D.Bloom

Yrast Decays in 87,89Zr, 87,88,89,90Y and 86Sr from 74,76Ge(18O, xn, yp, zαγ) Reactions

NUCLEAR REACTIONS 74,76Ge(18O, nα), (18O, 2nα), (18O, 3nα), (18O, 4nα), (18O, 2np), (18O, 3np), (18O, 4np), (18O, 5np), (18O, 2n), (18O, 3n), (18O, 4n), (18O, 5n), (18O, 6n), E=40-80 MeV; measured residual production σ, γγ-coin, γ(θ), σ(Eγ, E), γ yields, linear polarizations, DSA, recoil distance. 87,89Zr, 87,88,89,90Y, 86Sr deduced levels, J, π, T1/2, γ-branching, B(λ), γ-multipolarity. Ge detector. Shell model calculations.

doi: 10.1088/0305-4616/12/10/012
Citations: PlumX Metrics


1985BL11      Nucl.Phys. A440, 511 (1985)

S.D.Bloom, G.M.Fuller

Gamow-Teller Electron Capture Strength Distributions in Stars: Unblocked Iron and Nickel Isotopes

RADIOACTIVITY 56,54,60,64Fe, 56Ni(EC); calculated Gamow-Teller strength distributions.

doi: 10.1016/0375-9474(85)90243-X
Citations: PlumX Metrics


1985LI11      Phys.Rev. C32, 311 (1985)

C.J.Lister, J.W.Olness, E.K.Warburton, J.A.Becker, S.D.Bloom

Identification of the Yrast Decay Scheme of 86Y

NUCLEAR REACTIONS 62Ni(27Al, xnypzα), E=85 MeV; measured (particle)γ-coin, Eγ, Iγ. 86Y deduced levels, J, π.

doi: 10.1103/PhysRevC.32.311
Citations: PlumX Metrics


1985MA40      Phys.Rev. C32, 796 (1985)

G.J.Mathews, S.D.Bloom, G.M.Fuller, J.N.Bahcall

Shell Model Calculation for the 71Ga(ν, e-)71Ge Solar Neutrino Detector

NUCLEAR REACTIONS 71Ga(ν, e-), E not given; calculated Gamow-Teller transition strengths to residual nuclear levels following neutrino capture; deduced solar neutrino capture rate. 72Ge(p, d), 70Zn(3He, d), E not given; calculated spectroscopic factors.

NUCLEAR STRUCTURE 71Ga; calculated levels. 71Ge; calculated levels, Gamow-Teller transition strengths.

doi: 10.1103/PhysRevC.32.796
Citations: PlumX Metrics


1985ST19      Phys.Rev. C32, 1397 (1985)

B.Strohmaier, S.M.Grimes, S.D.Bloom

Comparison of Lanczos Methods and Moment Methods in Calculating Nuclear Level Densities

NUCLEAR STRUCTURE 20Ne; calculated level densities. Shell model, Lanczos moment methods.

doi: 10.1103/PhysRevC.32.1397
Citations: PlumX Metrics


1984BE33      ATOMKI Kozlem. 26, 86 (1984)

J.A.Becker, S.D.Bloom

Shell Model Calculations of 90Zr and 88Zr

NUCLEAR STRUCTURE 88,90Zr; calculated levels, B(E2). Shell model, effective nucleon charge.


1983GR12      Phys.Rev. C27, 2893 (1983)

S.M.Grimes, S.D.Bloom, H.K.Vonach, R.F.Hausman, Jr.

Spectral Distribution Calculations of the Level Density and Spin-Cutoff Parameters of 28Si

NUCLEAR STRUCTURE 28Si; calculated level density, spin cutoff parameter. Spectral distribution method.

doi: 10.1103/PhysRevC.27.2893
Citations: PlumX Metrics


1983MA45      Phys.Rev. C28, 1367 (1983)

G.J.Mathews, S.D.Bloom, R.F.Hausman, Jr.

Gamow-Teller Strength Function for 90Zr: Effects of spin and isospin exchange forces, and ground-state correlations

RADIOACTIVITY 90Zr(β-); calculated Gamow-Teller strength function; deduced spin, isospin exchange force, ground state correlation effects. Shell model.

doi: 10.1103/PhysRevC.28.1367
Citations: PlumX Metrics


1981BL17      Phys.Lett. 107B, 336 (1981)

S.D.Bloom, C.D.Goodman, S.M.Grimes, R.F.Hausman, Jr.

Gamow-Teller Strength Function for 26Mg → 26Al

NUCLEAR REACTIONS 26Mg(p, n), E=120 MeV; calculated Gamow-Teller strength function distribution. Shell model.

doi: 10.1016/0370-2693(81)90336-1
Citations: PlumX Metrics


1981GO18      Phys.Lett. 107B, 406 (1981)

C.D.Goodman, C.C.Foster, D.E.Bainum, S.D.Bloom, C.Gaarde, J.Larsen, C.A.Goulding, D.J.Horen, T.Masterson, S.Grimes, J.Rapaport, T.N.Taddeucci, E.Sugarbaker

Missing Gamow-Teller Strength in Mass 42

NUCLEAR REACTIONS 42Ca(p, n), E=160 MeV; measured σ(θ, En). 42Sc deduced Gamow-Teller transition strength distribution. Shell model.

doi: 10.1016/0370-2693(81)91217-X
Citations: PlumX Metrics


1981GR06      Phys.Rev. C23, 1259 (1981)

S.M.Grimes, S.D.Bloom

Shell Model Test of the Porter-Thomas Distribution

NUCLEAR STRUCTURE 18,19F, 20,21Ne, 26Mg; calculated levels, eigenvectors; deduced amplitude distribution dependence on Hamiltonian structure. Shell model, sd-basis.

doi: 10.1103/PhysRevC.23.1259
Citations: PlumX Metrics


1980BL06      Phys.Lett. 93B, 227 (1980)

S.D.Bloom, S.M.Grimes, R.F.Hausman, Jr.

A Monte Carlo Method for Calculating Strength Functions in Many-Fermion Systems

NUCLEAR STRUCTURE 21Ne, 28Si; calculated Hamiltonian moments, strength functions. Monte-Carlo method, random vectors, many-fermion system.

doi: 10.1016/0370-2693(80)90500-6
Citations: PlumX Metrics


1979GR07      Phys.Rev. C19, 2378 (1979)

S.M.Grimes, S.D.Bloom, R.F.Hausman, Jr., B.J.Dalton

Method for Calculating Operator Traces

NUCLEAR STRUCTURE 21Ne; calculated level density, operator moments. Spectral distribution expansion.

doi: 10.1103/PhysRevC.19.2378
Citations: PlumX Metrics


1978WO14      Phys.Rev. C18, 2052 (1978)

C.Wong, S.D.Bloom, S.M.Grimes, R.F.Hausman, Jr., V.A.Madsen

Population of the 1+ Levels in 58Co via the 58Fe(p, n) Reaction

NUCLEAR REACTIONS 58Fe(p, n), E=16, 19.1, 20.2 MeV; measured σ(θ). 58Co deduced 1+ strength distribution, fractional M1 strengths. Compared with reaction data, shell model calculations.

doi: 10.1103/PhysRevC.18.2052
Citations: PlumX Metrics


1976DI04      Nucl.Phys. A259, 75 (1976)

F.S.Dietrich, S.D.Bloom, D.W.Heikkinen

Gamma Decay of Analog States in 49Sc: Jπ = 5/2- and 9/2+

NUCLEAR REACTIONS 48Ca(p, γ), E=6.00-6.17 MeV; measured σ(E, Eγ, θ). 49Sc deduced isobaric analog resonances, Γ, Γγ. Enriched target, NaI detector.

doi: 10.1016/0375-9474(76)90496-6
Citations: PlumX Metrics


1974BL01      Phys.Lett. 48B, 420 (1974)

S.D.Bloom

Difference in the Electronic and Fission Decay Modes for Muonic Atoms

ATOMIC PHYSICS, Mesic-Atoms 238U; calculated electronic, fission decay rate of muonic 238U.

doi: 10.1016/0370-2693(74)90369-4
Citations: PlumX Metrics


1973BL01      Nucl.Phys. A199, 369 (1973)

S.D.Bloom, J.B.McGrory, S.A.Moszkowski

Analog and Configuration States in 49Sc(Jπ = 3/2- and 1/2-) and the Low-Lying Level Structure in 48Sc

NUCLEAR STRUCTURE 49,48Sc; calculated levels, B(M1), B(E2), Coulomb displacement energies, wave functions.

doi: 10.1016/0375-9474(73)90555-1
Citations: PlumX Metrics


1972BL01      Phys.Rev. C5, 238 (1972)

S.D.Bloom, M.S.Weiss, C.M.Shakin

Nuclear γ Rays Following K- Capture

NUCLEAR REACTIONS 16O, 208Pb(K-, Xγ), E approx 0; calculated capture rates.

doi: 10.1103/PhysRevC.5.238
Citations: PlumX Metrics


1970MA02      Nucl.Phys. A140, 598 (1970)

L.G.Mann, S.D.Bloom

β-γ(CP) Correlation Measurements and Anti-Analogue Structure in the Decay of 49Ca

RADIOACTIVITY 49Ca[from 48Ca(d, p)]; measured βγ-CP; deduced Fermi matrix element. 49Sc deduced isobaric analog, anti-analog state, J, π.

doi: 10.1016/0375-9474(70)90582-8
Citations: PlumX Metrics


1969AN06      Phys.Rev. 177, 1416(1969)

J.D.Anderson, S.D.Bloom, C.Wong, W.F.Hornyak, V.A.Madsen

Effective Two-Body Force Inferred from the (p, n) Reaction on 17O, 18O, 27Al, and Other Light Nuclei

NUCLEAR REACTIONS 17,18O, 27Al(p, n), E=7-13.5 MeV; measured σ(Ep; En, θ); deduced optical-model parameters.

doi: 10.1103/PhysRev.177.1416
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1016.


1969BI06      Nucl.Phys. A134, 620 (1969)

R.A.Bigoni, S.D.Bloom, K.G.Tirsell

Beta-Gamma (CP) Correlation and Gamma Spectroscopy in 27Mg

RADIOACTIVITY 27Mg [from 26Mg(d, p)]; measured Eγ, Iγ, βγ-CP; deduced log ft. 27Al deduced levels, γ-mixing. Ge(Li) detector.

doi: 10.1016/0375-9474(69)90025-6
Citations: PlumX Metrics


1969DI01      Nucl.Phys. A123, 481 (1969)

W.C.Dickinson, S.D.Bloom, L.G.Mann

High-Resolution Ge(Li) Study of the Decay of 129gTe and 129mTe

RADIOACTIVITY 129Te [from 128Te(n, γ), 130Te(n, 2n)]; measured Eγ, Iγ, γγ-coin, deduced level, log ft. 129I deduced levels, J, π. Enriched targets, Ge(Li) detector.

doi: 10.1016/0375-9474(69)90998-1
Citations: PlumX Metrics


1968AT03      Nucl.Phys. A114, 143 (1968)

J.Atkinson, L.G.Mann, K.G.Tirsell, S.D.Bloom

Coulomb Matrix Elements from β-γ (CP) Correlation Measurements in 57Ni and 65Ni

RADIOACTIVITY 57,65Ni[from 54Fe(α, n), 64Ni(n, γ)]; measured βγ-CP (circular-polarization correlation); deduced Coulomb matrix elements. Enriched targets.

doi: 10.1016/0375-9474(68)90821-X
Citations: PlumX Metrics


1968WA15      Phys.Rev. 171, 1178 (1968)

E.K.Warburton, J.W.Olness, S.D.Bloom, A.R.Poletti

E2 and M1 Matrix Elements in B10

NUCLEAR STRUCTURE 11B, 10B; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.171.1178
Citations: PlumX Metrics


1967BL10      Nucl.Phys. A93, 252(1967)

S.D.Bloom, L.G.Mann

β-γ (CP) Correlation Measurements and the Spin of 52V

RADIOACTIVITY 52V[from 51V(d, p)]; measured β (CP γ) (θ). 52V deduced J. Natural target.

doi: 10.1016/0375-9474(67)90268-0
Citations: PlumX Metrics


1967MA04      Nucl.Phys. A97, 425 (1967)

L.G.Mann, K.G.Tirsell, S.D.Bloom

64Ga Spin from β-γ(CP) Correlation Data and Decay to 64Zn levels

RADIOACTIVITY 64Ga[from 64Zn(p, n)]; measured Eγ, Iγ, γγ-coin, β(CP γ) (θ); deduced J, π; log ft, Fermi, Coulomb matrix elements. 64Zn deduced levels, J, π. Enriched target, Ge(Li) detector.

doi: 10.1016/0375-9474(67)90497-6
Citations: PlumX Metrics


1967TI01      Bull.Am.Phys.Soc. 12, No.1, 75, EG16 (1967)

K.G.Tirsell, S.D.Bloom

Beta Circularly Polarized γ Measurements in Ga72 Decay

NUCLEAR STRUCTURE 72Ga; measured not abstracted; deduced nuclear properties.


1967TI05      Nucl.Phys. A103, 461 (1967)

K.G.Tirsell, S.D.Bloom

β-γ(CP) Correlation Studies of 72Ga and Spin Assignments in 72Ge

RADIOACTIVITY 72Ga [from 71Ga(n, γ)]; measured β (CP γ)(θ). 72Ge levels deduced J, delta(M2/E1), Fermi, Coulomb matrix elements.

doi: 10.1016/0375-9474(67)90265-5
Citations: PlumX Metrics


1966BL09      Phys.Rev. 147, 789 (1966)

S.D.Bloom, L.G.Mann

Fermi and Coulomb Matrix Elements from β-γ (Circularly Polarized) Correlation Measurements on V48 and Mn52m

NUCLEAR STRUCTURE 52Mn, 48V; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.147.789
Citations: PlumX Metrics


1966MA45      Bull.Am.Phys.Soc. 11, No.3, 409, KB15 (1966)

L.G.Mann, K.G.Tirsell, S.D.Bloom

Circularly Polarized γ Measurements in Ga64 Decay

NUCLEAR STRUCTURE 64Ga; measured not abstracted; deduced nuclear properties.


1965BL07      Phys.Rev.Letters 15, 264 (1965)

S.D.Bloom, J.D.Anderson, W.F.Hornyak, C.Wong

Spin-Spin Interaction and the Reaction O18(p, n)F18

NUCLEAR STRUCTURE 18O; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.15.264
Citations: PlumX Metrics


1965CA08      Nucl.Phys. 73, 174 (1965)

D.C.Camp, L.G.Mann, S.D.Bloom

Circular Polarization Measurements and First-Forbidden Matrix Elements In 72Ga and 124Sb

RADIOACTIVITY 72Ga [from Ga(n, γ)], 124Sb; measured βγ circular polarization; deduced nuclear matrix elements. Natural Ga target.

doi: 10.1016/0029-5582(65)90164-1
Citations: PlumX Metrics


1965MA28      Phys.Rev. 139, B540 (1965)

L.G.Mann, S.D.Bloom

β-γ(Circularly Polarized) Correlation Measurements in F20 and Al28

NUCLEAR STRUCTURE 28Al, 20F; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.139.B540
Citations: PlumX Metrics


1964BL04      Phys. Rev. 134, B481 (1964)

S.D.Bloom, L.G.Mann, R.Polichar, J.R.Richardson, A.Scott

Circular Polarization Measurement of Gamma Rays Following Beta Decay of Al24 and Na24 to Determine the Meson Exchange Effect

NUCLEAR STRUCTURE 24Al, 24Na; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.134.B481
Citations: PlumX Metrics


1964BL05      Nuovo Cimento 32, 1023 (1964)

S.D.Bloom

Isotopic-Spin Conservation in Allowed β-Transitions and Coulomb Matrix Elements

doi: 10.1007/BF02733868
Citations: PlumX Metrics


1964CA06      Bull. Am. Phys. Soc. 9, No. 4, 496, KA2 (1964)

D.C.Camp, L.G.Mann, S.D.Bloom

β-γ (Circularly Polarized) Correlation in First-Forbidden Transitions: 124Sb and 72Ga

NUCLEAR STRUCTURE 124Sb, 72Ga; measured not abstracted; deduced nuclear properties.


1963MA11      Bull.Am.Phys.Soc. 8, No.4, 330, J1 (1963)

L.G.Mann, S.D.Bloom, J.R.Richardson

γ-Ray Circular-Polarization Measurement following Al24 and Na24 β Decay

NUCLEAR STRUCTURE 24Al, 24Na; measured not abstracted; deduced nuclear properties.


1963MA35      Conf.Low Medium Energy Nucl.Phys., Univ.Manchester, p.11 (1963)

L.G.Mann, S.D.Bloom, A.Scott, R.Polichar, J.R.Richardson

Circular Polarization Measurements in Na24 and Al24 to Determine the Mesonic Exchange Effect in β Decay

NUCLEAR STRUCTURE 24Na, 24Al; measured not abstracted; deduced nuclear properties.


1963MI16      Phys.Rev. 132, 1130 (1963)

J.A.Miskel, L.G.Mann, S.D.Bloom

β-γ Circular-Polarization Correlation Study of Sc46

NUCLEAR STRUCTURE 46Sc; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.132.1130
Citations: PlumX Metrics


1962BL02      Phys.Rev. 125, 2021 (1962)

S.D.Bloom, L.G.Mann, J.A.Miskel

Isospin Conservation and β-γ Circular-Polarization Correlation in Mixed Transitions

NUCLEAR STRUCTURE 22Na, 60Co, 52Mn, 46Sc, 44Sc, 41Ar, 24Na; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.125.2021
Citations: PlumX Metrics


1962MA13      Nucl.Phys. 30, 636 (1962)

L.G.Mann, S.D.Bloom, R.J.Nagle

Isospin Conservation in the β-Decay of Sc44, Zr95 and Nb95

NUCLEAR STRUCTURE 95Zr, 95Nb, 44Sc; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(62)90082-2
Citations: PlumX Metrics


1962MA29      Phys.Rev. 127, 2134 (1962)

L.G.Mann, S.D.Bloom, R.J.Nagel

Circular Polarization Measurements in the β Decay of V48, Co56, Fe59, and Cs134

NUCLEAR STRUCTURE 134Ce, 59Fe, 56Co, 48V; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.127.2134
Citations: PlumX Metrics


1961AL07      Phys.Rev. 122, 862 (1961)

R.D.Albert, S.D.Bloom, N.K.Glendenning

(p, n) Angular Distributions from Mirror Nucleus Targets: C13, B11, and Be9

NUCLEAR STRUCTURE 9Be, 11B, 13C; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.122.862
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1849.


1961BL06      Bull.Am.Phys.Soc. 6, No.4, 334, B3 (1961)

S.D.Bloom, L.G.Mann, R.J.Nagle

Isospin Conservation in the β Decay of Sc44

NUCLEAR STRUCTURE 44Sc; measured not abstracted; deduced nuclear properties.


1961BL12      Proc.Rutherford Jubilee Intern.Conf., Manchester, England, J.B.Birks, Ed., Academic Press, New York, 733 (1961)

S.D.Bloom, L.G.Mann

Isospin Conservation and β-γ Circular-Polarization Correlation


1961WO03      Phys.Rev. 123, 598 (1961)

C.Wong, J.D.Anderson, S.D.Bloom, J.W.McClure, B.D.Walker

Angular Distribution of the Ground-State Neutrons from the C13(p, n)N13 and N15(p, n)O15 Reactions

NUCLEAR STRUCTURE 15O, 13N, 15N, 13C; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.123.598
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0494.


1960BL01      Bull.Am.Phys.Soc. 5, No.1, 9, B2 (1960)

S.D.Bloom, L.G.Mann, J.A.Miskel

γ Circular Polarization in Ar41 and Isotopic Spin Conservation

NUCLEAR STRUCTURE 41Ar; measured not abstracted; deduced nuclear properties.


1960BL08      Phys.Rev.Letters 5, 326 (1960)

S.D.Bloom, L.G.Mann, J.A.Miskel

Isotopic Spin Conservation and Beta-Gamma Circular Polarization Correlation in A41 and Sc46

NUCLEAR STRUCTURE 41Ar, 46Sc; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.5.326
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1960BL09      Nuovo Cimento 17, 304 (1960)

S.D.Bloom, J.L.Uretsky

NUCLEAR STRUCTURE 7Be; measured not abstracted; deduced nuclear properties.


1960WO04      Bull.Am.Phys.Soc. 5, No.5, 346, F5 (1960)

C.Wong, J.D.Anderson, S.D.Bloom, J.McClure, B.D.Walker

Angular Distribution of the Ground-State Neutrons from the C13(p, n)N13 and N15(p, n)O15 Reactions

NUCLEAR STRUCTURE 13N, 15O; measured not abstracted; deduced nuclear properties.


1958AP48      Phys.Rev. 109, 2211 (1958)

H.Appel, H.Schopper, S.D.Bloom

(β, γ) Circular Polarization Correlation for Co60 and Na22

doi: 10.1103/PhysRev.109.2211
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1958BL55      Bull.Am.Phys.Soc. 3, No.8, 418, N4 (1958)

S.D.Bloom, R.M.Lemmon, S.A.Moszkowski

C13(p, n)N13ground state Excitation Function from 3 to 11.5 MeV


1958MA33      Phys.Rev.Letters 1, 34 (1958)

L.G.Mann, J.A.Miskel, S.D.Bloom

Circular Polarization of A37 Internal Bremsstrahlung

doi: 10.1103/PhysRevLett.1.34
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1957BL01      Phil.Mag. 2, 57 (1957)

S.D.Bloom, B.J.Toppel, D.H.Wilkinson

Isotope Spin Selection Rules. IX. The 9.58 MeV State of 16O

doi: 10.1080/14786435708231722
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1957BL02      Phys.Rev. 105, 232 (1957)

S.D.Bloom, C.M.Turner, D.H.Wilkinson

Lifetime of the First Excited State of B10

doi: 10.1103/PhysRev.105.232
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1957WI27      Phil.Mag. 2, 63 (1957)

D.H.Wilkinson, S.D.Bloom

Isotopic Spin Selection Rules. XI. The 8.06 and 6.23 MeV States of 14N

doi: 10.1080/14786435708231724
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1956MU96      Phys.Rev. 103, 720 (1956)

C.O.Muehlhause, S.D.Bloom, H.E.Wegner, G.N.Glasoe

Neutron Scattering From Iron And Carbon By Time-Of-Flight

NUCLEAR REACTIONS C(n, n), C(n, x), Fe(n, n), Fe(n, n'), Fe(n, x), E=1.4-1.6 MeV; measured products, C, Fe; deduced σ(θ), σ, σ(E). Data were imported from EXFOR entry 11316.

doi: 10.1103/PhysRev.103.720
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset11316.


1953TO18      Phys.Rev. 91, 473 PA8 (1953)

B.J.Toppel, S.D.Bloom

The A36(n, α)S33 reaction

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset11561.


1952BL53      Phys.Rev. 88, 312 (1952)

S.D.Bloom

Internal Pair Conversion in Mg24

doi: 10.1103/PhysRev.88.312
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