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NSR database version of April 27, 2024.

Search: Author = M.Friedman

Found 22 matches.

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2024SA12      Phys.Rev. C 109, 025808 (2024)

R.N.Sahoo, M.Paul, Y.Kashiv, M.Tessler, M.Friedman, S.Halfon, A.Kreisel, A.Shor, L.Weissman

Stellar s-process neutron capture cross section of Ce isotopes

doi: 10.1103/PhysRevC.109.025808
Citations: PlumX Metrics


2023SU03      Phys.Lett. B 839, 137801 (2023)

L.J.Sun, C.Fry, B.Davids, N.Esker, C.Wrede, M.Alcorta, S.Bhattacharjee, M.Bowry, B.A.Brown, T.Budner, R.Caballero-Folch, L.Evitts, M.Friedman, A.B.Garnsworthy, B.E.Glassman, G.Hackman, J.Henderson, O.S.Kirsebom, J.Lighthall, P.Machule, J.Measures, M.Moukaddam, J.Park, C.Pearson, D.Perez-Loureiro, C.Ruiz, P.Ruotsalainen, J.Smallcombe, J.K.Smith, D.Southall, J.Surbrook, L.E.Weghorn, M.Williams

First application of Markov chain Monte Carlo-based Bayesian data analysis to the Doppler-shift attenuation method

NUCLEAR REACTIONS 3He(32S, α)31S, E=128 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies, levels, T1/2, resonances. Comparison with the shell-model code NuShellX calculations. Modern Markov chain Monte Carlo-based Bayesian statistical techniques. The Doppler Shift Lifetimes (DSL2) facility at the TRIUMF Isotope Separator and Accelerator (ISAC-II) facility.

doi: 10.1016/j.physletb.2023.137801
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


2022BU14      Phys.Rev.Lett. 128, 182701 (2022)

T.Budner, M.Friedman, C.Wrede, B.A.Brown, J.Jose, D.Perez-Loureiro, L.J.Sun, J.Surbrook, Y.Ayyad, D.W.Bardayan, K.Chae, A.A.Chen, K.A.Chipps, M.Cortesi, B.Glassman, M.R.Hall, M.Janasik, J.Liang, P.O'Malley, E.Pollacco, A.Psaltis, J.Stomps, T.Wheeler

Constraining the 30P(p, γ)31S Reaction Rate in ONe Novae via the Weak, Low-Energy, β-Delayed Proton Decay of 31Cl

RADIOACTIVITY 31Cl(β+p) [from 9Be(36Ar, X), E=150 MeV/nucleon]; measured decay products, Eβ, Iβ, Ep, Ip; deduced β-delayed proton spectra, the weakest β-delayed proton intensity ever measured, resonance parameters, astrophysical reaction rates. The Gaseous Detector with Germanium Tagging (GADGET), the Coupled Cyclotron Facility at MSU.

doi: 10.1103/PhysRevLett.128.182701
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


2022PA36      Eur.Phys.J. A 58, 207 (2022)

M.Paul, M.Tessler, M.Friedman, S.Halfon, L.Weissman

The liquid-lithium target at the soreq applied research accelerator facility

doi: 10.1140/epja/s10050-022-00863-y
Citations: PlumX Metrics


2021AS06      Phys.Rev. C 103, L051302 (2021)

J.Ash, H.Iwasaki, T.Mijatovic, T.Budner, R.Elder, B.Elman, M.Friedman, A.Gade, M.Grinder, J.Henderson, B.Longfellow, A.Revel, D.Rhodes, M.Spieker, Y.Utsuno, D.Weisshaar, C.Y.Wu

Cross-shell excitations in 46Ca studied with fusion reactions induced by a reaccelerated rare isotope beam

NUCLEAR REACTIONS 7Li(45K, 2nα)46Ca, E=4.66 MeV/nucleon, [secondary 45K beam from 9Be(48Ca, X) primary reaction, followed by separation of fragments using A1900 fragment separator at NSCL-MSU]; measured charged-particle recoils, Eγ, Iγ, (particle)γγ-coin using JANUS array of SeGA array of sixteen 32-fold segmented HPGe detectors, and an annular double-sided silicon detector. 46Ca; deduced levels, J, π, rotational-like band built on the excited 0+ state, configurations. Comparison with shell-model calculations in the sd-pf-sdg orbital space.

doi: 10.1103/PhysRevC.103.L051302
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Data from this article have been entered in the XUNDL database. For more information, click here.


2021SU03      Phys.Rev. C 103, 014322 (2021)

L.J.Sun, M.Friedman, T.Budner, D.Perez-Loureiro, E.Pollacco, C.Wrede, B.A.Brown, M.Cortesi, C.Fry, B.E.Glassman, J.Heideman, M.Janasik, A.Kruskie, A.Magilligan, M.Roosa, J.Stomps, J.Surbrook, P.Tiwari

25Si β+-decay spectroscopy

RADIOACTIVITY 25Si(β+), (EC), (β+p)[from 9Be(36Ar, X), E=150 MeV/nucleon from the K500 and K1200 Coupled Cyclotron Facility at NSCL-MSU, followed by purification of 25Si beam by A1900 fragment separator]; measured Eγ, Iγ, γγ- and pγ-coin, E(p), I(p), half-life of 25Si decay using the Gaseous Detector with Germanium Tagging (GADGET) system of a proton detector and the SeGA array. 24Mg, 25Al; deduced levels, J, π, %Iβ+ feedings, %Iβp, γ branching ratios, logft, B(GT), Γγp and half-life for the 2673-keV level in 25Al, Γγ and Γγp for T=3/2 IAS in 25Al at 7902 keV. Comparison with shell-model calculations of levels, Jπ, β feedings, logft and B(GT) using USDC and USDI Hamiltonians, and with the experimental and theoretical decay characteristics of 25Na β- decay to 25Mg. Comparison with earlier experimental results.

doi: 10.1103/PhysRevC.103.014322
Citations: PlumX Metrics


2020FR04      Phys.Rev. C 101, 052802 (2020)

M.Friedman, T.Budner, D.Perez-Loureiro, E.Pollacco, C.Wrede, J.Jose, B.A.Brown, M.Cortesi, C.Fry, B.Glassman, J.Heideman, M.Janasik, M.Roosa, J.Stomps, J.Surbrook, P.Tiwari

Low-energy 23Al β-delayed proton decay and 22Na destruction in novae

RADIOACTIVITY 23Al(β+), (β+p)[from 9Be(36Ar, X), E=150 MeV/nucleon]; measured Ep, Ip, Eγ, Iγ, γp-coin, β-delayed proton branching ratios using the Gaseous Detector with Germanium Tagging (GADGET) detector at the NSCL-MSU facility. Comparison with previous experimental values of β-delayed proton branching ratios.

NUCLEAR REACTIONS 22Na(p, γ), E(cm)=204 keV; deduced Γp/Γ and resonance strength for the 204-keV proton resonance (7.79-MeV, (7/2) state in 23Mg), and compared with previous experimental values.

doi: 10.1103/PhysRevC.101.052802
Citations: PlumX Metrics


2020FR05      Eur.Phys.J. A 56, 155 (2020)

M.Friedman

Production of quasi-stellar neutron field at explosive stellar temperatures

doi: 10.1140/epja/s10050-020-00170-4
Citations: PlumX Metrics


2019AB12      J.Phys.(London) G46, 100501 (2019)

E.P.Abel, M.Avilov, V.Ayres, E.Birnbaum, G.Bollen, G.Bonito, T.Bredeweg, H.Clause, A.Couture, J.DeVore, M.Dietrich, P.Ellison, J.Engle, R.Ferrieri, J.Fitzsimmons, M.Friedman, D.Georgobiani, S.Graves, J.Greene, S.Lapi, C.S.Loveless, T.Mastren, C.Martinez-Gomez, S.McGuinness, W.Mittig, D.Morrissey, G.Peaslee, F.Pellemoine, J.D.Robertson, N.Scielzo, M.Scott, G.Severin, D.Shaughnessy, J.Shusterman, J.Singh, M.Stoyer, L.Sutherlin, A.Visser, J.Wilkinson

Isotope harvesting at FRIB: additional opportunities for scientific discovery

doi: 10.1088/1361-6471/ab26cc
Citations: PlumX Metrics


2019GL02      Phys.Rev. C 99, 065801 (2019)

B.E.Glassman, D.Perez-Loureiro, C.Wrede, J.Allen, D.W.Bardayan, M.B.Bennett, K.A.Chipps, M.Febbraro, M.Friedman, C.Fry, M.R.Hall, O.Hall, S.N.Liddick, P.O'Malley, W.-J.Ong, S.D.Pain, S.B.Schwartz, P.Shidling, H.Sims, L.J.Sun, P.Thompson, H.Zhang

Doppler broadening in 20Mg(βpγ)19Ne decay

RADIOACTIVITY 20Mg(β+p)[20Mg beam from 9Be(24Mg, X), E=170 MeV/nucleon, followed by separation using A1900 separator at NSCL-MSU]; measured Eβ+, Eγ, Iγ, β+γ-coin, γ-decay branching ratios, and E(p) using plastic scintillator for β detection and the SeGA array for γ detection. 19Ne; deduced levels, J, π, half-life of 1507.5 level from Doppler broadening analysis, β+p feedings. Comparison with previous experimental values. Discussed relevance to 15O(α, γ)19Ne thermonuclear reaction rates.

NUCLEAR REACTIONS 9Be(24Mg, X)15N/16O/17F/18Ne/20Mg, E=170 MeV/nucleon; measured time of flight, particle identification plot, yields using A1900 fragment separator at the K500 and K1200 coupled cyclotrons of NSCL-MSU.

doi: 10.1103/PhysRevC.99.065801
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


2019PA22      Eur.Phys.J. A 55, 44 (2019)

M.Paul, M.Tessler, M.Friedman, S.Halfon, T.Palchan, L.Weissman, A.Arenshtam, D.Berkovits, Y.Eisen, I.Eliahu, G.Feinberg, D.Kijel, A.Kreisel, I.Mardor, G.Shimel, A.Shor, I.Silverman

Reactions along the astrophysical s-process path and prospects for neutron radiotherapy with the Liquid-Lithium Target (LiLiT) at the Soreq Applied Research Accelerator Facility (SARAF)

NUCLEAR REACTIONS 7Li(p, n)7Be, E=1880.4 - 1.92 keV[reaction threshold]; measured thick-target Eγ, Iγ(θ) using the Liquid-Lithium Target (LiLiT) system with the Soreq Applied Research Accelerator Facility (SARAF) Phase I; deduced astrophysical s-process sequence of nuclei.

doi: 10.1140/epja/i2019-12723-5
Citations: PlumX Metrics


2018AB06      Phys.Rev. C 98, 024309 (2018)

E.Aboud, M.B.Bennett, C.Wrede, M.Friedman, S.N.Liddick, D.Perez-Loureiro, D.W.Bardayan, B.A.Brown, A.A.Chen, K.A.Chipps, C.Fry, B.E.Glassman, C.Langer, E.I.McNeice, Z.Meisel, W.-J.Ong, P.D.O'Malley, S.D.Pain, C.J.Prokop, H.Schatz, S.B.Schwartz, S.Suchyta, P.Thompson, M.Walters, X.Xu

Toward complete spectroscopy using β decay: The example of 32Cl (βγ)32S

RADIOACTIVITY 32Cl(β+), (EC)[from 9Be(36Ar, X), E=150 MeV/nucleon followed by beam separation and purification using A1900 fragment separator and time-of-flight separation method using Radio Frequency Fragment Separator (RFFS) at NSCL-MSU]; measured Eγ, Iγ, βγ- and βγγ-coin using the Clovershare array of HPGe detectors, 32Cl implants and β by a plastic scintillator at NSCL-MSU. 32S; deduced levels, J, π, β feedings, logft, Gamow-Teller strengths, half-lives, proton, γ and α widths of 8861- and 9650-keV resonances. Comparison with sd USDA and USDB shell model calculations, and with previous experimental values and ENSDF evaluations. 31P(p, α)28Si, E=9650 keV; deduced resonance strength.

doi: 10.1103/PhysRevC.98.024309
Citations: PlumX Metrics


2018GL01      Phys.Lett. B 778, 397 (2018)

B.E.Glassman, D.Perez-Loureiro, C.Wrede, J.Allen, D.W.Bardayan, M.B.Bennett, B.A.Brown, K.A.Chipps, M.Febbraro, M.Friedman, C.Fry, M.R.Hall, O.Hall, S.N.Liddick, P.O'Malley, W.J.Ong, S.D.Pain, C.Prokop, S.B.Schwartz, P.Shidling, H.Sims, P.Thompson, H.Zhang

β-delayed γ decay of 20Mg and the 19Ne(p, γ)20Na breakout reaction in Type I X-ray bursts

RADIOACTIVITY 20Mg(β+) [from 9Be(24Mg, X)20Mg, E=170 MeV/nucleon]; measured decay products, Eβ, Iβ, Eγ, Iγ; deduced γ-ray energies and limits on intensities of β-delayed γ-rays, Gamow-Teller strengths B(GT) and associated log ft values. Comparison with theoretical calculations.

doi: 10.1016/j.physletb.2018.01.041
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


2017SH47      Phys.Rev. C 96, 055805 (2017)

A.Shor, M.Tessler, A.Plompen, A.Arenshtam, O.Aviv, D.Berkovits, M.Brandis, Y.Eisen, I.Eliyahu, G.Feinberg, M.Friedman, S.Halfon, M.Hult, B.Kaizer, D.Kijel, A.Krasa, A.Kreisel, T.Palchan, M.Paul, A.Perry, I.Silverman, S.Vaintraub, L.Weissman

Bismuth activation with quasi-Maxwellian neutrons at kT ∼ 30 keV

NUCLEAR REACTIONS 209Bi(n, γ), kT≈30 keV quasi-Maxwellian neutrons; measured Eβ from the decay of 210Bi and Eα and Eγ, Iγ from the decay of 206Po using PIPS silicon detector for particles and HPGe detector for γ rays at the linear accelerator of Soreq Applied Research Accelerator facility (SARAF); deduced Maxwellian averaged (MACS) σ, and compared with previous experimental results, and with evaluated cross sections in the ENDF, JEFF and JENDL data libraries. Relevance to termination point of the s-process cycle of nucleosynthesis in stellar environments.

doi: 10.1103/PhysRevC.96.055805
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31780.


2015TE06      Phys.Lett. B 751, 418 (2015)

M.Tessler, M.Paul, A.Arenshtam, G.Feinberg, M.Friedman, S.Halfon, D.Kijel, L.Weissman, O.Aviv, D.Berkovits, Y.Eisen, I.Eliyahu, G.Haquin, A.Kreisel, I.Mardor, G.Shimel, A.Shor, I.Silverman, Z.Yungrais

Stellar 30-keV neutron capture in 94, 96Zr and the 90Zr(γ, n)89Zr photonuclear reaction with a high-power liquid-lithium target

NUCLEAR REACTIONS 94,96Zr(n, γ), E=30 keV; 90Zr(γ, n), E not given; measured reaction products, Eγ, Iγ; deduced yields, Maxwellian averaged σ. Comparison with available data.

doi: 10.1016/j.physletb.2015.10.058
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31765.


2013FR01      Nucl.Instrum.Methods Phys.Res. A698, 117 (2013)

M.Friedman, D.Cohen, M.Paul, D.Berkovits, Y.Eisen, G.Feinberg, G.Giorginis, S.Halfon, A.Krasa, A.J.M.Plompen, A.Shor

Simulation of the neutron spectrum from the 7Li(p, n) reaction with a liquid-lithium target at Soreq Applied Research Accelerator Facility

NUCLEAR REACTIONS 7Li(p, n), E<3.5 MeV; analyzed available data; deduced neutron source parameters for Maxwellian-averaged σ measurements. Comparison with available data.

doi: 10.1016/j.nima.2012.09.027
Citations: PlumX Metrics


2012FE06      Phys.Rev. C 85, 055810 (2012)

G.Feinberg, M.Friedman, A.Krasa, A.Shor, Y.Eisen, D.Berkovits, D.Cohen, G.Giorginis, T.Hirsh, M.Paul, A.J.M.Plompen, E.Tsuk

Quasi-stellar neutrons from the 7Li(p, n)7Be reaction with an energy-broadened proton beam

NUCLEAR REACTIONS 7Li(p, n)7Be, E=1.85-1.95 MeV; measured time of flight, spectrum, E(n), I(n), σ(θ), narrow and broad-energy proton beam; deduced angle-integrated spectrum and Maxwellian-flux distribution. 27Al(p, γ), E=0.985-1.0 MeV; measured thick-target σ(E). 197Au(n, γ), E<160 keV; measured Eγ, Iγ, average activation σ for neutrons from 7Li(p, n) reaction. Relevance to s-process cross sections.

doi: 10.1103/PhysRevC.85.055810
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23284.


2012FE11      J.Phys.:Conf.Ser. 337, 012044 (2012)

G.Feinberg, A.Shor, D.Berkovits, Y.Eisen, M.Friedman, G.Giorginis, T.Hirsh, A.Krasa, M.Paul, A.Plompen, E.Tsuk

Energy-broadened proton beam for production of quasi-stellar neutrons from the 7Li(p, n)7Be reaction

NUCLEAR REACTIONS 7Li(p, n), E=1912 keV; measured thick target En, In(θ) using ToF with 6Li glass detectors and both narrow- and broad-energy beams; deduced σ(En, θ).

doi: 10.1088/1742-6596/337/1/012044
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1970FR04      Priv.Comm. (1970)

M.H.Friedman, S.Jha, R.W.Bercaw

Particle and Collective Nature of the States in 86Sr


1970FR14      Nucl.Phys. A159, 422 (1970)

M.I.Friedman

Particle-Hole Admixtures to Hartree-Fock in the 2s-1d Shell

NUCLEAR STRUCTURE 20Ne, 24Mg, 28Si, 32S, 36Ar; calculated levels. Particle-hole excitations, Hartree-Fock orbitals.

doi: 10.1016/0375-9474(70)90718-9
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1968MO06      Phys.Letters 26B, 579 (1968); Erratum Phys.Letters 27B, 377 (1968)

R.Moreh, M.Friedman

M1 and E1 Resonant Scattering of Gamma Rays from Neutron Capture in Iron

NUCLEAR REACTIONS 62Ni, 112Cd, 141Pr, 203Tl, 208Pb(γ, γ), E=7.2-7.7 MeV; measured γγ-coin, γ linear polarization correlation. 62Ni, 112Cd, 141Pr, 203Tl, 208Pb levels deduced J, π, γ-multipolarity.

doi: 10.1016/0370-2693(68)90418-8
Citations: PlumX Metrics


1966JH01      Proc.Intern.Conf.Internal Conversion Process, Nashville, Tenn., (1965), J.H.Hamilton, Ed., Academic Press, Inc., New York, p.327 (1966)

S.Jha, M.Friedman, B.Patnaik, J.L.Power

The Conversion Coefficient of Some Gamma Rays in In113, In115, Xe129, and Xe133

NUCLEAR STRUCTURE 115Cd, 113Sn, 133I, 129Cs; measured not abstracted; deduced nuclear properties.


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Note: The following list of authors and aliases matches the search parameter M.Friedman: , M.H.FRIEDMAN, M.I.FRIEDMAN