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NSR database version of May 10, 2024.

Search: Author = J.Ross

Found 23 matches.

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2016HU14      Nat.Phys. 12, 800 (2016)

O.A.Hurricane, D.A.Callahan, D.T.Casey, E.L.Dewald, T.R.Dittrich, T.Doppner, S.Haan, D.E.Hinkel, L.F.Berzak Hopkins, O.Jones, A.L.Kritcher, S.Le Pape, T.Ma, A.G.MacPhee, J.L.Milovich, J.Moody, A.Pak, H.-S.Park, P.K.Patel, J.E.Ralph, H.F.Robey, J.S.Ross, J.D.Salmonson, B.K.Spears, P.T.Springer, R.Tommasini, F.Albert, L.R.Benedetti, R.Bionta, E.Bond, D.K.Bradley, J.Caggiano, P.M.Celliers, C.Cerjan, J.A.Church, R.Dylla-Spears, D.Edgell, M.J.Edwards, D.Fittinghoff, M.A.Barrios Garcia, A.Hamza, R.Hatarik, H.Herrmann, M.Hohenberger, D.Hoover, J.L.Kline, G.Kyrala, B.Kozioziemski, G.Grim, J.E.Field, J.Frenje, N.Izumi, M.Gatu-Johnson, S.F.Khan, J.Knauer, T.Kohut, O.Landen, F.Merrill, P.Michel, A.Moore, S.R.Nagel, A.Nikroo, T.Parham, R.R.Rygg, D.Sayre, M.Schneider, D.Shaughnessy, D.Strozzi, R.P.J.Town, D.Turnbull, P.Volegov, A.Wan, K.Widmann, C.Wilde, C.Yeamans

Inertially confined fusion plasmas dominated by alpha-particle self-heating

doi: 10.1038/nphys3720
Citations: PlumX Metrics

2013RO36      Sci. Rep. 3, 1453 (2013)

J.S.Ross, P.Amendt, L.J.Atherton, M.Dunne, S.H.Glenzer, J.D.Lindl, D.Meeker, E.I.Moses, A.Nikroo, R.Wallace

Lead (Pb) Hohlraum: Target for Inertial Fusion Energy

doi: 10.1038/srep01453
Citations: PlumX Metrics

1998UT02      Phys.Rev. C57, 2731 (1998); Erratum Phys.Rev. C58, 1354 (1998)

S.Utku, J.G.Ross, N.P.T.Bateman, D.W.Bardayan, A.A.Chen, J.Gorres, A.J.Howard, C.Iliadis, P.D.Parker, M.S.Smith, R.B.Vogelaar, M.Wiescher, K.Yildiz

Breakout from the Hot CNO Cycle: The 18F(p, γ) vs 18F(p, α) branching ratio

NUCLEAR REACTIONS 19F(3He, t), (3He, tα), (3He, pt), E=29.8 MeV; 16O(6Li, t), (6Li, 3He), E=32 MeV; measured particle spectra, tp-, tα-coin; deduced reaction rates for 18F + p. 19F deduced levels, resonance features. Astrophysical implications.

doi: 10.1103/PhysRevC.57.2731
Citations: PlumX Metrics

1997IL03      Nucl.Phys. A621, 211c (1997)

C.Iliadis, R.E.Azuma, J.Chow, J.D.King, A.C.Morton, L.Buchmann, M.Dombsky, K.P.Jackson, J.M.D'Auria, U.Giesen, J.G.Ross, H.Schatz, M.Wiescher

Decay Studies of Importance to Explosive Hydrogen Burning

RADIOACTIVITY 36K(β+p), (β+α) [from Ca(p, X), E=500 MeV]; measured α-, proton spectra; deduced log ft. 36Ar deduced α-emitting resonance.

doi: 10.1016/S0375-9474(97)00240-6
Citations: PlumX Metrics

1996LI23      J.Phys.Condens.Matter 8, 865 (1996)

Y.Li, C.Carboni, J.W.Ross, M.A.H.McCausland, D.St.P.Bunbury

Hyperfine Fields at Lanthanide Nuclei in the Intermetallic Compounds of RFe2

NUCLEAR MOMENTS 169Tm; measured spin-echo NMR; deduced hyperfine fields in Tm(0.02)Gd(0.98)Fe2, Tm(0.02)Y(0.98)Fe2 compounds.

doi: 10.1088/0953-8984/8/7/011
Citations: PlumX Metrics

1996LI24      J.Phys.Condens.Matter 8, 1059 (1996)

Y.Li, R.G.Graham, J.W.Ross, M.A.H.McCausland, D.St.P.Bunbury, L.Cao, L.-S.Kong, B.-G.Shen

Hyperfine Splitting of Terbium in Tb2Fe17C(x)

NUCLEAR MOMENTS 159Tb; measured spin-echo NMR, zero-field hfs in Tb2Fe17C(x=1, 1.5, 2); deduced hyperfine parameters, magnetocrystalline anisotropy contribution.

doi: 10.1088/0953-8984/8/8/016
Citations: PlumX Metrics

1995RO22      Phys.Rev. C52, 1681 (1995)

J.G.Ross, J.Gorres, C.Iliadis, S.Vouzoukas, M.Wiescher, R.B.Vogelaar, S.Utku, N.P.T.Bateman, P.D.Parker

Indirect Study of Low-Energy Resonances in 31P(p, α)28Si and 35Cl(p, α)32S

NUCLEAR REACTIONS 31P, 35Cl(3He, d), E=25 MeV; measured particle spectra, γd-, (particle)d-coin; deduced (p, γ), (p, α) reaction rates for 31P, 35Cl. 36Ar deduced levels Γ, J, π, T. 32S deduced levels Γ, J, π, T, resonance strength.

doi: 10.1103/PhysRevC.52.1681
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0794.

1994GI01      Nucl.Phys. A567, 146 (1994)

U.Giesen, C.P.Browne, J.Gorres, J.G.Ross, M.Wiescher, R.E.Azuma, J.D.King, J.B.Vise, M.Buckby

The Influence of Low-Energy Resonances on the Reaction Rate of 18O(α, γ)22Ne

NUCLEAR REACTIONS, ICPND 18O(6Li, 6Li), (6Li, d), E=32 MeV; measured σ(θ); deduced model parameters. 18O(α, γ), E < 1 MeV; measured γ(θ). 18O(p, γ), E ≈ resonance; measured thick target yield curve. 22Ne deduced resonances, J, π, spectroscopic factors, role in 18O(α, γ) reaction rate.

doi: 10.1016/0375-9474(94)90731-5
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1451.

1994GO16      Phys.Rev. C50, R1270 (1994)

J.Gorres, J.Meissner, J.G.Ross, K.W.Scheller, S.Vouzoukas, M.Wiescher, J.D.Hinnefeld

Lifetimes of Levels in 20F

NUCLEAR REACTIONS 19F(d, p), E=2 MeV; measured pγ-coin, Eγ, DSA. 20F levels deduced T1/2.

doi: 10.1103/PhysRevC.50.R1270
Citations: PlumX Metrics

1994IL01      Nucl.Phys. A571, 132 (1994)

C.Iliadis, J.Gorres, J.G.Ross, K.W.Scheller, M.Wiescher, R.E.Azuma, G.Roters, H.P.Trautvetter, H.C.Evans

Explosive Hydrogen Burning of 35Cl

NUCLEAR REACTIONS 35Cl(3He, d), E=15 MeV; measured σ(θ), σ(Ed). 32S(6Li, d), E=32 MeV; measured σ(Ed). 32S(α, γ), E ≈ resonance; measured Eγ, Iγ. 35Cl(p, γ), E ≈ 200-800 keV; measured γ yield vs E , stellar rates. 35Cl(p, X), E=177 keV; measured particle spectra. 36Ar deduced levels, J, π, L, spectroscopic factors, γ-branching ratios, resonance strengths. Deduced no evidence for (p, α) reactions.

doi: 10.1016/0375-9474(94)90345-X
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0908.

1994SC01      Phys.Rev. C49, 46 (1994)

K.W.Scheller, J.Gorres, J.G.Ross, M.Wiescher, R.Harkewicz, D.J.Morrissey, B.M.Sherrill, M.Steiner, N.A.Orr, J.A.Winger

Study of the β-Delayed Neutron Decay of 18N

RADIOACTIVITY 18N(β-) [from 9Be(22Ne, X), E=75 MeV/nucleon]; measured β-delayed neutron spectra, T1/2; deduced log ft. 18O deduced levels, J, π, total branching ratio.

doi: 10.1103/PhysRevC.49.46
Citations: PlumX Metrics

1994VO12      Phys.Rev. C50, 1185 (1994)

S.Vouzoukas, C.P.Browne, U.Giesen, J.Gorres, S.M.Graff, H.Herndl, C.Iliadis, L.O.Lamm, J.Meissner, J.G.Ross, K.Scheller, L.van Wormer, M.Wiescher, A.A.Rollefson

Reaction Rate for 31S(p, γ)32Cl and Its Influence on the SiP Cycle in Hot Stellar Hydrogen Burning

NUCLEAR REACTIONS 32S(3He, t), E=22.5-25 MeV; measured σ(Et), σ(θ); deduced 31S(p, γ) reaction rate, hot stellar hydrogen burning implications. 32Cl deduced level, J, π, C2S, Γγ.

doi: 10.1103/PhysRevC.50.1185
Citations: PlumX Metrics

1993IL01      Nucl.Phys. A559, 83 (1993)

C.Iliadis, J.Gorres, J.G.Ross, K.W.Scheller, M.Wiescher, C.Grama, Th.Schange, H.P.Trautvetter, H.C.Evans

Explosive Hydrogen Burning of 31P

NUCLEAR REACTIONS, ICPND 31P(p, γ), (p, α), E=160-370 keV; 28Si(α, γ), E=2.4-2.6 MeV; measured γ yield vs E; deduced stellar reaction rates, temperature dependence. 32S deduced proton thershold state features.

doi: 10.1016/0375-9474(93)90181-V
Citations: PlumX Metrics

1992IL03      Phys.Rev. C45, 2989 (1992)

C.Iliadis, J.G.Ross, J.Gorres, M.Wiescher, S.M.Graff, R.E.Azuma

Reaction 36Ar(p, γ)37K in Explosive Hydrogen Burning

NUCLEAR REACTIONS, ICPND 36Ar(p, γ), E=0.32-0.93 MeV; measured Eγ, Iγ, γ yield vs E; calculated thermonuclear reaction rate vs temperature. 37K levels deduced branching ratios, resonance strength.

doi: 10.1103/PhysRevC.45.2989
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0108.

1986RO01      Phys.Rev.Lett. 56, 663 (1986)

J.H.Ross, Jr., Zhiyue Wang, C.P.Slichter

NMR Study of the Structure and Motion of Charge-Density Waves in NbSe3

NUCLEAR MOMENTS 93Nb; measured NMR; deduced charge density wave motion, structure in NbSe3.

doi: 10.1103/PhysRevLett.56.663
Citations: PlumX Metrics

1984FO10      Phys.Rev. C30, 79 (1984)

J.L.Foster, Jr., S.E.Darden, M.C.Rozak, J.A.Ross, J.P.Martin, L.Lessard, S.Gales, G.Noury, J.M.Pearson, P.Depommier, M.C.Hermida, M.Ruiz

130Te(p(pol), p1) and 130Te(p, p1(pol)) Reactions on Analog Resonances

NUCLEAR REACTIONS 130Te(polarized p, p), (polarized p, p'), E(cm)=10.1-10.7 MeV; measured σ(θ) vs E, analyzing power vs θ, E, polarization vs θ; deduced optical model parameters. 131I deduced IAR, J, π, configuaration. Coupled-channels analysis.

doi: 10.1103/PhysRevC.30.79
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0096.

1968SN02      J.Phys., C(London) 1, 1662 (1968)

R.E.Snyder, J.W.Ross, D.S.P.Bunbury

Mossbauer Effect Measurements in 176,178,180Hf

NUCLEAR REACTIONS 176,178,180Hf(γ, γ), Eγ=0.08836, 0.09317, 0.0933 MeV; measured Eγ, Mossbauer effect in HfO2, HfB2, Hf. 176,178,180Hf levels deduced quadrupole moment.

doi: 10.1088/0022-3719/1/6/324
Citations: PlumX Metrics

1965HA11      Phys.Rev. 137, B790 (1965)

E.P.Haynes II, J.S.Ross

Isotope Shift in the Spectrum of Erbium I

NUCLEAR STRUCTURE 162Er; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.137.B790
Citations: PlumX Metrics

1964RO11      J.Phys.Soc.Japan 19, 249 (1964)

J.S.Ross, K.Murakawa

Nuclear Moments of Yb173

NUCLEAR STRUCTURE 173Yb, 171Yb; measured not abstracted; deduced nuclear properties.

1962RO19      mit-Lns Progr.Rept. p.59 (May 1962); NYO-2669 (1962)

J.Ross, H.A.Enge

III. The Ni64(d, p)Ni65 Stripping Reaction

NUCLEAR STRUCTURE 65Ni; measured not abstracted; deduced nuclear properties.

1962RO26      Phys.Rev. 128, 1159 (1962); See Also 64Ro11

J.S.Ross, K.Murakawa

Nuclear Quadrupole Moment of Yb173

NUCLEAR STRUCTURE 173Yb; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.128.1159
Citations: PlumX Metrics

1961EN07      mit-Lns Progr.Report p.126 (November 1961)

H.A.Enge, J.A.Ross

NUCLEAR STRUCTURE 65Ni; measured not abstracted; deduced nuclear properties.

1952RO05      Phys.Rev. 85, 559 (1952)

J.S.Ross, K.Murakawa

Hyperfine Structure and Isotope Shift in the Spectrum of Tellurium

doi: 10.1103/PhysRev.85.559
Citations: PlumX Metrics

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Note: The following list of authors and aliases matches the search parameter J.Ross: , J.A.ROSS, J.G.ROSS, J.H.ROSS, J.S.ROSS, J.W.ROSS