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NSR database version of May 6, 2024.
Search: Author = P.McKee
Found 12 matches.
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2023BR10
Phys.Lett. B 847, 138310 (2023)
A.D.Briscoe, R.D.Page, J.Uusitalo, D.T.Joss, M.A.M.AlAqeel, B.Alayed, B.Andel, S.Antalic, K.Auranen, H.Ayatollahzadeh, H.Badran, L.Barber, G.Beeton, M.Birova, V.Bogdanoff, R.M.Clark, J.G.Cubiss, D.M.Cullen, J.Deary, U.Forsberg, T.Grahn, P.T.Greenlees, J.B.Hilton, A.Illana, H.Joukainen, D.S.Judson, R.Julin, H.Jutila, J.M.Keatings, M.Labiche, M.Leino, M.C.Lewis, J.Louko, M.Luoma, I.Martel, A.McCarter, P.P.McKee, P.Mosat, S.N.Nathaniel, O.Neuvonen, D.O'Donnell, J.Ojala, C.A.A.Page, A.M.Plaza, J.Pakarinen, P.Papadakis, E.Parr, J.Partanen, P.Rahkila, P.Ruotsalainen, M.Sandzelius, J.Saren, B.Saygi, J.Smallcombe, J.F.Smith, J.Sorri, C.M.Sullivan, S.Szwec, H.Tann, A.Tolosa-Delgado, E.Uusikyla, M.Venhart, L.J.Waring, G.Zimba
Decay spectroscopy at the two-proton drip line: Radioactivity of the new nuclides 160Os and 156W
RADIOACTIVITY 160Os(α), 156W(β+), (EC), 156Ta(p) [from 106Cd(58Ni, X)160Os, 102Pd(58Ni, X)156Ta, E=310, 294 MeV]; measured decay products, Eα, Iα, Ep, Ip, Eβ, Iβ; deduced α-particles energies, T1/2, an improved value for the half-life of the proton-decaying high-spin isomeric state. Comparison with available data. The recoil separator MARA, the Accelerator Laboratory of the University of Jyvaskyla.
doi: 10.1016/j.physletb.2023.138310
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2022PA09
Phys.Rev. C 105, 034303 (2022)
E.Parr, J.F.Smith, P.T.Greenlees, P.A.Butler, K.Auranen, R.Chapman, D.M.Cox, D.M.Cullen, L.P.Gaffney, T.Grahn, E.T.Gregor, L.Grocutt, A.Herzan, R.-D.Herzberg, D.Hodge, U.Jakobsson, R.Julin, S.Juutinen, J.M.Keatings, J.Konki, M.Leino, P.P.McKee, C.McPeake, D.Mengoni, A.K.Mistry, B.S.Nara Singh, G.G.O'Neill, J.Pakarinen, P.Papadakis, J.Partanen, P.Peura, P.Rahkila, P.Ruotsalainen, M.Sandzelius, J.Saren, M.Scheck, C.Scholey, M.Siciliano, M.Smolen, J.Sorri, P.Spagnoletti, K.M.Spohr, S.Stolze, M.J.Taylor, J.Uusitalo
Single-particle states and parity doublets in odd-Z 221Ac and 225Pa from α-decay spectroscopy
RADIOACTIVITY 225Pa, 221Ac(α)[225Pa from 208Pb(20Ne, 2np), E=105 MeV, 221Ac from 208Pb(18O, 4np), E=95 MeV, 208Pb(20Ne, 2npα), E=105 MeV and 225Pa α decay]; 217Fr(α)[from 221Ac α decay]; 213At(α)[from 217Fr α decay]; measured reaction products, Eα, Iα, Eγ, Iγ, αγ-coin, summed α+ce(K); deduced T1/2 decays of ground states of 225Pa, 221Ac, 217Fr, 213At. 221Ac, 217Fr; deduced levels, J, π, α- and γ-branching ratios, total conversion coefficients, multipolarities, α-hindrance factors, configurations, parity-doublet states in 221Ac. 225Pa; deduced ground state J, π. Comparison with previous experimental data, and with model predictions. RITU gas-filled recoil separator, silicon strip detectors (DSSD) for ion implantation measurements and GREAT spectrometer combined with 3 HPGe clover detectors at the University of Jyvaskyla accelerator facility.
doi: 10.1103/PhysRevC.105.034303
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2019PA45
Phys.Rev. C 100, 044323 (2019)
E.Parr, J.F.Smith, P.T.Greenlees, K.Auranen, P.A.Butler, R.Chapman, D.M.Cox, D.M.Cullen, L.P.Gaffney, T.Grahn, E.T.Gregor, L.Grocutt, A.Herzan, R.-D.Herzberg, D.Hodge, U.Jakobsson, R.Julin, S.Juutinen, J.Keatings, J.Konki, M.Leino, P.P.McKee, C.McPeake, D.Mengoni, A.K.Mistry, K.F.Mulholland, B.S.Nara Singh, G.G.O'Neill, J.Pakarinen, P.Papadakis, J.Partanen, P.Peura, P.Rahkila, P.Ruotsalainen, M.Sandzelius, J.Saren, M.Scheck, C.Scholey, M.Siciliano, M.Smolen, J.Sorri, P.Spagnoletti, K.M.Spohr, S.Stolze, M.J.Taylor, J.Uusitalo
α-decay spectroscopy of the N=130 isotones 218Ra and 220Th: Mitigation of α-particle energy summing with implanted nuclei
RADIOACTIVITY 218Ra(α)[from α-decay of 222Th formed in 208Pb(18O, 4n), E=95 MeV]; 214Rn(α)[from α-decay of 218Ra]; 220Th(α)[from α-decay of 224U formed in 208Pb(20Ne, 4n), E=109 MeV]; 216Ra(α)[from α-decay of 220Th]; measured recoiling evaporation residues using RITU gas-filled recoil separator, Eα, Iα, Eγ, Iγ, αγ-coin, half-lives of decays of 218Ra, 214Rn, 220Th and 216Ra, α-branching ratio for decay to the g.s. and the first 2+ level in 214Rn using the GREAT spectrometer at Jyvaskyla accelerator facility; data analyzed using a newly developed technique to mitigate energy summing due to sequential short-lived α decays from nuclei implanted into a silicon detector. 214Rn; deduced 2+ level, α-hindrance factor. Comparison with previous experimental data.
doi: 10.1103/PhysRevC.100.044323
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2016SZ03
Phys.Rev. C 94, 054314 (2016)
S.V.Szwec, B.P.Kay, T.E.Cocolios, J.P.Entwisle, S.J.Freeman, L.P.Gaffney, V.Guimaraes, F.Hammache, P.P.McKee, E.Parr, C.Portail, J.P.Schiffer, N.de Sereville, D.K.Sharp, J.F.Smith, I.Stefan
Rearrangement of valence neutrons in the neutrinoless double-β decay of 136Xe
NUCLEAR REACTIONS 134Ba(d, p), E=15 MeV; 134Ba(α, 3He), E=40.1 MeV; 136Ba(p, d), E=23 MeV; 134Ba(3He, α), E=32.0 MeV; measured outgoing proton, deuteron, 3He and α spectra, σ(θ) using an Enge split-pole spectrometer at the ALTO Tandem accelerator at IPN-Orsay. DWBA analysis using PTOLEMY code. 135Ba; deduced levels, J, π. 136Xe, 134,136Ba; deduced ground-state neutron occupancies. Comparisons with theoretical calculations using various nuclear-structure models. Relevance to initial and final state in the 0νββ decay mode of 136Xe.
doi: 10.1103/PhysRevC.94.054314
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2012AS01
Phys.Rev. C 85, 015202 (2012)
R.Asaturyan, R.Ent, H.Mkrtchyan, T.Navasardyan, V.Tadevosyan, G.S.Adams, A.Ahmidouch, T.Angelescu, J.Arrington, A.Asaturyan, O.K.Baker, N.Benmouna, C.Bertoncini, H.P.Blok, W.U.Boeglin, P.E.Bosted, H.Breuer, M.E.Christy, S.H.Connell, Y.Cui, M.M.Dalton, S.Danagoulian, D.Day, J.A.Dunne, D.Dutta, N.El Khayari, H.C.Fenker, V.V.Frolov, L.Gan, D.Gaskell, K.Hafidi, W.Hinton, R.J.Holt, T.Horn, G.M.Huber, E.Hungerford, X.Jiang, M.Jones, K.Joo, N.Kalantarians, J.J.Kelly, C.E.Keppel, V.Kubarovsky, Y.Li, Y.Liang, D.Mack, S.P.Malace, P.Markowitz, E.McGrath, P.McKee, D.G.Meekins, A.Mkrtchyan, B.Moziak, G.Niculescu, I.Niculescu, A.K.Opper, T.Ostapenko, P.E.Reimer, J.Reinhold, J.Roche, S.E.Rock, E.Schulte, E.Segbefia, C.Smith, G.R.Smith, P.Stoler, L.Tang, M.Ungaro, A.Uzzle, S.Vidakovic, A.Villano, W.F.Vulcan, M.Wang, G.Warren, F.R.Wesselmann, B.Wojtsekhowski, S.A.Wood, C.Xu, L.Yuan, X.Zheng
Semi-inclusive charged-pion electroproduction off protons and deuterons: Cross sections, ratios, and access to the quark-parton model at low energies
doi: 10.1103/PhysRevC.85.015202
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2012FO06
Phys.Rev.Lett. 108, 092502 (2012)
N.Fomin, J.Arrington, R.Asaturyan, F.Benmokhtar, W.Boeglin, P.Bosted, A.Bruell, M.H.S.Bukhari, M.E.Christy, E.Chudakov, B.Clasie, S.H.Connell, M.M.Dalton, A.Daniel, D.B.Day, D.Dutta, R.Ent, L.El Fassi, H.Fenker, B.W.Filippone, K.Garrow, D.Gaskell, C.Hill, R.J.Holt, T.Horn, M.K.Jones, J.Jourdan, N.Kalantarians, C.E.Keppel, D.Kiselev, M.Kotulla, R.Lindgren, A.F.Lung, S.Malace, P.Markowitz, P.McKee, D.G.Meekins, H.Mkrtchyan, T.Navasardyan, G.Niculescu, A.K.Opper, C.Perdrisat, D.H.Potterveld, V.Punjabi, X.Qian, P.E.Reimer, J.Roche, V.M.Rodriguez, O.Rondon, E.Schulte, J.Seely, E.Segbefia, K.Slifer, G.R.Smith, P.Solvignon, V.Tadevosyan S.Tajima, L.Tang, G.Testa, R.Trojer, V.Tvaskis, W.F.Vulcan, C.Wasko, F.R.Wesselmann, S.A.Wood, J.Wright, X.Zheng
New Measurements of High-Momentum Nucleons and Short-Range Structures in Nuclei
doi: 10.1103/PhysRevLett.108.092502
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2010FO09
Phys.Rev.Lett. 105, 212502 (2010)
N.Fomin, J.Arrington, D.B.Day, D.Gaskell, A.Daniel, J.Seely, R.Asaturyan, F.Benmokhtar, W.Boeglin, B.Boillat, P.Bosted, A.Bruell, M.H.S.Bukhari, M.E.Christy, E.Chudakov, B.Clasie, S.H.Connell, M.M.Dalton, D.Dutta, R.Ent, L.El Fassi, H.Fenker, B.W.Filippone, K.Garrow, C.Hill, R.J.Holt, T.Horn, M.K.Jones, J.Jourdan, N.Kalantarians, C.E.Keppel, D.Kiselev, M.Kotulla, R.Lindgren, A.F.Lung, S.Malace, P.Markowitz, P.McKee, D.G.Meekins, T.Miyoshi, H.Mkrtchyan, T.Navasardyan, G.Niculescu, Y.Okayasu, A.K.Opper, C.Perdrisat, D.H.Potterveld, V.Punjabi, X.Qian, P.E.Reimer, J.Roche, V.M.Rodriguez, O.Rondon, E.Schulte, E.Segbefia, K.Slifer, G.R.Smith, P.Solvignon, V.Tadevosyan, S.Tajima, L.Tang, G.Testa, R.Trojer, V.Tvaskis, W.F.Vulcan, C.Wasko, F.R.Wesselmann, S.A.Wood, J.Wright, X.Zheng
Scaling of the F2 Structure Function in Nuclei and Quark Distributions at χ > 1
doi: 10.1103/PhysRevLett.105.212502
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2009DA11
Phys.Rev. C 80, 015205 (2009)
M.M.Dalton, G.S.Adams, A.Ahmidouch, T.Angelescu, J.Arrington, R.Asaturyan, O.K.Baker, N.Benmouna, C.Bertoncini, W.U.Boeglin, P.E.Bosted, H.Breuer, M.E.Christy, S.H.Connell, Y.Cui, S.Danagoulian, D.Day, T.Dodario, J.A.Dunne, D.Dutta, N.El Khayari, R.Ent, H.C.Fenker, V.V.Frolov, L.Gan, D.Gaskell, K.Hafidi, W.Hinton, R.J.Holt, T.Horn, G.M.Huber, E.Hungerford, X.Jiang, M.K.Jones, K.Joo, N.Kalantarians, J.J.Kelly, C.E.Keppel, V.Kubarovsky, Y.Li, Y.Liang, S.Malace, P.Markowitz, P.McKee, D.G.Meekins, H.Mkrtchyan, B.Moziak, T.Navasardyan, G.Niculescu, I.Niculescu, A.K.Opper, T.Ostapenko, P.E.Reimer, J.Reinhold, J.Roche, S.E.Rock, E.Schulte, E.Segbefia, C.Smith, G.R.Smith, P.Stoler, V.Tadevosyan, L.Tang, V.Tvaskis, M.Ungaro, A.Uzzle, S.Vidakovic, A.Villano, W.F.Vulcan, M.Wang, G.Warren, F.R.Wesselmann, B.Wojtsekhowski, S.A.Wood, C.Xu, L.Yuan, X.Zheng, H.Zhu
Electroproduction of η mesons in the S11(1535) resonance region at high momentum transfer
doi: 10.1103/PhysRevC.80.015205
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2009MA56
Phys.Rev. C 80, 035207 (2009)
S.P.Malace, G.S.Adams, A.Ahmidouch, T.Angelescu, J.Arrington, R.Asaturyan, O.K.Baker, N.Benmouna, H.P.Blok, W.U.Boeglin, P.E.Bosted, H.Breuer, M.E.Christy, Y.Cui, M.M.Dalton, S.Danagoulian, D.Day, J.A.Dunne, D.Dutta, R.Ent, H.C.Fenker, L.Gan, D.Gaskell, K.Hafidi, W.Hinton, R.J.Holt, T.Horn, G.M.Huber, E.Hungerford, X.Jiang, M.Jones, K.Joo, N.Kalantarians, J.J.Kelly, C.E.Keppel, E.R.Kinney, V.Kubarovsky, Y.Li, Y.Liang, P.Markowitz, E.McGrath, P.McKee, D.G.Meekins, H.Mkrtchyan, T.Navasardyan, G.Niculescu, I.Niculescu, P.E.Reimer, J.Reinhold, J.Roche, E.Schulte, E.Segbefia, C.Smith, G.R.Smith, V.Tadevosyan, L.Tang, M.Ungaro, A.Uzzle, S.Vidakovic, A.N.Villano, W.F.Vulcan, F.R.Wesselmann, B.Wojtsekhowski, S.A.Wood, L.Yuan, X.Zheng
Applications of quark-hadron duality in the F2 structure function
doi: 10.1103/PhysRevC.80.035207
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2001ZH20
Phys.Rev.Lett. 87, 081801 (2001)
H.Zhu, A.Ahmidouch, H.Anklin, H.Arenhovel, C.Armstrong, C.Bernet, W.Boeglin, H.Breuer, P.Brindza, D.Brown, S.Bultmann, R.Carlini, N.Chant, A.Cowley, D.Crabb, S.Danagoulian, D.B.Day, T.Eden, R.Ent, Y.Farah, R.Fatemi, K.Garrow, C.Harris, M.Hauger, A.Honegger, J.Jourdan, M.Kaufmann, M.Khandaker, G.Kubon, J.Lichtenstadt, R.Lindgren, R.Lourie, A.Lung, D.Mack, S.Malik, P.Markowitz, K.McFarlane, P.McKee, D.McNulty, G.Milanovich, J.Mitchell, H.Mkrtchyan, M.Muhlbauer, T.Petitjean, Y.Prok, D.Rohe, E.Rollinde, O.A.Rondon, P.Roos, R.Sawafta, I.Sick, C.Smith, T.Southern, M.Steinacher, S.Stepanyan, V.Tadevosyan, R.Tieulent, A.Tobias, W.Vulcan, G.Warren, H.Wohrle, S.Wood, C.Yan, M.Zeier, J.Zhao, B.Zihlmann
Measurement of the Electric Form Factor of the Neutron Through d(pol)(e(pol), e'n)p at Q2 = 0.5 (GeV/c)2
NUCLEAR REACTIONS 2H(polarized e, e'n), E=2.725 GeV; measured electron and neutron spectra, angular distributions, asymmetries. 1n deduced electric form factor. Solid polarized target.
doi: 10.1103/PhysRevLett.87.081801
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1999AN43
Phys.Lett. 463B, 339 (1999)
P.L.Anthony, R.G.Arnold, T.Averett, H.R.Band, M.C.Berisso, H.Borel, P.E.Bosted, S.L.Bultmann, M.Buenerd, T.Chupp, S.Churchwell, G.R.Court, D.Crabb, D.Day, P.Decowski, P.DePietro, R.Erbacher, R.Erickson, A.Feltham, H.Fonvieille, E.Frlez, R.Gearhart, V.Ghazikhanian, J.Gomez, K.A.Griffioen, C.Harris, M.A.Houlden, E.W.Hughes, C.E.Hyde-Wright, G.Igo, S.Incerti, J.Jensen, J.R.Johnson, P.M.King, Yu.G.Kolomensky, S.E.Kuhn, R.Lindgren, R.M.Lombard-Nelsen, J.Marroncle, J.McCarthy, P.McKee, W.Meyer, G.Mitchell, J.Mitchell, M.Olson, S.Penttila, G.Peterson, G.G.Petratos, R.Pitthan, D.Pocanic, R.Prepost, C.Prescott, L.M.Qin, B.A.Raue, D.Reyna, L.S.Rochester, S.Rock, O.A.Rondon-Aramayo, F.Sabatie, I.Sick, T.Smith, L.Sorrell, F.Staley, S.St.Lorant, L.M.Stuart, Z.Szalata, Y.Terrien, A.Tobias, L.Todor, T.Toole, S.Trentalange, D.Walz, R.C.Welsh, F.R.Wesselmann, T.R.Wright, C.C.Young, M.Zeier, H.Zhu, B.Zihlmann
Measurement of the Deuteron Spin Structure Function g1d(x) for 1 (GeV/c)2 < Q2 < 40 (GeV/c)2
NUCLEAR REACTIONS 2H, 6Li(polarized e, e'X), E=48.3 GeV; measured electrons σ(θ), longitudinal asymmetries. 2H deduced spin structure function.
doi: 10.1016/S0370-2693(99)00940-5
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1999BU09
Nucl.Instrum.Methods Phys.Res. A425, 23 (1999)
S.Bultmann, D.G.Crabb, D.B.Day, R.D.Fatemi, B.Gardner, C.M.Harris, J.R.Johnson, J.S.McCarthy, P.M.McKee, W.Meyer, S.I.Penttila, E.Ponikvar, A.Rijllart, O.A.Rondon, S.St.Lorant, W.A.Tobias, S.Trentalange, H.Zhu, B.Zihlmann, D.Zimmermann
A Study of Lithium Deuteride as a Material for a Polarized Target
NUCLEAR REACTIONS 2H, 6,7Li(e, e'X), E at 50 GeV/c; measured lithium deuteride target polarization before, after irradiation. Comparison with other target materials.
doi: 10.1016/S0168-9002(98)01341-2
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Note: The following list of authors and aliases matches the search parameter P.McKee: , P.M.MCKEE, P.P.MCKEE
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