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Search: Author = S.Nagamiya

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2016NA34      Nucl.Phys. A956, 248 (2016)

S.Nagamiya

Heavy Ion Physics in the Future

doi: 10.1016/j.nuclphysa.2016.03.003
Citations: PlumX Metrics


2016NA39      Nucl.Phys. A956, 911 (2016)

S.Nagamiya

My Memory on QM Conferences

doi: 10.1016/j.nuclphysa.2016.01.062
Citations: PlumX Metrics


2016SA40      Nucl.Phys. A956, 850 (2016)

H.Sako, H.Harada, T.Sakaguchi, T.Chujo, S.Esumi, T.Gunji, S.Hasegawa, S.H.Hwang, Y.Ichikawa, K.Imai, K.Itakura, M.Kaneta, B.C.Kim, M.Kinsho, M.Kitazawa, Y.Liu, H.Masui, S.Nagamiya, K.Nishio, M.Okamura, K.Oyama, K.Ozawa, P.K.Saha, A.Sakaguchi, S.Sato, K.Shigaki, H.Sugimura, K.Tanida, J.Tamura, H.Tamura, Y.Nara, T.R.Saito, for the J-PARC and Heavy-Ion Collaboration

Studies of high density baryon matter with high intensity heavy-ion beams at J-PARC

doi: 10.1016/j.nuclphysa.2016.03.030
Citations: PlumX Metrics


2009NA16      Nucl.Phys. A827, 179c (2009)

S.Nagamiya

J-PARC Program Overview

doi: 10.1016/j.nuclphysa.2009.05.033
Citations: PlumX Metrics


2006NA48      Nucl.Phys. A774, 895 (2006)

S.Nagamiya

J-PARC Project in Japan

doi: 10.1016/j.nuclphysa.2006.06.160
Citations: PlumX Metrics


2005NA23      Nucl.Phys. A755, 219c (2005)

S.Nagamiya

Current Status of the J-PARC Project

doi: 10.1016/j.nuclphysa.2005.03.153
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2003NA30      Nucl.Phys. A721, 190c (2003)

S.Nagamiya

Physics Prospects with High Intensity Proton Accelerator (J-PARC) at Tokai

doi: 10.1016/S0375-9474(03)01032-7
Citations: PlumX Metrics


1998BE39      Phys.Rev. C58, 1115 (1998)

M.J.Bennett, J.K.Pope, D.Beavis, J.B.Carroll, J.Chiba, A.Chikanian, H.J.Crawford, M.Cronqvist, Y.Dardenne, R.Debbe, T.Doke, J.Engelage, L.Greiner, R.S.Hayano, T.J.Hallman, H.H.Heckman, T.Kashiwagi, J.Kikuchi, B.S.Kumar, C.Kuo, P.J.Lindstrom, J.W.Mitchell, S.Nagamiya, J.L.Nagle, P.Stankus, K.H.Tanaka, R.C.Welsh, W.Zhan, and the E878 Collaboration

Light Nuclei Production in Relativistic Au + Nucleus Collisions

NUCLEAR REACTIONS 27Al, Cu, 197Au(197Au, X), E at 10.8 GeV/c/nucleon; measured light charged fragments rapidity distributions, multiplicities; deduced coalescence parameters.

doi: 10.1103/PhysRevC.58.1115
Citations: PlumX Metrics


1997AH03      Phys.Rev. C55, 2604 (1997)

L.Ahle, Y.Akiba, D.Beavis, P.Beery, H.C.Britt, B.Budick, C.Chasman, Z.Chen, C.Y.Chi, Y.Y.Chu, V.Cianciolo, B.A.Cole, J.B.Costales, H.J.Crawford, J.B.Cumming, R.Debbe, J.Engelage, S.Y.Fung, M.Gonin, S.Gushue, H.Hamagaki, R.S.Hayano, S.Hayashi, S.Homma, H.Kaneko, J.Kang, S.Kaufman, W.L.Kehoe, K.Kurita, R.J.Ledoux, M.J.LeVine, Y.Miake, D.P.Morrison, R.J.Morse, B.Moskowitz, S.Nagamiya, M.N.Namboodiri, T.Nayak, J.Olness, C.G.Parsons, L.P.Remsberg, D.Roehrich, P.Rothschild, H.Sakurai, T.C.Sangster, R.Seto, K.Shigaki, R.Soltz, P.Stankus, S.G.Steadman, G.S.F.Stephans, T.Sung, Y.Tanaka, M.J.Tannenbaum, J.Thomas, S.Tonse, S.Ueno, J.H.van Dijk, F.Videbaek, O.Vossnack, V.Vutsadakis, F.Q.Wang, Y.Wang, H.E.Wegner, H.E.Wegner, D.S.Woodruff, Y.D.Wu, K.Yagi, X.Yang, D.Zachary, W.A.Zajc, and the E802 Collaboration

Baryon Emission at Target Rapidities in Si + Al, Cu, Au Collisions at 14.6A GeV/c and Au + Au Collisions at 11.7A GeV/c

NUCLEAR REACTIONS 27Al, Cu, 197Au(28Si, X), E at 14.6 GeV/c/nucleon; 197Au(197Au, X), E at 11.7 GeV/c/nucleon; measured light charged particle momentum density distribution; deduced proton distributions at minimum bias target rapidities, pseudorapidity distributions shapes. Model comparison.

doi: 10.1103/PhysRevC.55.2604
Citations: PlumX Metrics


1997AK04      Phys.Rev. C56, 1544 (1997)

Y.Akiba, D.Beavis, P.Beery, H.C.Britt, B.Budick, C.Chasman, Z.Chen, C.Y.Chi, Y.Y.Chu, V.Cianciolo, B.A.Cole, J.B.Costales, H.J.Crawford, J.B.Cumming, R.Debbe, J.Engelage, S.Y.Fung, M.Gonin, S.Gushue, H.Hamagaki, O.Hansen, R.S.Hayano, S.Hayashi, S.Homma, H.Kaneko, J.Kang, S.Kaufman, W.L.Kehoe, K.Kurita, R.J.Ledoux, M.J.Levine, Y.Miake, D.P.Morrison, R.J.Morse, B.Moskowitz, S.Nagamiya, M.N.Namboodiri, T.K.Nayak, J.Olness, C.G.Parsons, L.P.Remsberg, D.Roehrich, P.Rothschild, H.Sakurai, T.C.Sangster, R.Seto, R.Soltz, P.Stankus, S.G.Steadman, G.S.F.Stephans, T.Sung, Y.Tanaka, M.J.Tannenbaum, J.Thomas, S.Tonse, J.H.Van Dijk, F.Videbaek, O.Vossnack, V.Vutsadakis, F.Q.Wang, Y.Wang, H.E.Wegner, D.S.Woodruff, Y.D.Wu, X.Yang, D.Zachary, W.A.Zajc

Two-Particle Rapidity Correlations from the Bose-Einstein Effect in Central 28Si + Au Collisions at 14.6A GeV/c and Intermittency

NUCLEAR REACTIONS 197Au(28Si, X), E at 14.6 GeV/c/nucleon; measured two-pion correlation functions vs Q(inv), rapidity, pseudorapidity; deduced correlation length, Bose-Einstein effect role.

doi: 10.1103/PhysRevC.56.1544
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1997BE44      Phys.Rev. C56, 1521 (1997)

M.J.Bennett, D.Beavis, J.B.Carroll, J.Chiba, A.Chikanian, H.J.Crawford, M.Cronqvist, Y.Dardenne, R.Debbe, T.Doke, J.Engelage, L.Greiner, R.S.Hayano, T.J.Hallman, H.H.Heckman, T.Kashiwagi, J.Kikuchi, B.S.Kumar, C.Kuo, P.J.Lindstrom, J.W.Mitchell, S.Nagamiya, J.L.Nagle, J.K.Pope, P.Stankus, K.H.Tanaka, R.C.Welsh, W.Zhan

Antiproton Distributions in Au + Nucleus Collisions

NUCLEAR REACTIONS 27Al, Cu, 197Au(197Au, X), E at 10.8 GeV/c; measured p-bar invariant production σ, multiplicity at several rigidities, rapidity distributions; deduced centrality, target dependencies. E878 experiment. Longitudinal, radial expansion, transport models.

doi: 10.1103/PhysRevC.56.1521
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1996AK04      Phys.Rev.Lett. 76, 2021 (1996)

Y.Akiba, D.Beavis, P.Beery, H.C.Britt, B.Budick, C.Chasman, Z.Chen, C.Y.Chi, Y.Y.Chu, V.Cianciolo, B.A.Cole, J.B.Costales, H.J.Crawford, J.B.Cumming, R.Debbe, J.Engelage, S.Y.Fung, M.Gonin, S.Gushue, H.Hamagaki, O.Hansen, R.S.Hayano, S.Hayashi, S.Homma, H.Kaneko, J.Kang, S.Kaufman, W.L.Kehoe, K.Kurita, R.J.Ledoux, M.J.Levine, Y.Miake, D.P.Morrison, R.J.Morse, B.Moskowitz, S.Nagamiya, M.N.Namboodiri, T.K.Nayak, J.Olness, C.G.Parsons, L.P.Remsberg, D.Roehrich, P.Rothschild, H.Sakurai, T.C.Sangster, R.Seto, R.Soltz, P.Stankus, S.G.Steadman, G.S.F.Stephans, T.Sung, Y.Tanaka, M.J.Tannenbaum, J.Thomas, S.Tonse, J.H.Van Dijk, F.Videbaek, O.Vossnack, V.Vutsadakis, F.Q.Wang, Y.Wang, H.E.Wegner, D.S.Woodruff, Y.D.Wu, X.Yang, D.Zachary, W.A.Zajc, and the E-802 Collaboration

Production of φ Mesons in Central 28Si + 197Au Collisions at 14.6A GeV/c

NUCLEAR REACTIONS 197Au(28Si, X), E at 14.6 GeV/c/nucleon; measured invariant φ yield; deduced invariant transverse mass distribution width.

doi: 10.1103/PhysRevLett.76.2021
Citations: PlumX Metrics


1995AB18      Phys.Rev. C52, 2663 (1995)

T.Abbott, Y.Akiba, D.Alburger, D.Beavis, P.Beery, M.A.Bloomer, P.D.Bond, C.Chasman, Z.Chen, Y.Y.Chu, B.A.Cole, J.B.Costales, H.J.Crawford, J.B.Cumming, R.Debbe, E.Duek, J.Engelage, S.Y.Fung, L.Grodzins, S.Gushue, H.Hamagaki, O.Hansen, P.Haustein, S.Homma, H.Z.Huang, Y.Ikeda, J.Kang, S.Katcoff, S.Kaufman, R.J.Ledoux, M.J.Levine, P.J.Lindstrom, Y.Miake, R.J.Morse, S.Nagamiya, J.Olness, C.G.Parsons, L.P.Remsberg, H.Sakurai, M.Sarabura, R.Seto, S.G.Steadman, G.S.F.Stephans, T.Sugitate, M.Tanaka, M.J.Tannenbaum, M.Torikoshi, J.H.van Dijk, F.Videbaek, M.Vient, P.Vincent, E.Vulgaris, V.Vutsadakis, W.A.Watson III, H.E.Wegner, D.S.Woodruff, W.A.Zajc, and the E-802 Collaboration

Multiplicity Distributions from Central Collisions of 16O + Cu at 14.6A GeV/c and Intermittency

NUCLEAR REACTIONS Cu(16O, X), E=14.6 GeV/c/nucleon; measured central relativistic collisions associated multiplicity distributions. Negative binomial distributions analysis.

doi: 10.1103/PhysRevC.52.2663
Citations: PlumX Metrics


1995BE45      Phys.Rev.Lett. 75, 3078 (1995)

D.Beavis, M.J.Bennett, J.B.Carroll, J.Chiba, A.Chikanian, H.Crawford, M.Cronqvist, Y.Dardenne, R.Debbe, T.Doke, J.Engelage, L.Greiner, T.J.Hallman, R.S.Hayano, H.H.Heckman, T.Kashiwagi, J.Kikuchi, S.Kumar, C.Kuo, P.J.Lindstrom, J.W.Mitchell, S.Nagamiya, J.L.Nagle, J.K.Pope, P.Stankus, K.H.Tanaka, R.C.Welsh, W.Zhan, and the E878 Collaboration

Search for New Metastable Particles Produced in Au + Au Collisions at 10.8A GeV/c

NUCLEAR REACTIONS 197Au(197Au, X), E at 10.8 GeV/c/nucleon; measured particle production invariant multiplicities, σ; deduced no new metastable particles.

doi: 10.1103/PhysRevLett.75.3078
Citations: PlumX Metrics


1995BE46      Phys.Rev.Lett. 75, 3633 (1995)

D.Beavis, M.J.Bennett, J.B.Carroll, J.Chiba, A.Chikanian, H.Crawford, M.Cronqvist, Y.Dardenne, R.Debbe, T.Doke, J.Engelage, L.Greiner, T.J.Hallman, R.S.Hayano, H.H.Heckman, T.Kashiwagi, J.Kikuchi, S.Kumar, C.Kuo, P.J.Lindstrom, J.W.Mitchell, S.Nagamiya, J.L.Nagle, J.K.Pope, P.Stankus, K.H.Tanaka, R.C.Welsh, W.Zhan, and the E878 Collaboration

Centrality Dependence of Antiproton Production in Au + Au Collisions

NUCLEAR REACTIONS 197Au(197Au, X), E=high; measured p-bar yields vs rapidity; deduced p-bar production, annihilation dynamics related features.

doi: 10.1103/PhysRevLett.75.3633
Citations: PlumX Metrics


1994HA02      Phys.Rev. C49, 420 (1994)

O.Hashimoto, H.Hamagaki, T.Kobayashi, K.Nakayama, Y.Shida, I.Tanihata, O.Yamakawa, N.Yoshikawa, S.Nagamiya, J.A.Bistirlich, K.M.Crowe, T.J.Humanic, M.Justice, J.O.Rasmussen, Y.-W.Xu

Projectile Rapidity Pions in 775 MeV/nucleon 139La + 12C and 139La + 139La Reactions

NUCLEAR REACTIONS 139La, 12C(139La, X), E=775 MeV/nucleon; measured projectile (fragment)(π-)-coin; deduced pion peak position, width. Participant-spectator interaction.

doi: 10.1103/PhysRevC.49.420
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1993AB04      Phys.Rev. C47, R1351 (1993)

T.Abbott, Y.Akiba, D.Beavis, M.A.Bloomer, P.D.Bond, C.Chasman, Z.Chen, Y.Y.Chu, B.A.Cole, J.B.Costales, H.J.Crawford, J.B.Cumming, R.Debbe, J.Engelage, S.-Y.Fung, S.Gushue, H.Hamagaki, O.Hansen, R.Hayano, S.Hayashi, S.Homma, H.Z.Huang, Y.Ikeda, I.Juricic, J.Kang, S.Katcoff, S.Kaufman, K.Kimura, K.Kitamura, K.Kurita, R.J.Ledoux, M.J.Le Vine, Y.Miake, R.J.Morse, B.Moskowitz, S.Nagamiya, J.Olness, C.G.Parsons, L.P.Remsberg, D.Roehrich, H.Sakurai, M.Sarabura, P.Stankus, S.G.Steadman, G.S.F.Stephans, T.Sugitate, M.J.Tannenbaum, J.H.Van Dijk, F.Videbaek, M.Vient, P.Vincent, V.Vutsadakis, H.E.Wegner, D.S.Woodruff, Y.D.Wu, W.A.Zajc, and the E-802 Collaboration

Antiproton Production in p + A Collisions at 14.6 GeV/c

NUCLEAR REACTIONS 9Be, 27Al, Cu(p, p-bar), E at 14.6 GeV/c; measured p-bar production σ, multiplicity.

doi: 10.1103/PhysRevC.47.R1351
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1992AB07      Phys.Rev. D45, 3906 (1992)

T.Abbott, Y.Akiba, D.Beavis, M.A.Bloomer, P.D.Bond, C.Chasman, Z.Chen, Y.Y.Chu, B.A.Cole, J.B.Costales, H.J.Crawford, J.B.Cumming, R.Debbe, J.Engelage, S.Y.Fung, S.Gushue, H.Hamagaki, O.Hansen, R.S.Hayano, S.Hayashi, S.Homma, H.Z.Huang, Y.Ikeda, I.Juricic, J.Kang, S.Katcoff, S.Kaufman, K.Kimura, K.Kitamura, K.Kurita, R.J.Ledoux, M.J.Levine, Y.Miake, R.J.Morse, B.Moskowitz, S.Nagamiya, J.Olness, C.G.Parsons, L.P.Remsberg, H.Sakurai, M.Sarabura, P.Stankus, S.G.Steadman, G.S.F.Stephans, T.Sugitate, M.J.Tannenbaum, J.H.van Dijk, F.Videbaek, M.Vient, P.Vincent, V.Vutsadakis, H.E.Wegner, D.S.Woodruff, Y.D.Wu, W.Zajc, and the E-802 Collaboration

Measurement of Particle Production in Proton-Induced Reactions at 14.6 GeV/c

NUCLEAR REACTIONS 9Be, 27Al, Cu, 197Au(p, xp), (p, xπ+), (p, xπ-), (p, xK+), (p, xK-), (p, xp), E at 14.6 GeV/c; measured invariant particle production σ; deduced particle production mechanism.

doi: 10.1103/PhysRevD.45.3906
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1989SC16      Phys.Rev. C40, 640 (1989)

S.Schnetzer, R.M.Lombard, M.-C.Lemaire, E.Moeller, S.Nagamiya, G.Shapiro, H.Steiner, I.Tanihata

Inclusive Production of K+ Mesons in 2.1-GeV/Nucleon Nuclear Collisions

NUCLEAR REACTIONS Na, F, Pb(p, K+X), E=2 GeV; Pb, Na, F(d, K+X), (Ne, K+X), E=2 GeV/nucleon; Ar(20Ne, K+X), E=2 Gev/nucleon; measured σ(θ) vs kaon momentum; deduced reaction mechanism.

doi: 10.1103/PhysRevC.40.640
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1987KI10      Phys.Rev.Lett. 58, 1508 (1987)

Y.Kitazoe, M.Sano, H.Toki, S.Nagamiya

Pion-Reabsorption Effect on Pion Spectra in High-Energy Heavy-Ion Collisions

NUCLEAR REACTIONS Na, F(Ne, p), (Ne, π-), E=0.8 GeV/nucleon; calculated σ(Ep, θp), σ(Eπ, θπ); deduced slope parameters, multiplicities vs mass. Cascade model.

doi: 10.1103/PhysRevLett.58.1508
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1986KI02      Phys.Lett. 166B, 35 (1986)

Y.Kitazoe, M.Sano, H.Toki, S.Nagamiya

Pion Production Mechanism in High Energy Heavy Ion Collisions

NUCLEAR REACTIONS K, Cl(Ar, π-), E=800-1600 MeV/nucleon; calculated pion multiplicity vs E. Cascade model.

NUCLEAR STRUCTURE A=10-110; calculated charged pion production σ at E=730 MeV. Cascade model.

doi: 10.1016/0370-2693(86)91150-0
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1985MI09      Phys.Rev. C31, 2168 (1985)

Y.Miake, H.Hamagaki, S.Kadota, S.Nagamiya, S.Schnetzer, Y.Shida, H.Steiner, I.Tanihata

Production Mechanism of Backward Energetic Protons Studied from Two-Particle Correlations in 800 MeV Proton-Nucleus Collisions

NUCLEAR REACTIONS C, K, Cl, Pb(p, pX), E at 350-650 MeV/c; measured inclusive σ(θ) vs proton momentum.

doi: 10.1103/PhysRevC.31.2168
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1985TA13      Phys.Lett. 160B, 380 (1985)

I.Tanihata, H.Hamagaki, O.Hashimoto, S.Nagamiya, Y.Shida, N.Yoshikawa, O.Yamakawa, K.Sugimoto, T.Kobayashi, D.E.Greiner, N.Takahashi, Y.Nojiri

Measurements of Interaction Cross Sections and Radii of He Isotopes

NUCLEAR REACTIONS 9Be, C, 27Al(3He, X), (α, X), (6He, X), (8He, X), E= 790 MeV/nucleon; measured interaction σ. 3,4,6,8He deduced interaction radii. Transmission type experiment, secondary beams from 11B projectile fragmentation.

doi: 10.1016/0370-2693(85)90005-X
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2011.


1984KI20      Phys.Rev.Lett. 53, 2000 (1984)

Y.Kitazoe, H.Furutani, H.Toki, Y.Yamamura, S.Nagamiya, M.Sano

Cascade-Model Analysis of the Sideward ' Splash ' in Nb + Nb Collisions with High-Multiplicity Events

NUCLEAR REACTIONS Ca(Ca, X), 93Nb(93Nb, X), E=400 MeV/nucleon; calculated high multiplicity event σ(θ); deduced cascade collision development, bounceoff effect. Cascade model.

doi: 10.1103/PhysRevLett.53.2000
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1983AN13      Phys.Rev. C28, 1224 (1983)

L.Anderson, W.Bruckner, E.Moeller, S.Nagamiya, S.Nissen-Meyer, L.Schroeder, G.Shapiro, H.Steiner

Inclusive Particle Production at Forward Angles from Collisions of Light Relativistic Nuclei: Nuclear fragments

NUCLEAR REACTIONS C, Cu, Pb, 1H(p, X), (d, X), (12C, X), E=1.05, 2.1 GeV/nucleon; C, Cu, Pb, 1H(α, X), E=0.4, 1.05, 2.1 GeV/nucleon; measured inclusive production σ vs θ, momentum for p, d, t, 3He, α, 6He, 8He light fragments. Glauber-type, hard scattering, coalescence model analyses.

doi: 10.1103/PhysRevC.28.1224
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1983MO14      Phys.Rev. C28, 1246 (1983)

E.Moeller, L.Anderson, W.Bruckner, S.Nagamiya, S.Nissen-Meyer, L.Schroeder, G.Shapiro, H.Steiner

Inclusive Particle Production at Forward Angles from Collisions of Light Relativistic Nuclei: Negative pions

NUCLEAR REACTIONS C, Cu, Pb, 1H(p, π-X), (d, π-X), (α, π-X), (12C, π-X), E=1.05, 2.1 GeV/nucleon; measured inclusive pion production σ vs θ, momentum; deduced reaction mechanism.

doi: 10.1103/PhysRevC.28.1246
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1982NA10      Phys.Rev.Lett. 48, 1780 (1982)

S.Nagamiya, H.Hamagaki, P.Hecking, S.Kadota, R.Lombard, Y.Miake, E.Moeller, S.Schnetzer, H.Steiner, I.Tanihata, S.Bohrmann, J.Knoll

Production of Negative Pions with 183-MeV/Nucleon Ne Beams

NUCLEAR REACTIONS Na, F, Pb(Ne, π-), E=183 MeV/nucleon; measured pion production σ; deduced reaction mechanism. NaF target.

doi: 10.1103/PhysRevLett.48.1780
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1981TA03      Phys.Lett. 100B, 121 (1981)

I.Tanihata, S.Nagamiya, S.Schnetzer, H.Steiner

One-and Two-Proton Inclusive Spectra in 800 MeV Proton-Nucleus Collisions and the Mean Free Path of Protons in Nuclei

NUCLEAR REACTIONS C, Na, F, K, Cl, Cu, Pb(p, p), (p, 2p), E=800 MeV; measured σ(θp), σ(θp1, θp2) vs proton momentum; deduced target dependence, proton mean free path. Quasielastic scattering model.

doi: 10.1016/0370-2693(81)90757-7
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1980NA07      Phys.Rev.Lett. 45, 602 (1980)

S.Nagamiya, M.-C.Lemaire, S.Schnetzer, H.Steiner, I.Tanihata

Single-Particle Spectra Associated with High-Multiplicity Events in 800-MeV/Nucleon Ar on KCl and Pb

NUCLEAR REACTIONS K, Cl(Ar, p), (Ar, π-), E=800 MeV/nucleon; Pb(Ar, p), E=800 MeV/nucleon; measured σ(θ, Ep), σ(θ, E(π-)). Inclusive, high-multiplicity events.

doi: 10.1103/PhysRevLett.45.602
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1979CH26      Phys.Rev. C20, 1332 (1979)

J.Chiba, K.Nakai, I.Tanihata, S.Nagamiya, H.Bowman, J.Ingersoll, J.O.Rasmussen

Low-Energy Pion Production with 800 MeV/N 20Ne

NUCLEAR REACTIONS Na, Cu, Pb(20Ne, π+), E=800 MeV/nucleon; measured σ(E(π), θπ).

doi: 10.1103/PhysRevC.20.1332
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1979LE14      Phys.Lett. 85B, 38 (1979)

M.-C.Lemaire, S.Nagamiya, S.Schnetzer, H.Steiner, I.Tanihata

Composite Particle Emission in Relativistic Heavy Ion Collisions

NUCLEAR REACTIONS C, Pb(12C, d), (12C, t), (12C, 3He), E=800 MeV/nucleon; Na, F, Pb(20Ne, d), (20Ne, t), (20Ne, 3He), E=400, 800, 2100 MeV/nucleon; K, Cl, Pb(40Ar, d), (40Ar, t), (40Ar, 3He), E=800 MeV/nucleon; measured inclusive spectra. Coalescence model interpretation.

doi: 10.1016/0370-2693(79)90772-X
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1979NA02      Phys.Lett. 81B, 147 (1979)

S.Nagamiya, L.Anderson, W.Bruckner, O.Chamberlain, M.-C.Lemaire, S.Schnetzer, G.Shapiro, H.Steiner, I.Tanihata

Wide-Angle High-Energy Proton Spectra by 800 MeV/A C, Ne, and Ar Beams

NUCLEAR REACTIONS C(12C, p), Na, Pb(Pb, p), (20Ne, p), K, Pb(40Ar, p), E=800 MeV/A; measured σ(Ep), two-particle correlation in inclusive reactions.

doi: 10.1016/0370-2693(79)90509-4
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1979NA12      Phys.Rev. C20, 2210 (1979)

K.Nakai, J.Chiba, I.Tanihata, M.Sasao, H.Bowman, S.Nagamiya, J.O.Rasmussen

Low-Energy Pion Production in High-Energy Nucleus-Nucleus Collisions

NUCLEAR REACTIONS C, Na, F, Cu, Pb(20Ne, π+), E=400 MeV/nucleon; measured σ(Eπ, θπ).

doi: 10.1103/PhysRevC.20.2210
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1979TA19      Phys.Lett. 87B, 349 (1979)

I.Tanihata, S.Nagamiya, O.Chamberlain, M.-C.Lemaire, S.Schnetzer, G.Shapiro, H.Steiner

Negative Pion Production by 800 MeV/A, C, Ne, and Ar Beams

NUCLEAR REACTIONS 12C(12C, π-), Na, Pb(208Pb, π-), (20Ne, π-), K, Pb(40Ar, π-), E=800 MeV/nucleon; measured σ(Eπ-, θπ-). Hard-scattering, firestreak model calculations.Cl targets.

doi: 10.1016/0370-2693(79)90552-5
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1978SH18      Nucl.Phys. A308, 513 (1978)

T.Shibata, H.Ejiri, J.Chiba, S.Nagamiya, K.Nakai

In-Beam Nuclear Gamma-Ray Studies of Relativistic Heavy Ion Reactions

NUCLEAR REACTIONS Sr(12C, X), E=3-12.6 GeV; Na, S, Ca(12C, X), E=3-4.8 GeV; Na, S, Ca(α, X), E=1.6 GeV; measured σ(Eγ), Iγ.

doi: 10.1016/0375-9474(78)90563-8
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1976HA20      Phys.Lett. 62B, 233 (1976)

O.Hashimoto, S.Nagamiya, K.Nagamine, T.Yamazaki

Total Muon Captures Rates in Actinide Nuclei

NUCLEAR REACTIONS 232Th, 235,238U, 239Pu(μ-, X); measured muon capture rates, muonic atom T1/2. 232Th, 233,235,238U, 239,242Pu, 237Np(μ-, X); analyzed muon capture rates.

doi: 10.1016/0370-2693(76)90515-3
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1975MA02      Nucl.Phys. A237, 182 (1975)

E.Matthias, E.Recknagel, O.Hashimoto, S.Nagamiya, K.Nakai, T.Yamazaki, Y.Yamazaki

The g-Factor Measurement for the 8+ Isomeric State of 86Sr Produced in Kr Gas

NUCLEAR REACTIONS Kr(α, 2n), E=22 MeV; measured αγ(θ, H, t). 86mSr deduced g. Stroboscopic method, natural Kr gas target.

doi: 10.1016/0375-9474(75)90471-6
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1974HA06      Nucl.Phys. A218, 180 (1974)

O.Hashimoto, A.Sumi, T.Nomura, S.Nagamiya, K.Nakai, T.Yamazaki, K.Miyano

Measurement of the g-Factor of the 0.57 ms 7+ State in 202Tl

NUCLEAR REACTIONS Hg(p, xn), E=28 MeV; measured γ(θ, H, t). 202Tl level deduced g.

doi: 10.1016/0375-9474(74)90029-3
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1974NA02      Nucl.Instrum.Methods 114, 349 (1974)

S.Nagamiya

The γ-Ray PAD Pattern in the Presence of Two Isomeric Levels

doi: 10.1016/0029-554X(74)90554-0
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1974RE09      Phys.Lett. 52B, 414 (1974)

E.Recknagel, Y.Yamazaki, O.Hashimoto, S.Nagamiya, K.Nakai

Magnetic Moment of the 29/2+ Isomeric State in 213Fr

NUCLEAR REACTIONS 204Hg(14N, 5nγ), E=94 MeV; measured γ(θ, H), Eγ. 213Fr level deduced g. Stroboscopic resonance method.

doi: 10.1016/0370-2693(74)90113-0
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1974YA09      Phys.Rev.Lett. 33, 1614 (1974)

Y.Yamazaki, O.Hashimoto, H.Ikezoe, S.Nagamiya, K.Nakai, T.Yamazaki

Blocking Effect of the M1 Core Polarization Studied from the g Factor Of the 8+ State in 214Ra

NUCLEAR REACTIONS 206Pb(12C, 4nγ), E=90 MeV; measured γ(θ, H). 214Ra level deduced g.

doi: 10.1103/PhysRevLett.33.1614
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1973NA18      Nucl.Phys. A211, 381 (1973)

S.Nagamiya, Y.Yamazaki, O.Hashimoto, T.Nomura, K.Nakai, T.Yamazaki

Magnetic Moments of the [πh29/2]8+ States in Po Isotopes and of the [(πh29/2)8+ X νp-11/2]17/2- State in 209Po

NUCLEAR REACTIONS 204,206Pb(3He, 3nγ), E=30 MeV; 204Pb(α, 2nγ), E=29 MeV; 208Pb(3He, 3nγ), E=28 MeV; 207Pb(α, 2nγ), E=28 MeV; 208Pb(α, 2nγ), E=25 MeV; measured γ(θ, H, t). 204,206,208,209,210Po levels deduced g, stroboscopic method.

doi: 10.1016/0375-9474(73)90727-6
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1973NA21      Phys.Scr. 8, 95 (1973)

S.Nagamiya, O.Hashimoto, Y.Yamazaki

Half-Lives of the [πh29/2] 6+ and 4+ States of 210Po

RADIOACTIVITY 210At; measured γγ(t). 210Po levels deduced T1/2.

doi: 10.1088/0031-8949/8/3/004
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1973YA06      Phys.Lett. 44B, 440 (1973)

Y.Yamazaki, S.Nagamiya, T.Nomura, K.Nakai, T.Yamazaki

Magnetic Moment of a Core-Excited Isomeric State in 210Po

NUCLEAR REACTIONS 208Pb(α, 2nγ), E=33 MeV; measured Iγ(θ, H). 210Po level deduced g.

doi: 10.1016/0370-2693(73)90328-6
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1972IN02      J.Phys.Soc.Jap. 32, 1163 (1972)

T.Inamura, Y.Tendow, S.Nagamiya, A.Hashizume

Excited Levels in 190Hg and a 24.5 ns Isomer

NUCLEAR REACTIONS 181Ta(14N, 5nγ), E=75-100 MeV; measured σ(E;Eγ, θ(γ)), (14N)(γ)-delay. 190mHg deduced levels, J, π, T1/2.

doi: 10.1143/JPSJ.32.1163
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1972NA02      Nucl.Phys. A182, 84 (1972)

S.Nagamiya, T.Inamura

Isomeric States in Neutron-Deficient Po Isotopes (A = 200-203) Studied by (HI, xnγ) Reactions

NUCLEAR REACTIONS Pt(12C, xnγ), E=80 MeV; Ir(14N, xnγ), 191Ir(14N, xnγ), E=85 MeV; measured (12C)(γ)-, (14N)(γ)-delay. 202Po, 200Po levels deduced T1/2.

doi: 10.1016/0375-9474(72)90203-5
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1972NA08      Nucl.Phys. A189, 526 (1972)

K.Nakai, B.Herskind, J.Blomqvist, A.Filevich, K.-G.Rensfelt, J.Sztarkier, I.Bergstrom, S.Nagamiya

The g-Factor of the 12+ Isomeric State in 206Pb and the Effective Orbital g-Factor of the Neutron

NUCLEAR REACTIONS 204Hg(α, 2nγ), E=27 MeV; measured αγ(θ, H, t). 206mPb deduced g, neutron effective orbital g.

doi: 10.1016/0375-9474(72)90311-9
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1972NA33      Sci.Pap.Inst.Phys.Chem.Res. 66, 39 (1972)

S.Nagamiya

Study of the Effective Spin and Orbital Magnetic Moments of Nucleons

NUCLEAR REACTIONS 204,206,208Pb, 90Zr, 88Sr(α, 2nγ), E=25-30 MeV; 206,208Pb(3He, 3nγ), E=30-32 MeV; 40Ca(α, 2pγ), E=25 MeV; measured Eγ, Iγ, γ(θ, H, t). 210Po, 208Po, 206Po, 92Mo, 90Zr, 42Ca levels deduced g.


1972NO09      J.Phys.Soc.Jap. 33, 286 (1972)

T.Nomura, T.Yamazaki, S.Nagamiya, T.Katou

Magnetic Moment of the Lowest 6+ State in 42Ca

NUCLEAR REACTIONS 40Ca(α, 2pγ), E=25 MeV; measured αγ(θ, H, t). 42Ca level deduced g, T1/2.

doi: 10.1143/JPSJ.33.286
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1971NA16      J.Phys.Soc.Japan 31, 319 (1971)

S.Nagamiya, T.Katou, T.Nomura, T.Yamazaki

Magnetic Moments of the 8+ Isomeric States of 90Zr and 92Mo

NUCLEAR REACTIONS 88Sr, 90Zr(α, 2nγ), E=29, 25 MeV; measured αγ(θ, H, t). 90mZr, 92mMo deduced g.

doi: 10.1143/JPSJ.31.319
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1971NA19      Phys.Rev. C4, 1961 (1971)

S.Nagamiya, T.Yamazaki

Evidence for Anomalous g1 Factors of the Nucleons and the Mesonic-Exchange Effect

NUCLEAR MOMENTS 16O, 88Sr, 208Pb; analyzed μ; deduced anomalous nucleon g(L) factors.

doi: 10.1103/PhysRevC.4.1961
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1971NO06      Phys.Rev.Lett. 27, 523 (1971)

T.Nomura, T.Yamazaki, S.Nagamiya, T.Katou

Magnetic Moment of the Lowest 6+ State in 42Ca and Effects of the Deformed States

NUCLEAR REACTIONS 40Ca(α, 2pγ), E=25 MeV; measured αγ(θ, H, t). 42Ca level deduced g.

doi: 10.1103/PhysRevLett.27.523
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1970NA11      Nucl.Phys. A159, 653 (1970)

S.Nagamiya, T.Nomura, T.Yamazaki

Stroboscopic Determination of the Magnetic Moment of the 8+ Isomeric State of 208Po

NUCLEAR REACTIONS 206Pb(α, 2nγ), E=29 MeV; measured αγ(θ, H, t). 208Po level deduced μ. Stroboscopic method.

doi: 10.1016/0375-9474(70)90864-X
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1970NA13      Phys.Lett. 33B, 574 (1970)

S.Nagamiya, T.Katou, T.Nomura, T.Yamazaki

Effective Spin and Orbital Magnetism of the Proton Studied from the g-Factors of the 8+ States in 90Zr, and 92Mo

NUCLEAR REACTIONS 88Sr, 90Zr(α, 2nγ), E=29, 25 MeV; measured αγ(θ, H, t). 90Zr, 92Mo levels deduced g.

doi: 10.1016/0370-2693(70)90353-9
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1970YA06      Phys.Rev.Lett. 25, 547 (1970)

T.Yamazaki, T.Nomura, S.Nagamiya, T.Katou

Anomalous Orbital Magnetism of Proton Deduced from the Magnetic Moment of the 11- State of 210Po

NUCLEAR REACTIONS 208Pb(α, 2n), E=30 MeV; measured αγ(θ, H, t). 210Po level deduced g. 1H deduced anomalous orbital magnetism.

doi: 10.1103/PhysRevLett.25.547
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