Nuclear Science References (NSR)

NUCLEAR REACTIONS ¹H(p-bar, X), E at 600-1940 MeV/c; measured ωη production associated mass spectra, angular distributions; deduced resonance features.

doi: 10.1016/S0370-2693(01)00466-X
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2001AN15 Phys.Lett. 508B, 6 (2001)

A.V.Anisovich, C.A.Baker, C.J.Batty, D.V.Bugg, V.A.Nikonov, A.V.Sarantsev, V.V.Sarantsev, B.S.Zou

Resonances in (p-bar)p → ωπ⁰ with Masses 1960 to 2410 MeV

NUCLEAR REACTIONS ¹H(p-bar, π⁰X), E at 600-1940 MeV/c; analyzed ω-meson production associated σ, mass and angular distributions; deduced resonance features.

doi: 10.1016/S0370-2693(01)00475-0
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2001AN21 Nucl.Phys. A690, 567 (2001)

A.V.Anisovich, D.V.Bugg, N.Djaoshvili, C.Hodd, J.Kisiel, L.Montanet, A.V.Sarantsev, B.S.Zou

Resonances in (p-bar)p → ηπ⁺π^-π⁺π^- at Rest

NUCLEAR REACTIONS ¹H(p-bar, X), E at rest; measured ηπ⁺π^-π⁺π^- associated invariant mass spectra; deduced resonance contributions, branching ratios.

doi: 10.1016/S0375-9474(01)00349-9
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2001AN23 Phys.Lett. 513B, 281 (2001)

A.V.Anisovich, C.A.Baker, C.J.Batty, D.V.Bugg, V.A.Nikonov, A.V.Sarantsev, V.V.Sarantsev, B.S.Zou

Resonances in (p-bar)p → ωηπ⁰ in the Mass Range 1960 to 2410 MeV

NUCLEAR REACTIONS ¹H(p-bar, X), E at 600-1940 MeV/c; measured ωηπ⁰ production associated invariant mass spectra; deduced resonance features.

doi: 10.1016/S0370-2693(01)00476-2
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2001AN30 Phys.Lett. 517B, 261 (2001)

A.V.Anisovich, C.A.Baker, C.J.Batty, D.V.Bugg, V.A.Nikonov, A.V.Sarantsev, V.V.Sarantsev, B.S.Zou

Partial Wave Analysis of (p-bar)p Annihilation Channels in Flight with I = 1, C = + 1

NUCLEAR REACTIONS ¹H(p-bar, X), E at 600-1940 MeV/c; analyzed data; deduced resonance parameters. Partial wave analysis.

doi: 10.1016/S0370-2693(01)01017-6
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2001AN31 Phys.Lett. 517B, 273 (2001)

A.V.Anisovich, C.A.Baker, C.J.Batty, D.V.Bugg, V.A.Nikonov, A.V.Sarantsev, V.V.Sarantsev, B.S.Zou

A Partial Wave Analysis of (p-bar)p → ηηπ⁰

NUCLEAR REACTIONS ¹H(p-bar, π⁰X), E at 600-1940 MeV/c; analyzed ηη production associated data; deduced resonance parameters. Partial wave analysis.

doi: 10.1016/S0370-2693(01)01018-8
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2000AM01 Nucl.Phys. A668, 83 (2000)

D.Amelin, E.Berdnikov, S.Bityukov, G.Borisov, D.V.Bugg, Yu.Gouz, V.Dorofeev, R.Dzhelyadin, A.Ekimov, A.Karyukhin, I.Kachaev, Yu.Khokhlov, V.Konstantinov, S.Kopikov, V.Kostyukhin, S.Likhoded, V.Matveev, A.Ostankov, B.Polyakov, D.Ryabchikov, G.Sekhniaidze, O.Solovianov, A.Solodkov, E.Starchenko, E.Tskhadadze, N.Vishnevsky, E.Vlasov, A.Zaitsev, and the VES Collaboration

Natural Parity Resonances in ηπ⁺π^-

NUCLEAR REACTIONS ¹H(π^-, π⁺π^-X), E=37 GeV; analyzed ν meson associated invariant mass distributions; deduced resonances masses and widths. Partial wave analysis.

doi: 10.1016/S0375-9474(99)00370-X
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2000AN02 Nucl.Phys. A662, 319 (2000)

A.V.Anisovich, C.A.Baker, C.J.Batty, D.V.Bugg, A.Hasan, C.Hodd, J.Kisiel, V.A.Nikonov, A.V.Sarantsev, V.V.Sarantsev, B.S.Zou

Partial Wave Analysis of (p-bar)p → π^-π⁺, π⁰π⁰, ηη and ηη'

NUCLEAR REACTIONS ¹H(p-bar, X), E at 600-1940 MeV/c; analyzed two-pion and two-η related σ(θ), polarization data; deduced resonance parameters. Partial wave analysis.

doi: 10.1016/S0375-9474(99)00407-8
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2000AN03 Nucl.Phys. A662, 344 (2000)

A.V.Anisovich, C.A.Baker, C.J.Batty, D.V.Bugg, C.Hodd, J.Kisiel, V.A.Nikonov, A.V.Sarantsev, V.V.Sarantsev, B.S.Zou

Data on (p-bar)p → π⁰π⁰, ηη and ηη' from 600 to 1940 MeV/c

NUCLEAR REACTIONS ¹H(p-bar, 2π⁰), E at 600-1940 MeV/c; measured σ(θ), deduced integrated σ. ¹H(p-bar, X), E at 600-1940 MeV/c; measured 2η-associated σ(θ), integrated σ. Crystal Barrel detector.

doi: 10.1016/S0375-9474(99)00410-8
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2000AN04 Phys.Lett. 472B, 168 (2000)

A.V.Anisovich, C.A.Baker, C.J.Batty, D.V.Bugg, C.Hodd, V.A.Nikonov, A.V.Sarantsev, V.V.Sarantsev, B.S.Zou

A J^PC = 0^-⁺ Enhancement at the f₀(980)η Threshold

NUCLEAR REACTIONS ¹H(p-bar, X), E at 900-1200 MeV/c; measured mass distributions and spectra, Dalitz plots; deduced resonance threshold enhancement.

doi: 10.1016/S0370-2693(99)01398-2
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2000AN06 Phys.Lett. 476B, 15 (2000)

A.V.Anisovich, C.A.Baker, C.J.Batty, D.V.Bugg, C.Hodd, V.A.Nikonov, A.V.Sarantsev, V.V.Sarantsev, B.S.Zou

Resonances in (p-bar)p → ωπ⁰π⁰ from 600 to 1940 MeV/c

NUCLEAR REACTIONS ¹H(p-bar, 2π⁰X), E at 600-1940 MeV/c; measured ω meson associated invariant mass spectra; deduced resonance features. Partial wave analysis.

doi: 10.1016/S0370-2693(00)00125-8
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2000AN23 Nucl.Phys. A675, 197c (2000)

A.V.Anisovich, C.A.Baker, C.J.Batty, D.V.Bugg, C.Hodd, J.Kisiel, V.A.Nikonov, A.V.Sarantsev, V.V.Sarantsev, I.Scott, B.S.Zou

Resonances in (p-bar)p → f₂(1270)π, π⁰η and π⁰η' in the Mass Range 1960-2410 MeV

NUCLEAR REACTIONS ¹H(p-bar, X), E at 600-1940 MeV/c; analyzed σ(θ), mass spectra; deduced resonance features.

doi: 10.1016/S0375-9474(00)00245-1
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2000AN28 Phys.Lett. 491B, 40 (2000)

A.V.Anisovich, C.A.Baker, C.J.Batty, D.V.Bugg, C.Hodd, V.A.Nikonov, A.V.Sarantsev, V.V.Sarantsev, B.S.Zou

Data on (p-bar)p → η'π⁰π⁰ for Masses 1960 to 2410 MeV/c²

NUCLEAR REACTIONS ¹H(p-bar, 2π⁰X), E at 600-1940 MeV/c; measured η' production associated invariant mass spectra, angular distributions; deduced resonance features.

doi: 10.1016/S0370-2693(00)01019-4
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2000AN29 Phys.Lett. 491B, 47 (2000)

A.V.Anisovich, C.A.Baker, C.J.Batty, D.V.Bugg, C.Hodd, H.C.Lu, V.A.Nikonov, A.V.Sarantsev, V.V.Sarantsev, B.S.Zou

I = 0 C = + 1 Mesons from 1920 to 2410 MeV

NUCLEAR REACTIONS ¹H(p-bar, X), E at 600-1940 MeV/c; measured fragments invariant mass spectra, angular distributions; deduced resonance features. Partial wave analysis.

doi: 10.1016/S0370-2693(00)01018-2
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2000AN37 Phys.Lett. 496B, 145 (2000)

A.V.Anisovich, C.A.Baker, C.J.Batty, D.V.Bugg, V.A.Nikonov, A.V.Sarantsev, V.V.Sarantsev, B.S.Zou

A Study of (p-bar)p → ηηη for Masses 1960 to 2410 MeV/c²

NUCLEAR REACTIONS ¹H(p-bar, X), E at 600-1940 MeV/c; measured 3η production associated σ, invariant mass spectra; deduced resonance features.

doi: 10.1016/S0370-2693(00)01301-0
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2000BU03 Phys.Lett. 475B, 17 (2000)

D.V.Bugg

Antiproton Annihilation at Rest in Deuterium

NUCLEAR REACTIONS ²H(p-bar, X), E at rest; calculated atomic partial wave contributions, related features.

ATOMIC PHYSICS ²H(p-bar, X), E at rest; calculated atomic partial wave contributions, related features.

doi: 10.1016/S0370-2693(00)00094-0
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2000BU21 Nucl.Phys. A675, 19c (2000)

D.V.Bugg

Resonances Around 2 GeV: q(q-bar) and glueballs

NUCLEAR REACTIONS ¹H(p-bar, X), E at 600-1940 MeV/c; analyzed data; deduced resonance properties.

doi: 10.1016/S0375-9474(00)00210-4
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1999AN11 Phys.Lett. 449B, 145 (1999)

A.V.Anisovich, C.A.Baker, C.J.Batty, D.V.Bugg, R.P.Haddock, C.Hodd, V.A.Nikonov, C.N.Pinder, A.V.Sarantsev, V.V.Sarantsev, I.Scott, B.S.Zou

Study of the Process (p-bar)p → ηηπ⁰ from 1350 to 1940 MeV/c

NUCLEAR REACTIONS ¹H(p-bar, X), E at 1350-1940 MeV/c; measured eta-pion channel associated photon spectra, decay angular distributions; deduced resonances, branching fractions.

doi: 10.1016/S0370-2693(99)00077-5
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1999AN12 Phys.Lett. 449B, 154 (1999)

A.V.Anisovich, C.A.Baker, C.J.Batty, D.V.Bugg, R.P.Haddock, C.Hodd, V.A.Nikonov, A.V.Sarantsev, V.V.Sarantsev, I.Scott, B.S.Zou

Observation of f₀(1770) → ηη in (p-bar)p → ηηπ⁰ Reactions from 600 to 1200 MeV/c

NUCLEAR REACTIONS ¹H(p-bar, X), E at 600-1200 MeV/c; measured eta-pion channel associated photon spectra, decay angular distributions; deduced f₀ resonance features.

doi: 10.1016/S0370-2693(99)00078-7
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1999AN18 Phys.Lett. 452B, 173 (1999)

A.V.Anisovich, C.A.Baker, C.J.Batty, D.V.Bugg, C.Hodd, J.Kisiel, V.A.Nikonov, A.V.Sarantsev, V.V.Sarantsev, I.Scott, B.S.Zou

(p-bar)p → π⁰η and π⁰η' from 600 to 1940 MeV/c

NUCLEAR REACTIONS ¹H(p-bar, π⁰X), E at 600-1940 MeV/c; measured η-meson associated σ(θ); deduced resonance parameters. Partial wave analysis.

doi: 10.1016/S0370-2693(99)00248-8
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1999AN19 Phys.Lett. 452B, 180 (1999)

A.V.Anisovich, C.A.Baker, C.J.Batty, D.V.Bugg, C.Hodd, J.Kisiel, V.A.Nikonov, A.V.Sarantsev, V.V.Sarantsev, I.Scott, B.S.Zou

Study of (p-bar)p → π⁰π⁰η from 600 to 1940 MeV/c

NUCLEAR REACTIONS ¹H(p-bar, 2π⁰X), E at 600-1940 MeV/c; measured η-meson associated invariant mass spectra, σ, σ(θ); deduced resonance parameters. Partial wave analysis.

doi: 10.1016/S0370-2693(99)00249-X
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1999AN20 Phys.Lett. 452B, 187 (1999)

A.V.Anisovich, C.A.Baker, C.J.Batty, D.V.Bugg, C.Hodd, J.Kisiel, V.A.Nikonov, A.V.Sarantsev, V.V.Sarantsev, I.Scott, B.S.Zou

Resonances in (p-bar)p → f₂(1270)π

NUCLEAR REACTIONS ¹H(p-bar, 3π⁰), E at 600-1940 MeV/c; measured invariant mass spectra, σ, σ(θ); deduced resonance parameters. Partial wave analysis.

doi: 10.1016/S0370-2693(99)00247-6
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1999AN24 Nucl.Phys. A651, 253 (1999)

A.V.Anisovich, C.A.Baker, C.J.Batty, D.V.Bugg, C.Hodd, J.Kisiel, V.A.Nikonov, A.V.Sarantsev, V.V.Sarantsev, I.Scott, B.S.Zou

Resonances Formed by (p-bar)p and Decaying into π⁰π⁰η for Masses 1960 to 2410 MeV

NUCLEAR REACTIONS ¹H(p-bar, 2π⁰X), E at 600-1940 MeV/c; measured η production assiciated invariant mass spectra, angular distributions; deduced resonances E, Γ. Partial wave analysis.

doi: 10.1016/S0375-9474(99)00137-2
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1999AN49 Phys.Lett. 468B, 304 (1999)

A.V.Anisovich, C.A.Baker, C.J.Batty, D.V.Bugg, C.Hodd, J.Kisiel, V.A.Nikonov, A.V.Sarantsev, V.V.Sarantsev, B.S.Zou

p(bar)p → π⁰π⁰ from 600 to 1940 MeV/c

NUCLEAR REACTIONS ¹H(p-bar, 2π⁰), E at 600-1940 MeV/c; measured σ, σ(θ); deduced resonance features. Crystal Barrel detector.

doi: 10.1016/S0370-2693(99)01206-X
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1999AN50 Phys.Lett. 468B, 309 (1999)

A.V.Anisovich, C.A.Baker, C.J.Batty, D.V.Bugg, C.Hodd, J.Kisiel, V.A.Nikonov, A.V.Sarantsev, V.V.Sarantsev, B.S.Zou

p(bar)p → ηη and ηη' from 600 to 1940 MeV/c

NUCLEAR REACTIONS ¹H(p-bar, X), E at 600-1940 MeV/c; measured ηη production σ, σ(θ); deuced resonance features. Crystal Barrel detector.

doi: 10.1016/S0370-2693(99)01207-1
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1999BA19 Phys.Lett. 449B, 114 (1999)

C.A.Baker, C.J.Batty, P.Blum, D.V.Bugg, R.P.Haddock, C.Hodd, C.Holtzhaussen, L.Montanet, D.Odoom, C.N.Pinder, I.Scott, B.S.Zou

Evidence for a J^PC = 1⁺⁺ I = 1 Meson at 1640 MeV

NUCLEAR REACTIONS ¹H(p-bar, X), E at 1940 MeV/c; analyzed data; deduced resonance energy, width.

doi: 10.1016/S0370-2693(99)00075-1
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1999BA99 Phys.Lett. 467B, 147 (1999)

C.A.Baker, B.M.Barnett, C.J.Batty, K.Braune, D.V.Bugg, O.Cramer, V.Crede, N.Djaoshvili, W.Dunnweber, M.A.Faessler, N.P.Hessey, P.Hidas, C.Hodd, D.Jamnik, H.Kalinowsky, J.Kisiel, E.Klempt, C.Kolo, L.Montanet, B.Pick, W.Roethel, A.Sarantsev, I.Scott, C.Strassburger, U.Thoma, C.Volcker, S.Wallis, D.Walther, K.Wittmack, B.S.Zou

The f₂(1565) in (p-bar)p → (ωω)π⁰ Interactions at Rest

NUCLEAR REACTIONS ¹H(p-bar, π⁰X), E at rest; measured (ωω) associated invariant mass spectra; deduced resonance role.

doi: 10.1016/S0370-2693(99)01107-7
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1999BU22 Nucl.Phys. A655, 57c (1999)

D.V.Bugg

Study of (p-bar)p → ηηπ⁰ from 600 to 1940 MeV/c

NUCLEAR REACTIONS ¹H(p-bar, π⁰X), E at 600-1940 MeV/c; measured ηη associated invariant mass spectra; deduced resonance features.

doi: 10.1016/S0375-9474(99)00180-3
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1999BU23 Nucl.Phys. A655, 117c (1999)

D.V.Bugg, A.V.Sarantsev

(p-bar)p → π⁰π⁰ from 600 to 1940 MeV/c

NUCLEAR REACTIONS ¹H(p-bar, 2π⁰), E at 600-1940 MeV/c; measured σ, σ(E, θ); deduced resonance features.

doi: 10.1016/S0375-9474(99)00188-8
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1996AB32 Nucl.Phys. A609, 562 (1996); Erratum Nucl.Phys. A625, 899 (1997)

A.Abele, J.Adomeit, D.S.Armstrong, C.A.Baker, C.J.Batty, M.Benayoun, A.Berdoz, K.Beuchert, S.Bischoff, P.Blum, K.Braune, D.V.Bugg, T.Case, A.R.Cooper, O.Cramer, K.M.Crowe, H.P.Dietz, N.Djaoshvili, W.Dunnweber, D.Engelhardt, M.Englert, M.A.Faessler, R.P.Haddock, F.H.Heinsius, M.Herz, N.P.Hessey, P.Hidas, C.Holtzhaussen, P.Illinger, D.Jamnik, B.Kammle, P.Kammel, T.Kiel, H.Koch, C.Kolo, M.Lakata, H.Matthay, R.McCrady, J.Meier, C.A.Meyer, L.Montanet, C.N.Pinder, G.Pinter, C.Regenfus, J.Reissmann, W.Rothel, P.Schmidt, I.Scott, R.Seibert, C.Strassburger, U.Strohbusch, M.Suffert, U.Thoma, M.Tischhauser, C.Volcker, D.Walther, B.Zou

Further Analysis of (p-bar)p → 3π⁰, ηηπ⁰ and ηπ⁰π⁰ at Rest

NUCLEAR REACTIONS ¹H(p-bar, X), E at rest; analyzed 3π⁰, 2ηπ⁰, η2π⁰ production data; deduced f₀, f₂ resonances, widths.

doi: 10.1016/S0375-9474(96)00306-5
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1996HA38 Phys.Lett. 388B, 376 (1996)

A.Hasan, D.V.Bugg

A Search for the ξ(2235) in (p-bar)p → π^-π⁺

NUCLEAR REACTIONS ¹H(p-bar, X), E=low; analyzed π^-π⁺-production data; deduced no narrow resonance evidence.

doi: 10.1016/S0370-2693(96)01196-3
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1995BU22 Phys.Rev. C52, 1203 (1995)

D.V.Bugg, R.Machleidt

πNN Coupling Constants from NN Elastic Data between 210 and 800 MeV

NUCLEAR REACTIONS ¹H(p, p), (n, n), E=210-800 MeV; analyzed data; deduced πNN coupling constants.

doi: 10.1103/PhysRevC.52.1203
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1994AN25 Yad.Fiz. 57, No 9, 1666 (1994); Phys.Atomic Nuclei 57, 1595 (1994)

V.V.Anisovich, D.V.Bugg, A.V.Sarantsev, B.S.Zou

How to Solve the Three-Pion Annihilation Problem

NUCLEAR REACTIONS ¹H(p-bar, X), E at rest; analyzed 3π production; deduced scalar resonances, width, spin, mass.

1994BU31 Phys.Rev. D50, 4412 (1994)

D.V.Bugg, V.V.Anisovich, A.Sarantsev, B.S.Zou

Coupled Channel Analysis of Data on (p-bar)p → 3π⁰, (Eta)(Eta)π⁰, and (Eta)π⁰π⁰ at Rest, with the N/D Method

NUCLEAR REACTIONS ¹H(p-bar, X), E at rest; analyzed annihilation data; deduced resonances, parameters. Coupled-channels approach, N/D method.

doi: 10.1103/PhysRevD.50.4412
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1994HA47 Phys.Lett. 334B, 215 (1994)

A.Hasan, D.V.Bugg

Amplitudes for (p-bar)p → ππ from 0.36 to 2.5 GeV/c

NUCLEAR REACTIONS ¹H(p-bar, X), E ≤ 2.5 GeV/c; analyzed π⁺π^-, 2π⁰ production data. Amplitude analysis.

doi: 10.1016/0370-2693(94)90614-9
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1993AR11 Phys.Rev. C48, 1926 (1993); Erratum Phys.Rev. C49 1229 (1994)

R.A.Arndt, I.I.Strakovsky, R.L.Workman, D.V.Bugg

Analysis of the Reaction π⁺d → pp to 500 MeV

NUCLEAR REACTIONS ²H(π⁺, 2p), E=500 MeV; analyzed σ(θ), deuteron vector analyzing power, 2p-spin correlation parameter; deduced dominant partial wave amplitude characteristics. Energy-dependent approach.

doi: 10.1103/PhysRevC.48.1926
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1993BU17 Nucl.Phys. A558, 183c (1993)

D.V.Bugg

(p-bar)p → π^-π⁺ and K^-K⁺

NUCLEAR REACTIONS ¹H(p-bar, X), E at 360-1550 MeV/c; measured σ(θ), polarization for (π^-π⁺), (K^-K⁺) production, σ(ratio) vs momentum.

doi: 10.1016/0375-9474(93)90393-C
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1992AN01 Nucl.Phys. A537, 501 (1992)

V.V.Anisovich, A.V.Sarantsev, D.V.Bugg

Analysis of the NN → NΔ Threshold using the Coupled-Channel N/D Method

NUCLEAR REACTIONS ¹H(p, p), (p, π⁺), (p, X), E < 1 GeV; analyzed data. Coupled-channels, N/D method.

doi: 10.1016/0375-9474(92)90366-R
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1992BU08 Nucl.Phys. A540, 449 (1992)

D.V.Bugg, R.A.Bryan

Comments on np Scattering, 142-800 MeV

NUCLEAR REACTIONS ¹H(polarized n, n), E=142-800 MeV; analyzed data; deduced I=0 inelasticity onset, no dibaryon evidence.

doi: 10.1016/0375-9474(92)90168-J
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1992HA36 Nucl.Phys. B378, 3 (1992)

A.Hasan, D.V.Bugg, J.R.Hall, R.L.Shypit, F.Tessarotto, R.Birsa, F.Bradamante, S.Dalla Torre-Colautti, A.Martin, A.Penzo, P.Schiavon, A.Villari, S.Degli-Agosti, E.Heer, C.Lechanoine-Leluc, Y.Onel, D.Rapin, R.Kunne, K.Bos, J.C.Kluyver, L.Linssen, A.S.Clough

Differential Cross Sections and Analysing Powers for (P-bar)P → π^-π⁺ and K^-K⁺ from 360 to 1550 MeV/c

NUCLEAR REACTIONS ¹H(p-bar, π⁺π^-), (p-bar, K⁺K^-), E at 360-1550 MeV/c; measured analyzing power, σ(θ).

doi: 10.1016/0550-3213(92)90002-S
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1991KU15 Phys.Lett. 261B, 191 (1991)

R.A.Kunne, C.I.Beard, R.Birsa, K.Bos, F.Bradamante, D.V.Bugg, A.S.Clough, S.Dalla Torre-Colautti, J.A.Edgington, M.Giorgi, J.R.Hall, E.Heer, R.Hess, J.C.Kluyver, C.Lechanoine-Leluc, L.Linssen, A.Martin, T.O.Niinikoski, Y.Onel, A.Penzo, D.Rapin, J.M.Rieubland, A.Rijllart, P.Schiavon, R.L.Shypit, F.Tessarotto, A.Villari

First Measurement of D(onon) in (p-bar)p Elastic Scattering

NUCLEAR REACTIONS ¹H(p-bar, p-bar), E at 679-1550 MeV/c; measured depolarization parameter. Polarized target. Model comparison.

doi: 10.1016/0370-2693(91)91349-Z
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1990BU11 Phys.Rev. C41, 2708 (1990)

D.V.Bugg

np Phase Shifts, 142 to 800 MeV

NUCLEAR REACTIONS ¹H(p, p), (polarized p, p), E=142-800 MeV; analyzed data; deduced phase shifts.

doi: 10.1103/PhysRevC.41.2708
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1989KU16 Nucl.Phys. B323, 1 (1989)

R.A.Kunne, C.I.Beard, R.Birsa, K.Bos, F.Bradamante, D.V.Bugg, A.S.Clough, S.Dalla Torre-Colautti, J.A.Edgington, J.R.Hall, E.Heer, R.Hess, J.C.Kluyver, C.Lechanoine-Leluc, L.Linssen, A.Martin, T.O.Niinikoski, Y.Onel, A.Penzo, D.Rapin, J.M.Rieubland, A.Rijllart, P.Schiavon, R.L.Shypit, F.Tessarotto, A.Villari, P.Wells

Measurement of d(sigma)/d(omega) and A(on) in (p-bar)p Elastic Scattering between 497 and 1550 MeV/c

NUCLEAR REACTIONS ¹H(p-bar, p-bar), E at 497-1550 MeV/c; measured σ(θ), asymmetry. Different nucleon-antinucleon potential models.

doi: 10.1016/0550-3213(89)90585-3
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1989SH26 Phys.Rev. C40, 2203 (1989)

R.L.Shypit, D.V.Bugg, A.H.Sanjari, D.M.Lee, M.W.McNaughton, R.R.Silbar, C.L.Hollas, K.H.McNaughton, P.Riley, C.A.Davis

Spin Dependence of pp → npπ⁺ from 492 to 796 MeV

NUCLEAR REACTIONS ¹H(polarized p, pπ⁺), E=492-796 MeV; measured spin correlation parameters; deduced no dibaryon evidence. Longitudinally polarized target.

doi: 10.1103/PhysRevC.40.2203
Citations: PlumX Metrics

1988MA48 Nucl.Phys. A487, 563 (1988)

A.Martin, R.Birsa, K.Bos, F.Bradamante, D.V.Bugg, S.Dalla Torre-Colautti, J.R.Hall, E.Heer, R.Hess, J.C.Kluyver, R.A.Kunne, C.Lechanoine-Leluc, A.Penzo, D.Rapin, P.Schiavon, F.Tessarotto, A.Villari, A.M.Zanetti

Polarization at Small Angles in Antiproton-Carbon Elastic Scattering at LEAR Energies

NUCLEAR REACTIONS C(p-bar, p-bar), E at 800-1100 MeV/c; measured polarization parameter.

doi: 10.1016/0375-9474(88)90028-0
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1988SH06 Phys.Rev.Lett. 60, 901 (1988)

R.L.Shypit, D.V.Bugg, D.M.Lee, M.W.McNaughton, R.R.Silbar, N.M.Stewart, A.S.Clough, C.L.Hollas, K.H.McNaughton, P.Riley, C.A.Davis

Evidence against Broad Dibaryons

NUCLEAR REACTIONS ¹H(polarized p, π⁺n), E=492-796 MeV; measured spin correlation parameters; deduced no broad dibaryons. Isobar analysis.

doi: 10.1103/PhysRevLett.60.901
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1988SH09 Nucl.Phys. A477, 541 (1988)

R.L.Shypit, D.V.Bugg, D.M.Lee, M.W.McNaughton, R.R.Silbar, N.M.Stewart, A.S.Clough, C.L.Hollas, K.H.McNaughton, P.Riley, C.A.Davis

A(SL), A(LL) and A(N0) for NN → πD at 492, 729 and 796 MeV

NUCLEAR REACTIONS ¹H(polarized p, π⁺), E=492-796 MeV; measured spin correlation parameters A(LL), A(SL), A(N0). Longitudinally polarized propanediol target.

doi: 10.1016/0375-9474(88)90404-6
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1987BU13 Nucl.Phys. A467, 575 (1987)

D.V.Bugg, C.Wilkin

Polarisation in the (d, 2p) Reaction at Intermediate Energies

NUCLEAR REACTIONS ¹H(n, p), E=142 MeV; calculated charge exchange amplitudes. ¹H(d, 2p), (polarized d, 2p), E=200, 280 MeV; calculated tensor polarization, pp-singlet, triplet, effective σ. ²H(polarized p, n), E not given; deduced spin-transfer polarized neutron spectra. Impulse approximation, diagrammatic approach.

doi: 10.1016/0375-9474(87)90387-3
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1985BU04 Phys.Lett. 152B, 37 (1985)

D.V.Bugg, C.Wilkin

An Analyser of Deuteron Tensor Polarisation for the GeV/c Momentum Range

NUCLEAR REACTIONS ¹H(d, 2p), E at 0.6-3 GeV/c; calculated analyzing power t₂₀, t₂₂ vs momentum transfers.

doi: 10.1016/0370-2693(85)91134-7
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1985WA01 Nucl.Phys. A433, 649 (1985)

C.E.Waltham, R.Shypit, D.A.Axen, F.Entezami, M.Comyn, D.Healey, G.A.Ludgate, G.D.Wait, D.V.Bugg, J.A.Edgington, N.R.Stevenson

Spin-Spin Correlations and Spin Asymmetries for the Reaction p(pol)p(pol) → pnπ⁺ at Intermediate Energies

NUCLEAR REACTIONS ¹H(polarized p, pπ⁺), E=420, 465, 510 MeV; measured spin-spin correlation parameters, spin asymmetry vs proton momentum; deduced ¹D₂ partial wave dominance. Polarized target.

doi: 10.1016/0375-9474(85)90023-5
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1984BU02 J.Phys.(London) G10, 47 (1984)

D.V.Bugg

NN → πd Amplitudes up to 580 MeV

NUCLEAR REACTIONS ¹H(p, π⁺), (polarized p, π⁺), E=450-580 MeV; analyzed data; deduced reaction amplitudes.

doi: 10.1088/0305-4616/10/1/010
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1984BU12 J.Phys.(London) G10, 717 (1984)

D.V.Bugg

Amplitudes for NN → dπ up to 800 MeV

NUCLEAR REACTIONS ¹H(p, p), (polarized p, p), E=500-800 MeV; analyzed σ(θ), vector, tensor analyzing power, spin transfer coefficient data; deduced ¹S₀, ³F₂ amplitudes.

doi: 10.1088/0305-4616/10/6/008
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1984CL13 Phys.Lett. 146B, 299 (1984)

A.S.Clough, C.I.Beard, D.V.Bugg, J.A.Edgington, J.Hall, K.Bos, J.C.Kluyver, R.A.Kunne, L.Linssen, R.Birsa, F.Bradamante, S.Dalla Torre-Colautti, M.Giorgi, A.Martin, A.Penzo, P.Schiavon, A.Villari, S.Degli-Agosti, E.Heer, R.Hess, C.Lechanoine-Leluc, Y.Onel, D.Rapin

Evidence Against the S-Meson

NUCLEAR REACTIONS ¹H(p-bar, p-bar), E at 388-599 MeV/c; calculated σ; deduced no S-meson evidence.

doi: 10.1016/0370-2693(84)91700-3
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1983SH11 Phys.Lett. 124B, 314 (1983)

R.Shypit, C.E.Waltham, D.A.Axen, F.Entezami, M.Comyn, D.Healey, G.A.Ludgate, G.D.Wait, D.V.Bugg, J.A.Edgington, N.R.Stevenson

Spin-Spin Correlations and Spin-Asymmetries for the Reaction p(pol)p(pol) → pnπ⁺ at 510 MeV

NUCLEAR REACTIONS ¹H(polarized p, π⁺p), E=510 MeV; measured spin-spin correlation parameters, spin asymmetries. Polarized target.

doi: 10.1016/0370-2693(83)91461-2
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1983ST08 Nucl.Phys. A403, 525 (1983)

J.P.Stanley, N.M.Stewart, D.V.Bugg, J.A.Edgington, N.R.Stevenson, A.S.Clough, D.A.Axen, R.Shypit, M.Comyn, D.Healey, G.A.Ludgate

Measurements of Δσ(L) and Δσ(T) in pp Scattering between 200 and 520 MeV

NUCLEAR REACTIONS ¹H(polarized p, p), E=200, 520 MeV; measured spin-dependent σ differences. Longitudinal, transverse beam polarization, polarized target.

doi: 10.1016/0375-9474(83)90621-8
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1982DU03 Nucl.Phys. A377, 554 (1982)

R.Dubois, D.Axen, R.Keeler, M.Comyn, G.A.Ludgate, J.R.Richardson, N.M.Stewart, A.S.Clough, D.V.Bugg, J.A.Edgington

Nucleon-Nucleon Phase Shifts from 142 to 800 MeV

NUCLEAR REACTIONS ¹H(n, n), E=120-550 MeV; ¹H(p, p), E=120-831 MeV; analyzed σ(total), σ(θ); deduced unique set of phase shifts.

doi: 10.1016/0375-9474(82)90055-0
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1982KE02 Nucl.Phys. A377, 529 (1982)

R.K.Keeler, R.Dubois, E.G.Auld, D.A.Axen, M.Comyn, G.Ludgate, L.P.Robertson, J.R.Richardson, D.V.Bugg, J.A.Edgington, W.R.Gibson, A.S.Clough, N.M.Stewart, B.Dieterle

Neutron-Proton Scattering Cross Sections between 200 and 500 MeV

NUCLEAR REACTIONS ¹H(n, n), E=212, 268, 319, 369, 417, 495 MeV; measured σ(total), σ(θ). Liquid hydrogen target, transmission method.

doi: 10.1016/0375-9474(82)90054-9
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12884.

1981AX01 J.Phys.(London) G7, L225 (1981)

D.Axen, R.Shypit, M.Comyn, D.Healey, J.Stanley, N.M.Stewart, D.V.Bugg, J.A.Edgington, N.Stevenson

Δσ(L) and Δσ(T) between 200 amd 520 MeV

NUCLEAR REACTIONS ¹H(polarized p, p), E=200-520 MeV; measured σ(total), σ(transverse), σ(longitudinal) differences. Transmission method, polarized beam, polarized target.

doi: 10.1088/0305-4616/7/10/003
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1980AX01 Phys.Rev. C21, 998 (1980)

D.Axen, R.Dubois, R.Keeler, G.A.Ludgate, C.J.Oram, L.P.Robertson, N.M.Stewart, C.Amsler, D.V.Bugg, J.A.Edgington, W.R.Gibson, N.Wright, A.S.Clough

Neutron-Proton Elastic Scattering between 200 and 500 MeV. II. Measurement of R(t) and A(t)

NUCLEAR REACTIONS ¹H(polarized n, p), E=220, 325, 425, 495 MeV; measured P(θp); deduced parameters Rt(θ), At(θ).

doi: 10.1103/PhysRevC.21.998
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14193.

1980BU03 Phys.Rev. C21, 1004 (1980)

D.V.Bugg, J.A.Edgington, W.R.Gibson, N.Wright, N.M.Stewart, A.S.Clough, D.Axen, G.A.Ludgate, C.J.Oram, L.P.Robertson, J.R.Richardson, C.Amsler

Neutron-Proton Elastic Scattering between 200 and 500 MeV. III. Phase Shift Analysis

NUCLEAR REACTIONS ¹H(n, n), E=210, 325, 425, 515 MeV; calculated σ(θ). Phase shift analysis.

doi: 10.1103/PhysRevC.21.1004
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1980CL02 Phys.Rev. C21, 988 (1980)

A.S.Clough, D.R.Gibson, D.Axen, R.Dubois, L.Felawka, R.Keeler, G.A.Ludgate, C.J.Oram, C.Amsler, D.V.Bugg, J.A.Edgington, L.P.Robertson, N.M.Stewart, J.Beveridge, J.R.Richardson

Neutron-Proton Elastic Scattering between 200 and 500 MeV. I. Experimental Details and Measurements of the D(t) and P Parameters

NUCLEAR REACTIONS ¹H(polarized n, p), E=220, 325, 425, 495 MeV; measured analyzing power, polarization transfer vs θ.

doi: 10.1103/PhysRevC.21.988
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13495.

1978AM07 Nucl.Instrum.Methods 157, 203 (1978)

C.Amsler, R.C.Brown, D.V.Bugg, J.A.Edgington, C.Oram, D.Axen, R.Dubois, L.Felawka, S.Jaccard, R.Keeler, J.Vavra, A.Clough, D.Gibson, G.A.Ludgate, N.M.Stewart, L.P.Robertson, J.R.Richardson

A Monoenergetic Polarized Neutron Beam from 200 to 500 MeV

NUCLEAR REACTIONS ²H(polarized p, n), E=237, 343, 445, 516 MeV; measured polarization of n, polarization transfer R.

doi: 10.1016/0029-554X(78)90608-0
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1977AM04 Phys.Lett. 69B, 419 (1977)

C.Amsler, D.Axen, J.Beveridge, D.V.Bugg, A.S.Clough, J.A.Edgington, S.Jaccard, G.Ludgate, C.Oram, J.R.Richardson, L.Robertson, N.Stewart, J.Vavra

Neutron-Proton Elastic Scattering at 325 MeV

NUCLEAR REACTIONS ¹H(polarized n, n); measured polarization parameters. Phase shift analysis.

doi: 10.1016/0370-2693(77)90834-6
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1977AX01 Lett.Nuovo Cim. 20, 151 (1977)

D.Axen, L.Felawka, S.Jaccard, J.Vavra, G.A.Ludgate, N.M.Stewart, C.Amsler, R.C.Brown, D.V.Bugg, J.A.Edgington, C.J.Oram, K.Shakarchi, A.S.Clough

D, R, R' and P in pp Elastic Scattering from 209 to 515 MeV

NUCLEAR REACTIONS ¹H(polarized p, p), E=209-515 MeV; measured scattering parameters.

doi: 10.1007/BF02785134
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