NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = E.T.Boschitz Found 39 matches. 1992BO18 Nucl.Phys. A543, 17c (1992) Interaction of Pions with Few-Nucleon Systems NUCLEAR STRUCTURE 2H, 3,4He, 6Li; compiled, reviewed pion-nucleus interaction data, analyses.
doi: 10.1016/0375-9474(92)90408-C
1991BA60 Pisma Zh.Eksp.Teor.Fiz. 54, 549 (1991); JETP Lett.(USSR) 54, 551 (1991) N.A.Bazhanov, V.G.Vovchenko, V.A.Efimovykh, A.A.Zhdanov, A.I.Kovalev, S.I.Kalentarova, V.I.Murzin, V.V.Polyakov, A.N.Prokofev, V.Yu.Trautman, O.Ya.Fedorov, A.V.Shvedchikov, V.A.Shchedrov, E.I.Bunyatova, Yu.M.Kazarinov, Yu.A.Usov, E.T.Boschitz, B.Brinkmoller, M.Wessler Vector Analyzing Power iT11 in the π+ d → pp Reaction in the Energy Region 350-450 MeV NUCLEAR REACTIONS 2H(π+, 2p), E=350-450 MeV; measured iT11(θ). Polarized deuterated propanediol target.
1991RI01 Phys.Rev. C43, 745 (1991) S.Ritt, E.T.Boschitz, R.Meier, R.Tacik, M.Wessler, K.Junker, J.A.Konter, S.Mango, D.Renker, B.van den Brandt, V.Efimovykh, A.Kovaliov, A.Prokofev, R.Mach, P.Chaumette, J.Deregel, G.Durand, J.Fabre, W.Thiel Measurement of the Vector Analyzing Power iT11 in π+-6Li(pol) Scattering NUCLEAR REACTIONS 6Li(π+, π+), (π+, π+'), E=100-219 MeV; measured σ(θ), vector analyzing power vs θ. Vector polarized 6LiD target. Model analyses.
doi: 10.1103/PhysRevC.43.745
1990ME11 Phys.Rev. C42, 2222 (1990) R.Meier, E.T.Boschitz, S.Ritt, R.Tacik, M.Wessler, J.A.Konter, S.Mango, D.Renker, B.van den Brandt, W.Meyer, W.Thiel, R.Mach, P.Amaudruz, R.R.Johnson, G.R.Smith, P.Weber Pion Scattering from Polarized 15N at T(π) = 164 MeV NUCLEAR REACTIONS 15N(π+, π+), (π+, π+'), E=164 MeV; measured σ(E(π)), σ(θ), analyzing power vs θ. Polarized 15NH3 target. Momentum space coupled-channels formalism.
doi: 10.1103/PhysRevC.42.2222
1990TA24 Phys.Rev. C42, 1841 (1990) R.Tacik, E.T.Boschitz, W.Gyles, M.Wessler, S.Mango, B.van den Brandt, J.A.Konter, D.R.Gill, P.Weber Comparison of the Vector Analyzing Power iT11 for π±d Scattering at 180 MeV NUCLEAR REACTIONS 2H(π+, π+), (π-, π-), E=180 MeV; measured vector analyzing power iT11(θ). Polarized target, magnetic spectrometer.
doi: 10.1103/PhysRevC.42.1841
1990TA25 Phys.Rev. C42, 1846 (1990) R.Tacik, E.T.Boschitz, W.Gyles, C.R.Ottermann, M.Wessler, U.Wiedner, H.Garcilazo, R.R.Johnson Kinematically Complete Measurement of the π+d → π0pp Charge-Exchange Reaction NUCLEAR REACTIONS 2H(π+, π0p), E=228, 294 MeV; measured σ(θp1, θp2) vs proton momentum. Relativistic Faddeev formalism.
doi: 10.1103/PhysRevC.42.1846
1989GA03 Phys.Rev. C39, 942 (1989) H.Garcilazo, E.T.Boschitz, W.Gyles, W.List, C.R.Ottermann, R.Tacik, M.Wessler Polarization Observables in πd(pol) Elastic Scattering: Amplitude analysis NUCLEAR REACTIONS 2H(π, π), E=254, 294 MeV; analyzed polarization observables data; deduced πd helicity amplitudes. Polarized targets, amplitude analysis.
doi: 10.1103/PhysRevC.39.942
1989TA14 Phys.Rev. C40, 256 (1989) R.Tacik, E.T.Boschitz, W.Gyles, W.List, C.R.Ottermann, M.Wessler, U.Wiedner, R.R.Johnson Three-Nucleon Pion Absorption in Carbon NUCLEAR REACTIONS 12C(π+, 3p), E=130, 180, 228 MeV; measured σ(θ1, θ2, θ3); deduced absorption σ.
doi: 10.1103/PhysRevC.40.256
1989TA21 Phys.Rev.Lett. 63, 1784 (1989) R.Tacik, E.T.Boschitz, R.Meier, S.Ritt, M.Wessler, K.Junker, J.A.Konter, S.Mango, D.Renker, B.van den Brandt, W.Meyer, W.Thiel, P.Chaumette, J.Deregel, G.Durand, J.Fabre, P.Amaudruz, R.R.Johnson, G.Smith, P.Weber, R.Mach Spin Effects in π-Nucleus Scattering in the Region of the Δ(3, 3) Resonance NUCLEAR REACTIONS 15N(π+, π+), (π+, π+'), E=164 MeV; 6Li(π+, π+), (π+, π+'), E=134, 164 MeV; measured σ(θ), vector, tensor analyzing power vs θ. Polarized targets.
doi: 10.1103/PhysRevLett.63.1784
1988LI08 Phys.Rev. C37, 1587 (1988) W.List, E.T.Boschitz, H.Garcilazo, W.Gyles, C.R.Ottermann, R.Tacik, M.Wessler, U.Wiedner, R.R.Johnson Neutron-Proton Final-State Interaction in πd Breakup: Differential cross section NUCLEAR REACTIONS 2H(π+, np), E=294 MeV; measured σ(θ(π), θp) vs proton momentum; deduced np-final state interaction role. Kinematically complete experiment.
doi: 10.1103/PhysRevC.37.1587
1988LI09 Phys.Rev. C37, 1594 (1988) W.List, E.T.Boschitz, H.Garcilazo, W.Gyles, C.R.Ottermann, R.Tacik, S.Mango, J.A.Konter, B.van den Brandt, G.R.Smith Neutron-Proton Final-State Interaction in πd Breakup: Vector analyzing power NUCLEAR REACTIONS 2H(π+, np), E=134-228 MeV; measured iT11(θ) following breakup; deduced final state interaction role. Polarized target.
doi: 10.1103/PhysRevC.37.1594
1988OT06 Phys.Rev. C38, 2296 (1988) C.R.Ottermann, E.T.Boschitz, W.Gyles, W.List, R.Tacik, M.Wessler, S.Mango, B.van den Brandt, J.A.Konter, D.R.Gill, G.R.Smith Polarization Observables in πd(pol) Elastic Scattering: Analyzing powers T20 and τ21 NUCLEAR REACTIONS 2H(π, π), E=256, 294 MeV; measured absolute σ(θ), T20(θ), other observables. Tensor polarized target.
doi: 10.1103/PhysRevC.38.2296
1988OT07 Phys.Rev. C38, 2310 (1988) C.R.Ottermann, E.T.Boschitz, H.Garcilazo, W.Gyles, W.List, R.Tacik, M.Wessler, S.Mango, B.van den Brandt, J.A.Konter, E.L.Mathie Polarization Observables in πd(pol) Elastic Scattering: Analyzing powers τ22 and iT11 NUCLEAR REACTIONS 2H(π, π), E=134-294 MeV; measured iT11, T20, T21, T22 vs θ, other observables. Polarized target, frozen spin mode.
doi: 10.1103/PhysRevC.38.2310
1987SM02 Nucl.Instrum.Methods Phys.Res. A254, 263 (1987) G.R.Smith, P.Delheij, D.R.Gill, D.Healey, D.Ottewell, G.D.Wait, P.Walden, R.R.Johnson, G.Jones, F.M.Rozon, M.Sevior, F.Tervisidis, R.P.Trelle, E.L.Mathie, S.I.H.Naqvi, G.J.Lolos, C.R.Otterman, E.T.Boschitz, G.S.Kyle, P.A.Amaudruz Direct Measurement of the Tensor Polarization of a Polarized Deuteron Target NUCLEAR MOMENTS 2H; measured NMR; deduced vector polarization. Polarized target, 2H(π, 2p) data input.
doi: 10.1016/0168-9002(87)90673-5
1986GY01 Phys.Rev. C33, 583 (1986) W.Gyles, E.T.Boschitz, H.Garcilazo, W.List, E.L.Mathie, C.R.Ottermann, G.R.Smith, R.Tacik, R.R.Johnson π+d → π+pn Reaction as a Test of Relativistic Faddeev Theories: Differential cross section NUCLEAR REACTIONS 2H(π+, π+p), E=228, 294 MeV; measured σ(θπ, θp) vs proton momentum; deduced nonconventional dynamics insignificance. Faddeev method.
doi: 10.1103/PhysRevC.33.583
1986GY02 Phys.Rev. C33, 595 (1986) W.Gyles, E.T.Boschitz, H.Garcilazo, E.L.Mathie, C.R.Ottermann, G.R.Smith, S.Mango, J.A.Konter, R.R.Johnson π+d → π+pn Reaction as a Test of Relativistic Faddeev Theories: Vector analyzing power NUCLEAR REACTIONS 2H(π+, π+p), E=180, 228, 294 MeV; measured vector analysing power iT11(θπ, θp), σ(θπ, θp) vs proton momentum. Relativistic Faddeev method.
doi: 10.1103/PhysRevC.33.595
1986OT02 Phys.Rev. C33, 1802 (1986) C.R.Ottermann, E.T.Boschitz, W.Gyles, W.List, R.Tacik, S.Mango, J.A.Konter, B.van den Brandt, G.R.Smith Measurement of the πd(pol) → pp Reaction at T(π) = 65 MeV NUCLEAR REACTIONS 2H(π, p), E=65 MeV; measured vector analyzing power vs θ. Vector polarized target. Coupled-channels, Faddeev, perturbation theory calculations.
doi: 10.1103/PhysRevC.33.1802
1986SM06 Phys.Rev.Lett. 57, 803 (1986) G.R.Smith, A.Altman, P.Delheij, D.R.Gill, D.Healey, R.R.Johnson, G.Jones, D.Ottewell, F.M.Rozon, M.E.Sevior, F.Tervisidis, R.P.Trelle, G.D.Wait, P.Walden, E.L.Mathie, G.J.Lolos, S.I.H.Naqvi, E.T.Boschitz, C.R.Ottermann, G.S.Kyle, P.A.Amaudruz Tensor Analyzing Power in πd Elastic Scattering NUCLEAR REACTIONS 2H(π, π), E=138, 150.9 MeV; measured tensor analyzing power vs θ. Tensor polarized target. Faddeev calculations.
doi: 10.1103/PhysRevLett.57.803
1985MA17 Phys.Lett. 154B, 28 (1985) E.L.Mathie, G.R.Smith, E.T.Boschitz, W.Gyles, C.R.Ottermann, S.Mango, J.A.Konter, A.Matsuyama, R.R.Johnson, R.Olszewski First Measurement of iT11 in the Pion-Deuteron Breakup Reaction NUCLEAR REACTIONS 2H(π+, π+p), E=228 MeV; measured σ(θ), iT11(θ), σ(θp, θ(π)) vs proton momentum. Polarized target, kinematically complete experiment.
doi: 10.1016/0370-2693(85)91561-8
1985OT04 Phys.Rev. C32, 928 (1985) C.R.Ottermann, E.T.Boschitz, W.Gyles, W.List, R.Tacik, R.R.Johnson, G.R.Smith, E.L.Mathie Large Angle πd Scattering in the Region of the (3, 3) Resonance NUCLEAR REACTIONS 2H(π+, π+), E=124-324 MeV; measured σ(θ). Comparison with Faddeev calculation.
doi: 10.1103/PhysRevC.32.928
1985TA14 Phys.Rev. C32, 1335 (1985) R.Tacik, E.T.Boschitz, W.Gyles, W.List, C.R.Ottermann Measurement of Three Protons in Coincidence following Absorption of 228 MeV π+ in Carbon NUCLEAR REACTIONS C(π+, 3p), E=228 MeV; measured ppp-coin, σ(θ1, θ2, θ3), σ(θ1, θ2, E2), σ(θ1, θ3, E3); deduced three proton emission associated σ(absorption), reaction mechanism.
doi: 10.1103/PhysRevC.32.1335
1984SM03 Phys.Rev. C29, 2206 (1984) G.R.Smith, E.L.Mathie, E.T.Boschitz, C.R.Ottermann, S.Mango, J.A.Konter, M.Daum, M.Meyer, R.Olszewski, F.Vogler Measurements of the Vector Analyzing Power iT11 in the πd(pol) Elastic Scattering Reaction between 117 and 325 MeV NUCLEAR REACTIONS 2H(π+, π+), E=117-325 MeV; measured iT11(θ) vs E; deduced dibaryon resonance effects. Vector polarized target. Faddeev calculation comparison.
doi: 10.1103/PhysRevC.29.2206
1984SM06 Phys.Rev. C30, 980 (1984) G.R.Smith, E.L.Mathie, E.T.Boschitz, C.R.Ottermann, W.Gyles, W.List, S.Mango, J.A.Konter, B.van den Brandt, R.Olszewski, R.R.Johnson Vector Analyzing Power iT11 in the πd → 2p Reaction between 112 and 325 MeV NUCLEAR REACTIONS 2H(π, 2p), E=112-325 MeV; measured recoil deuteron iT11(θ). Faddeev calculation comparison.
doi: 10.1103/PhysRevC.30.980
1983IN02 Phys.Rev. C27, 1578 (1983) C.H.Q.Ingram, P.A.M.Gram, J.Jansen, R.E.Mischke, J.Zichy, J.Bolger, E.T.Boschitz, G.Probstle, J.Arvieux Quasielastic Scattering of Pions from 16O at Energies Around the Δ(1232) Resonance NUCLEAR REACTIONS 16O(π+, π+'), E=114, 163, 240 MeV; measured σ(θ, E(π)); deduced reaction mechanism, σ, charge exchange σ. Nuclear medium role, isobar propogation.
doi: 10.1103/PhysRevC.27.1578
1983MA74 Phys.Rev. C28, 2558 (1983) E.L.Mathie, G.R.Smith, E.T.Boschitz, M.Meyer, F.Vogler, M.Daum, S.Mango, J.A.Konter Search for Rapid Angular and Energy Dependence of d(sigma)/d(Omega) and iT11 in Large Angle π-d Elastic Scattering NUCLEAR REACTIONS 2H(π, π), E=117-151 MeV; measured σ(θ), iT11(θ); deduced smooth energy dependence. Polarized target.
doi: 10.1103/PhysRevC.28.2558
1977HE01 Nucl.Phys. A275, 212 (1977) E.F.Hefter, E.T.Boschitz, V.Heidt, C.Weddigen The Conventional DWBA and the Impulse Approximation for 14N(d, p0)15N at E = 52 MeV NUCLEAR REACTIONS 14N(d, p0), E=52 MeV; measured σ(θ). 15N deduced spectroscopic amplitude. DWBA, impulse approximation. Gas target.
doi: 10.1016/0375-9474(77)90284-6
1974UL02 Phys.Rev.Lett. 33, 433 (1974) H.Ullrich, E.T.Boschitz, H.D.Engelhardt, C.W.Lewis Multinucleon Removal in the Absorption of π- at Rest and at 60 MeV NUCLEAR REACTIONS 16O, 19F, 24Mg, 31P, 40Ca, 93Nb(π-, xnypγ), E=0, 60 MeV; measured π-γ-coin; deduced yields.
doi: 10.1103/PhysRevLett.33.433
1973LE22 Phys.Lett. 47B, 339 (1973) C.W.Lewis, H.Ullrich, H.D.Engelhardt, E.T.Boschitz Possible Alpha-Particle Cluster Absorption of Pions by 16O NUCLEAR REACTIONS 16O(π-, γ), E < 6.13 MeV; measured σ(Eγ).
doi: 10.1016/0370-2693(73)90617-5
1972BE57 Phys.Rev.Lett. 29, 1031 (1972) R.W.Bercaw, J.S.Vincent, E.T.Boschitz, M.Blecher, K.Gotow, D.K.Anderson, R.Kerns, R.Minehart, K.Ziock, R.Johnson Elastic Scattering of Negative Pions from 16O in the Region of the (3, 3) Resonance NUCLEAR REACTIONS 16O(π-, π-), E=160, 170, 220, 230, 240 MeV; measured σ(θ) near 3-3 resonance; deduced optical model parameters.
doi: 10.1103/PhysRevLett.29.1031
1972BO29 Phys.Rev. C6, 457 (1972) E.T.Boschitz, W.K.Roberts, J.S.Vincent, M.Blecher, K.Gotow, P.C.Gugelot, C.F.Perdrisat, L.W.Swenson, J.R.Priest Elastic Scattering of 600-MeV Protons from H, D, 3He, and 4He NUCLEAR REACTIONS 1,2H, 3,4He(p, p), E=600 MeV; measured σ(θ), P(θ).
doi: 10.1103/PhysRevC.6.457
1970BL05 Phys.Rev.Lett. 24, 1126 (1970) M.Blecher, K.Gotow, E.T.Boschitz, W.K.Roberts, J.S.Vincent, P.C.Gugelot, C.F.Perdrisat Elastic Scattering of 580-MeV Protons from 3He NUCLEAR REACTIONS 3He(p, p), E=580 MeV; measured σ(Ep, E(3He)).
doi: 10.1103/PhysRevLett.24.1126
1970VI01 Nucl.Phys. A143, 121 (1970) Interaction of 42 MeV α-Particles with 3He NUCLEAR REACTIONS 3He(α, α), (α, p), E=42 MeV; measured σ(θ); deduced optical model parameters. Enriched target.
doi: 10.1016/0375-9474(70)90685-8
1969PE15 Phys.Rev. 187, 1201 (1969) C.F.Perdrisat, L.W.Swenson, P.C.Gugelot, E.T.Boschitz, W.K.Roberts, J.S.Vincent, J.R.Priest (p, 2p) Reactions at 600 MeV on Deuterium and Helium-4 NUCLEAR REACTIONS 2H, 4He(p, 2p), E=600 MeV; measured σ(Ep1, Ep2, θ(p1), θ(p2)).
doi: 10.1103/PhysRev.187.1201
1967VI02 Phys.Letters 25B, 81 (1967) J.S.Vincent, E.T.Boschitz, J.R.Priest Large Angle Alpha Particle Scattering from the 3+ Unnatural Parity States in Magnesium NUCLEAR STRUCTURE 24Mg, 26Mg; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(67)90183-9
1967WA01 Phys.Letters 24B, 91 (1967) R.E.Warner, J.S.Vincent, E.T.Boschitz A Search for Unbound T = 1/2 Levels in 3He NUCLEAR STRUCTURE 3He; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(67)90353-X
1964BE03 Bull. Am. Phys. Soc. 9, No. 1, 55, FA2 (1964) R.W.Bercaw, E.T.Boschitz, J.S.Vincent Scattering of 19-MeV Polarized Protons by Light Nuclei NUCLEAR STRUCTURE 39K, 28Si, 32S, 9Be, 16O; measured not abstracted; deduced nuclear properties.
1964BO06 Bull. Am. Phys. Soc. 9, No. 4, 439, EA2 (1964) E.T.Boschitz, R.W.Bercaw, J.S.Vincent Proton Polarization in Inelastic Scattering at 19 MeV NUCLEAR STRUCTURE 20Ne, 32S, 28Si, 24Mg, 88Sr; measured not abstracted; deduced nuclear properties.
1964BO27 Phys. Letters 13, 322 (1964) E.T.Boschitz, R.W.Bercaw, J.S.Vincent Effects of Nuclear Structure on the Scattering on Polarized Protons NUCLEAR STRUCTURE 39K, 40Ar, 40Ca, 116Sn, 122Sn; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.13.442
1963BO34 Bull.Am.Phys.Soc. 8, No.8, 611, N2 (1963) E.T.Boschitz, R.W.Bercaw, J.S.Vincent Polarization of 18-MeV Protons Elastically Scattered from the Isobars Ar40 and Ca40 NUCLEAR STRUCTURE 40Ar, 40Ca; measured not abstracted; deduced nuclear properties.
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