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Search: Author = E.T.Boschitz

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1992BO18      Nucl.Phys. A543, 17c (1992)

E.T.Boschitz

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
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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
Citations: PlumX Metrics


1970VI01      Nucl.Phys. A143, 121 (1970)

J.S.Vincent, E.T.Boschitz

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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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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