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Measurement of the Ratio Between the Real and the Imaginary Part of the K- p Forward Scattering Amplitude at 14.3-GeV/c

De Boer, R.J. ; Van Dam, Piet ; Meijer, R.W. ; et al.

Nucl.Phys.B 106 (1976) 125-135, 1976.

Inspire Record 113577 DOI 10.17182/hepdata.35923

Elastic scattering of 14.3 GeV/ c K − with protons has been analyzed in the | t | region between 0.005 and 0.550 (GeV/ c ) 2 . The ratio α between the real and the imaginary part of the elastic forward scattering amplitude is found to be α =+0.056 ± 0.052. The slope parameters A and B in the expression d σ /d| t | ∞ exp( At + Bt 2 ) are A = 8.47 ± 0.20 (GeV/ c ) −2 and B = 1.82 ± 0.52 (GeV/ c ) −4 .

2 data tables

Table 1

Axis error includes +- 0.05/0.05 contribution.

Table 2

No description provided.

Reactions K- p --> Sigma+ pi- and K- p --> Sigma- pi+ at 3.13-GeV/c and 3.3-GeV/c

Mason, G.C. ; Wohl, C.G. ;

Nucl.Phys.B 103 (1976) 279-295, 1976.

Inspire Record 113041 DOI 10.17182/hepdata.36055

We have measured the differential cross sections for K − p→ Σ + π − and K − p→ Σ − π + scattering, and the polarization distribution of the Σ + in the first reaction, at K − lab momenta of 3.13 and 3.30 GeV/ c . Our K − p→ Σ + π − cross sections are at least 40% larger than interpolations between measurements at nearby momenta. A comparison using isospin conservation of K − p →Σ + π − , K − p →Σ − π + , and K 0 p → Σ 0 π + cross sections favors our results. The K − p→ Σ + π − differential cross sections have about the same shape and are about twice as large as corresponding K − p→ Λπ 0 differential cross sections across the whole forward region. We discuss the results briefly with reference to simple exchange models.

6 data tables

Table 1

No description provided.

Table 2

TMIN = 0.018 GEV**2. TMAX = 4.67 GEV**2.

Table 3

TMIN = 0.017 GEV**2. TMAX = 4.98 GEV**2.

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Measurement of the p Parameter in pi+ p Scattering in the Energy Region of the P33 Resonance

Amsler, Claude ; Dubal, L. ; Eaton, G.H. ; et al.

Lett.Nuovo Cim. 15 (1976) 209-213, 1976.

Inspire Record 113333 DOI 10.17182/hepdata.37429

None

5 data tables

Table 1

No description provided.

Table 2

No description provided.

Table 3

No description provided.

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Experimental Test for the 1 >= Delta I (Isospin) Rule in Electromagnetic Transitions

Christ, A. ; Noldeke, G. ; Nuding, W. ; et al.

Nucl.Phys.B 102 (1976) 429-438, 1976.

Inspire Record 112957 DOI 10.17182/hepdata.35990

At the Bonn 500 MeV synchrotron the differential cross sections for the photoproduction of neutral pions on protons and neutrons have been measured in a single experiment using a target of liquid deuterium. The final state has been completely determined by measuring the outgoing pion and one nucleon in coincidence. Measurements of the ratio R = π 0 n/ π 0 p have been done at different angles and energies. The possible existence of an isotensor contribution has been limited to (−2 ± 3)% of the isovector amplitude.

1 data table

Table 1

No description provided.

pi+ p Scattering Below 100-MeV

Bertin, P.Y. ; Coupat, B. ; Hivernat, A. ; et al.

Nucl.Phys.B 106 (1976) 341-354, 1976.

Inspire Record 113573 DOI 10.17182/hepdata.35966

The π + p cross section for elastic scattering from hydrogen was measured at seven incident energies ranging from 20.8 to 95.9 MeV for an angular range from 60° to 145°. The experimental set-up is discussed in detail as well as the method used for data analysis. A table of results and a set of phase shifts are provided.

7 data tables

Table 1

No description provided.

Table 2

No description provided.

Table 3

No description provided.

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The Exclusive Channel pi- pi- pi+ p in pi- p Interactions at 147-GeV/c.

Fong, D. ; Heller, M. ; Shapiro, A.M. ; et al.

Nuovo Cim.A 34 (1976) 659-671, 1976.

Inspire Record 112629 DOI 10.17182/hepdata.37618

The results of a study of the reaction π-p→π-π-π+p at2 147 GeV/c carried out at the Fermilab Proportional Wire 30″ Bubble Chamber Hybrid Spectrometer are reported. More than 92% of the cross-section ((670±41) μb) for this reaction is contained in those for proton and pion diffraction dissociation. The cross-sections for pion diffraction events with three-pion invariant mass in given regions are in agreement with values obtained by extrapolation of fits to data at lower incidentpion momenta. ρ0π- events make an important contribution in the A1 and A2 mass regions, and the data are consistent with contributions from f0π- in the A3 mass region. The cross-section for proton diffraction events is in agreement with a smooth extrapolation of the data at lower momentum.

1 data table

Table 1

No description provided.

Angular Dependence of the Polarization of the Recoil Proton from the Reaction gamma p --> pi0 p in the Region of the Second Resonance

Blum, P. ; Brinckmann, P. ; Brockmann, R. ; et al.

Z.Phys.A 277 (1976) 311, 1976.

Inspire Record 108242 DOI 10.17182/hepdata.16619

The polarization of the recoil proton from the reactionγp→π0p has been measured for photon energies between 600 and 1,200 MeV and pion c.m. angles between 90° and 150°.

1 data table

Table 1

No description provided.

Angular Dependence of the Polarization of the Recoil Proton from the Reaction gamma p --> pi0 p in the Region of the Third Resonance

Blum, P. ; Brockmann, R. ; Mohr, W. ;

Z.Phys.A 278 (1976) 275, 1976.

Inspire Record 108304 DOI 10.17182/hepdata.16615

The polarization of the recoil proton from the reactionγp→π0p has been measured for photon energies between 900–1,350 MeV and pion c.m. angles between 70° and 150°. There are significant deviations from recent analysis.

3 data tables

Table 1

No description provided.

Table 2

No description provided.

Table 3

No description provided.