Inclusive pi0 Production in pi- p Interactions at 5-GeV/c

Burleson, G. ; Hicks, G. ; Wilson, C.L. ; et al.
Phys.Rev.D 12 (1975) 2557-2560, 1975.
Inspire Record 104821 DOI 10.17182/hepdata.24848

We have measured the cross section for the reaction π−p→π0+anything at an incident momentum of 5 GeV/c. The two γ rays from π0 decays were detected using a 150-element lead-glass hodoscope array. A comparison is given of the inclusive π0 spectrum from hydrogen (obtained through a subtraction of CH2 and C target data) with π0 production from C and Cu.

4 data tables

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The Charge Form Factor of the Proton at a Momentum Transfer of 75 F$^-^2$

Bartel, W. ; Dudelzak, B. ; Krehbiel, H. ; et al.
Phys.Lett.B 25 (1967) 236-237, 1967.
Inspire Record 1333753 DOI 10.17182/hepdata.29448

The proton form factors GE(q2) and GM(q2) are determined at q2 = 75fm−2.

2 data tables

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Pion-deuteron coherent scattering at 895 mev/c

Bradamante, F. ; Conetti, S. ; Fidecaro, G. ; et al.
Phys.Lett.B 28 (1968) 191-194, 1968.
Inspire Record 56839 DOI 10.17182/hepdata.29099

The elastic scattering cross-section of π - on deuterium at 895 MeV/ c measured with counters and wire spark chambers is given in a region of momentum transfer between 0.16 and 0.96 (GeV/ c ) 2 .

1 data table

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EXCITATION OF THE 15.1-MeV AND 16.1-MeV LEVELS OF THE C-12 NUCLEUS BY ELECTRON SCATTERING

Dudelzak, B. ; Taylor, R.E. ;
J.Phys.Radium 22 (1961) 544, 1961.
Inspire Record 16520 DOI 10.17182/hepdata.37717

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6 data tables

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On the construction of pion photoproduction amplitudes from experimental data

Alvarez-Estrada, R.F. ; Sanchez-Gomez, J.L. ;
Nucl.Phys.B 26 (1971) 433-444, 1971.
Inspire Record 68784 DOI 10.17182/hepdata.76722

New formulae for constructing the pion photoproduction amplitude J from experimental data are presented. The phase of J is expressed in terms of its zeroes in the energy plane, the particle poles and a dispersion integral over the modulus of J , the latter being given, except for a finite unphysical interval, in terms of differential cross sections and recoil nucleon polarizations. For γ p→ π + n at t ≈−0.870 μ 2 , where the unphysical-region contribution vanishes, the zeroes are found approximately, so that the phase of J can be uniquely determined from the experimental data.

3 data tables