Negative-to-Positive Ratio of Photomesons from Deuterium

Sands, Matthew ; Teasdale, J.G. ; Walker, Robert L. ;
Phys.Rev. 95 (1954) 592-593, 1954.
Inspire Record 944931 DOI 10.17182/hepdata.589

None

2 data tables

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Differential cross-sections for photoproduction of positive pions in hydrogen I. — low energies

Beneventano, M. ; Bernardini, G. ; Carlson-Lee, D. ; et al.
Nuovo Cim. 4 (1956) 323-356, 1956.
Inspire Record 1185320 DOI 10.17182/hepdata.37599

The cross-sections σ(Eγ,ϑ ) for the reaction pγ→ n+ have been measured near threshold as a function of photon energy and at four angles. See Table I. These results combined with previously known data, have given a fairly complete and accurate description of σ(Eγ,θ) between the limits 30°≤θ≤180° and 170≤ Eγ 270 MeV. See Table II and Pig. 2. Writing σ(Eγ,θ) = W·a0 + a1 cos θ + a2 cos2 θ× withW= ηωl +(μ/Ei)ξ −1·l + (μ/E f )ω×−1 (see formula (5)) the experimental data indicate that (Table III) a0 is constant up to about Eγ ≃ 260 MeV; and that (Table V) the three ai coefficients analyzed in terms ofS andP waves give a very small spin flippingP-amplitudeK. The presumption that theS amplitudeE 1 ismainly due to the gauge invariance requirement is definitely not consistent with the data (see Table IV). A discussion based on the Kroll and Rudermann theorem leads to the conclusion that this inconsistency may be eliminated if allowance is made for the contribution of fairly large nucleon recoils. However, it turns out that only the changing sign part of these recoils is really large and apparently so up to terms of order higher than μM. The amount of the recoil at threshold is estimated and consequently a value for the pspv interaction constant is derived.

7 data tables

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Photoproduction of charged pions in deuterium

Beneventano, M. ; Bernardini, G. ; Stoppini, G. ; et al.
Nuovo Cim. 10 (1958) 1109-1142, 1958.
Inspire Record 1184858 DOI 10.17182/hepdata.37846

perimental analysis of the process is presented. Theσ(−)/σ(+) ratio has been measured in the photon energy interval (170÷230) MeV and Lab. angles 45°, 75°, 105°, 150°. The results are interpreted on the base of the impulse approximation with the aim of getting information on the processhv+n →π −+p.

6 data tables

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Form factor ...

Barkov, L.M. ; Blinov, G.A. ; Vasserman, I.B. ; et al.
NOVO-82-122, 1982.
Inspire Record 1501544 DOI 10.17182/hepdata.76464

None

1 data table

Axis error includes +- 7/7 contribution (/LUMINOCITY, RADIATIVE CORRECTIONS, NUCLEAR ABSORPTION AND DECAY IN FLIGHT).


Proton compton effect

Bernardini, G. ; Hanson, A.O. ; Odian, A.C. ; et al.
Nuovo Cim. 18 (1960) 1203-1236, 1960.
Inspire Record 1184998 DOI 10.17182/hepdata.37758

The elastic scattering of photons by protons has been measured for 100 MeV to 290 MeV photons at 90° c.m.s. and 139° c.m.s. scattering angles. The expected large increase in cross-section is observed at energies approaching that of (3/2, 3/2) pion-nucleon resonance. The scattering can be qualitatively explained by the ordinary Thomson amplitude combined with that of the (3/2, 3/2) resonance. A more detailed examination of the cross-section in the region just above the photo-meson threshold has shown that it is sensitive to the π0 photon coupling. From the experimental data, one may conclude that the π0 mean life should be between 10−16 and 10−18 s.

1 data table

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