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Electromagnetic proton form-factors at squared four momentum transfers between 1-GeV/c2 and 3-GeV/c2

Bartel, W. ; Busser, F.W. ; Dix, W.R. ; et al.

Phys.Lett.B 33 (1970) 245-248, 1970.

Inspire Record 63047 DOI 10.17182/hepdata.45284

Electron-proton elastic scattering cross sections have been measured at four-momentum transfers between 1.0 and 3.0 (GeV/ c ) 2 and at electron scattering angles between 10° and 20° and at about 86° in the laboratory. The proton electromagnetic form factors G E and G M were determined. The results indicate that G E ( q 2 ) decreases faster with increasing q 2 than G M ( q 2 ).

2 data tables

Table 1

Axis error includes +- 2.5/2.5 contribution (Due to counting statisticss, separation of elastic events, beam monitoring, incident energy, scattering angle, proton absorption, solid angle, target length and density).

Table 2

CONST(NAME=MU) is the magnetic moment.

Study of k- pi- scattering using the reaction k- d ---> k- pi- p p(s)

Cho, Y. ; Derrick, M. ; Johnson, D. ; et al.

Phys.Lett.B 32 (1970) 409-412, 1970.

Inspire Record 63111 DOI 10.17182/hepdata.28719

Approximately 700 events of the reaction K − d → K − π − pp s produced by 5.5 GeV/ c kaons were used to measure the cross section for Kπ elastic scattering in the T = 3 2 state by a Chew-Low extrapolation. The cross section does not exceed 2.1 mb and has no structure for Kπ masses from threshold up to 2.0 GeV.

1 data table

Table 1

Chew-Low extrapolation is used for evaluation of the K- P elastic cross section.

Inelastic electron - proton scattering at fixed four momentum transfer of 0.773-GeV/c2 and 1.935-GeV/c2

Albrecht, W. ; Brasse, F.W. ; Dorner, H. ; et al.

DESY-69-7, 1969.

Inspire Record 56612 DOI 10.17182/hepdata.45281

None

4 data tables

Table 1

No description provided.

Table 2

No description provided.

Table 3

No description provided.

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Photoproduction of eta meson between threshold and 900 mev

Delcourt, B. ; Lefrancois, J. ; Perez-Y-Jorba, J.P. ; et al.

Phys.Lett.B 29 (1969) 75-78, 1969.

Inspire Record 56793 DOI 10.17182/hepdata.28963

We have measured differential cross sections of γ + p → p + η 0 at several energies. The angular distributions show that S 11 production is predominant in the energy range investigated and that the other resonant terms seen in π-production of η are absent or very low. Finally, experimental data are theoretically interpreted and the S 11 parameters deduced.

6 data tables

Table 1

No description provided.

Table 2

No description provided.

Table 3

No description provided.

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$\pi^+$ $\pi^-$ production in $e^+$ $e^-$ collisions and $\rho$-$\omega$ interference

Augustin, J.E. ; Benaksas, D. ; Buon, J. ; et al.

(1969) 35, 1969.

Inspire Record 58289 DOI 10.17182/hepdata.37427

None

1 data table

Table 1

RELATIVE PRODUCTION OF PION PAIRS WITHOUT RADIATIVE CORRECTIONS.

Omega-neutral production by e-plus e-minus annihilation

Augustin, J.E. ; Benaksas, D. ; Buon, J. ; et al.

Phys.Lett.B 28 (1969) 513-516, 1969.

Inspire Record 56682 DOI 10.17182/hepdata.29065

The reaction e + e − → ω o has been measured by detecting the charged pions of the π + π − π o decay mode of the ω o. A partial decay width of ω o in e + e − : Γ e + e − =0.94±0.18 keV is deduced from this result.

1 data table

Table 1

FITTED, BACKGROUND SUBTRACTED, PEAK OMEGA CROSS SECTION, CORRECTED FOR UNOBSERVED DECAYS, IS 1.82 +- 0.34 MUB. TABULATED ASSUMING CENTRAL ENERGY IS 782.6 MEV. VACUUM POLARIZATION AND RADIATIVE CORRECTIONS APPLIED.

Study of Electron-Positron Annihilation into pi+pi- at 775 MeV with the Orsay Storage Ring

Augustin, J.E. ; Bizot, J.C. ; Buon, J. ; et al.

Phys.Rev.Lett. 20 (1968) 126-129, 1968.

Inspire Record 54563 DOI 10.17182/hepdata.21756

None

1 data table

Table 1

No description provided.

Deuteron Electromagnetic Form Factors for F-3-2 < q2 < F-6-2

Benaksas, D. ; Drickey, D. ; Frerejacque, D. ;

Phys.Rev. 148 (1966) 1327-1331, 1966.

Inspire Record 944953 DOI 10.17182/hepdata.26653

Two groups of measurements have been made on the elastic scattering of electrons by deuterium; in each case we observed the recoil deuteron instead of the scattered electron. In the first case the spectrometer was set at 45° so that magnetic scattering was unimportant (about 10%) and we deduced the electric form factors of the deuteron. In the second case deuterons were observed at 0°, allowing us to measure directly the magnetic form factor of the deuteron. Form factors of the neutron were deduced from these measurements for the transfer values q2=3, 4, and 5 (F−2). Preliminary results were given in a first paper. Here we also include a description of the experimental setup and discuss relativistic and exchange-current corrections.

3 data tables

Table 1

No description provided.

Table 2

No description provided.

Table 3

No description provided.

PROTON FORM-FACTORS FROM PROTON OBSERVATION

Frerejacque, Daniel ; Benaksas, David ; Drickey, Darrell James ;

Phys.Rev. 141 (1966) 1308-1312, 1966.

Inspire Record 48595 DOI 10.17182/hepdata.26652

A determination of the electric and magnetic form factors of the proton has been made by studying the elastic scattering of electrons from a polyethylene target by observation of the recoiling proton at 0° and 30° for values of q2 between 1 and 1.8 F−2. From these measurements we have deduced the charge radius Rc and the magnetic radius Rm of the proton and find equality within the experimental errors (Rc=0.800±0.025 F; Rm=0.810±0.029 F).

8 data tables

Table 1

No description provided.

Table 2

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Table 3

No description provided.