Date

Discontinuous behaviour in large angle proton-proton elastic scattering at high energies

Allaby, J.V. ; Cocconi, G. ; Diddens, A.N. ; et al.
Phys.Lett.B 25 (1967) 156-159, 1967.
Inspire Record 1389227 DOI 10.17182/hepdata.754

Measurements of elastic proton-proton differential cross sections for angles between 65° and 90° c.m.s. have been made at 8, 9, 10, 11, 14, 15 and 21 GeV/c. The shape of the angular distribution is found to change suddenly between 8 and 11 GeV/c. An interpretation of this discontinuous behaviour in terms of the reactive effects of baryon-antibaryon pair production is proposed.

2 data tables

No description provided.

No description provided.


Single photoproduction of neutral π-mesons on hydrogen at small angles between 1.3 and 3 GeV

Braunschweig, M. ; Husmann, D. ; Lübelsmeyer, K. ; et al.
Phys.Lett. 22 (1966) 705-708, 1966.
Inspire Record 1389452 DOI 10.17182/hepdata.753

The differential cross section of the reaction γ + p → p + πo has been measured at the Deutsches Elektronen- Synchrotron, Hamburg, at mean phonon energies of 1.36, 2.0 and 3.0 GeV and pion center of mass angles between 0o and 70o. The results are compared with some theoretical calculations based on elementary and reggeized 1- meson exchange.

4 data tables

Axis error includes +- 12/12 contribution.

Axis error includes +- 12/12 contribution.

Axis error includes +- 12/12 contribution.

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Proton-antiproton interactions at 3.6 GeV/c and one pion exchange

Dehne, H.C. ; Raubold, E. ; Söding, P. ; et al.
Phys.Lett. 9 (1964) 185-187, 1964.
Inspire Record 1389629 DOI 10.17182/hepdata.27257

None

1 data table

The cross section for the reaction PBAR P --> INELASTIC comprises pion production without annihilation and without strange particle production.


Energy dependence of the spin-spin correlation parameter $C_{NN}$ at 50° and 90° c.m. for pp-elastic scattering in the energy range 0.69–0.95 GeV

Efimovyh, V.A. ; Kovalev, A.I. ; Poljakov, V.V. ; et al.
Phys.Lett.B 99 (1981) 28-32, 1981.
Inspire Record 1389635 DOI 10.17182/hepdata.27135

The spin-spin correlation parameter C NN at 50° and 90° c.m. for elastic pp-scattering has been obtained in the energy range 0.69–0.95 GeV. It was found that the parameter C NN (90°) shows resonance-like structure at energies near 700 MeV. Its energy dependence does not agree with Hoshizaki's phase-shift analysis predictions. C NN (50°) agrees well with these predictions and does not show any structure within the accuracy of the measurements.

1 data table

No description provided.


Nuclear reactions of silver with 25.2 GeV $^{12}$C

Rudy, C.R. ; Porile, N.T. ;
Phys.Lett.B 59 (1975) 240-243, 1975.
Inspire Record 1389455 DOI 10.17182/hepdata.27780

Nuclear reactions induced in silver by 25.2 GeV 12C ions have been studied by the activation technique and compared with those induced by 300 GeV protons.

1 data table

Two sets of data were normalized to each other by requiring that the weighted mean of 15 cross section ratios for products in A = 66 - 90 region be equal to unity. SIG(C=PROTON) stands for the reacion with proton beam (PLAB=300 GeV) with the same final state.


Reaction cross sections for 65 MeV protons on targets from $^9$Be to $^{208}$Pb

Ingemarsson, A. ; Nyberg, J. ; Renberg, P.U. ; et al.
Nucl.Phys.A 653 (1999) 341-354, 1999.
Inspire Record 1389640 DOI 10.17182/hepdata.36231

Reaction cross sections for 65.5 MeV protons have been measured for 9 Be, 12 C, 16 O, 28 Si, 40 Ca, 58,60 Ni, 112.116.118.120.124 Sn, and 208 Pb. The results are compared with optical model predictions using relativistic global potentials.

13 data tables

No description provided.

No description provided.

No description provided.

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Emission of helium ions after antiproton annihilation in nuclei

Markiel, W. ; Daniel, H. ; Von Egidy, T. ; et al.
Nucl.Phys.A 485 (1988) 445-460, 1988.
Inspire Record 1389648 DOI 10.17182/hepdata.37037

Spectra of hydrogen and helium ions emitted after stopped antiproton annihilation in nuclei have been measured with a Si-detector telescope. Targets of 12 C, 40 Ca, 63 Cu, 92 Mo, 98 Mo and 238 U were used. The 3 He and 4 He energy spectra can be fitted with the exponential function e − E / T . The parameter T is essentially independent of the target mass number A . A simple pickup model reproduces the 4 He/ 3 He ratios as a function of Z and N (target proton and neutron number). The proton spectra from the 238 U target indicate that some protons are also emitted by the fission fragments.

11 data tables

No description provided.

No description provided.

No description provided.

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Single photoproduction of neutral $\pi$-mesons on hydrogen at small angles between 4 and 5.8 GeV

Braunschweig, M. ; Braunschweig, W. ; Husmann, D. ; et al.
Phys.Lett.B 26 (1968) 405-409, 1968.
Inspire Record 1389637 DOI 10.17182/hepdata.29336

The differential cross-section of the reaction γ + p → p + π 0 was measured at the Deutsches Elektronen-Synchrotron, Hamburg, at mean photon energies of 4.0, 5.0 and 5.8 GeV and pion center of mass angles between 0° and 60°. The results are compared wiht theoretical calculations based on Reggeized vector meson exchange.

6 data tables

Axis error includes +- 7/7 contribution.

Axis error includes +- 7/7 contribution.

Axis error includes +- 7/7 contribution.

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An accurate determination of the total pair production cross section in carbon, aluminium, copper and lead for photons from 1.200 to 4.050 GeV

Knasel, T.M. ; Walker, J.K. ;
Phys.Lett.B 27 (1968) 103-105, 1968.
Inspire Record 1389649 DOI 10.17182/hepdata.29227

The total pair production cross section for photons of energies 1.200 to 4.050 GeV has been measured for targets of carbon, aluminium, copper and lead by a good geometry absorption technique. The accuracy of the work is ± 0.3%.

1 data table

The errors are the sum in quadrature of the statistical and systematical errors.


Kaonic disintegration of the deuteron near 400 MeV/c

Cline, D. ; Laumann, R. ; Mapp, J. ;
Phys.Lett.B 27 (1968) 110-112, 1968.
Inspire Record 1389657 DOI 10.17182/hepdata.29226

The processes K − d → Σ − p and K − d → Λn have been observed at K − momenta of 340 MeV/c and 400 MeV/c. The cross sections for these processes are: σ ( Σ − p) = 200 ± 30 μ b at 400 MeV/c, σ ( Λ n) = 200 ± 30 μ b at 400 MeV/c, σ ( Σ − p) = 300 ± 100 μ b at 340 MeV/c, σ ( Λ n) = 360 ± 150 μ b at 340 MeV/c.

1 data table

No description provided.