Measurement of the anti-p p --> K(S) K(S) eta cross section at beam momenta in the regions of 1.45-GeV/c and 1.7-GeV/c.

Barnes, P.D. ; Bunker, B. ; Dennert, H. ; et al.
Phys.Lett.B 516 (2001) 257-263, 2001.
Inspire Record 559482 DOI 10.17182/hepdata.41678

The PS185 experiment at LEAR/CERN has investigated strangeness production in antiproton-proton collisions with final states such as $\overline{\Lambda} \Lambda$, $\overline{\Sigma}^0 \Lambda + c.c$, $\overline{\Sigma^+} \Sigma^+$, $\overline{\Sigma^-} \Sigma^-$ and $K_S K_S$. Results are presented from a study of about 32,000 {$K_S K_S X$} events obtained at several antiproton momenta in the regions of 1.45 and 1.7 GeV/c. The $\overline{p} p \to K_S K_S \eta$ cross sections extracted at these momenta constitute the first measurement of this reaction in flight and are broadly consistent with expectations of a phase-space extrapolation of branching ratios from annihilation at rest.

1 data table

No description provided.


Mechanism of the close-to-threshold production of the eta meson.

Czyzykiewicz, R. ; Moskal, P. ; Adam, H.-H. ; et al.
Phys.Rev.Lett. 98 (2007) 122003, 2007.
Inspire Record 731185 DOI 10.17182/hepdata.41775

Measurements of the analysing power for the p(pol)p --> ppeta reaction have been performed in the close-to-threshold energy region at beam momenta of p_{beam}=2.010 and 2.085 GeV/c, corresponding to excess energies of Q=10 and 36 MeV, respectively. The determined analysing power is essentially consistent with zero implying that the eta meson is produced predominantly in the s-wave at both excess energies. The angular dependence of the analysing power, combined with the hitherto determined isospin dependence of the total cross section for the eta meson production in nucleon-nucleon collisions, reveal a statistically significant indication that the excitation of the nucleon to the S_{11}(1535) resonance, the process which intermediates the production of the eta meson, is predominantly due to the exchange of the pi meson between the colliding nucleons.

2 data tables

Analysing power measurements for excess energy 10 MeV.

Analysing power measurements for excess energy 36 MeV.


LONGITUDINAL CORRELATIONS BETWEEN PIONS IN INCIDENT HADRON FRAGMENTATION REGION IN K- p INTERACTIONS AT 32-GeV/c

Bumazhnov, V.A. ; Buschbeck, B. ; Cochet, C. ; et al.
IFVE-81-112, 1981.
Inspire Record 168441 DOI 10.17182/hepdata.41430

None

62 data tables

DISTRIBUTION IS PRESENTED IN THE BEAM FRAGMENTATION REGIONS.

DISTRIBUTION IS PRESENTED IN THE BEAM FRAGMENTATION REGIONS.

DISTRIBUTION IS PRESENTED IN THE BEAM FRAGMENTATION REGIONS.

More…

Kaon pair production close to threshold.

Winter, P. ; Wolke, M. ; Adam, H.-H. ; et al.
Phys.Lett.B 635 (2006) 23-29, 2006.
Inspire Record 710616 DOI 10.17182/hepdata.41803

The total cross section of the reaction pp->ppK+K- has been measured at excess energies Q=10 MeV and 28 MeV with the magnetic spectrometer COSY-11. The new data show a significant enhancement of the total cross section compared to pure phase space expectations or calculations within a one boson exchange model. In addition, we present invariant mass spectra of two particle subsystems. While the K+K- system is rather constant for different invariant masses, there is an enhancement in the pK- system towards lower masses which could at least be partially connected to the influence of the Lambda(1405) resonance.

1 data table

Total cross sections.


Polarization in proton proton elastic scattering at 10, 14 and 17.5 gev/c

Borghini, M. ; Dick, L. ; Olivier, J.C. ; et al.
Phys.Lett.B 36 (1971) 501-503, 1971.
Inspire Record 69146 DOI 10.17182/hepdata.37233

Data on the polarization parameter in pp elastic scattering in the | t |-range from ∼0.1 to ∼ 2.9 (GeV/ c ) 2 and at 10, 14 and 17.5 GeV/ c are presented.

3 data tables

No description provided.

No description provided.

No description provided.


Structures and t Dependence of Two-Body Proton Diffraction Dissociation at 28.5-GeV/c

Cavalli-Sforza, M. ; Fermi, G. ; Goggi, G. ; et al.
Lett.Nuovo Cim. 18 (1977) 174-180, 1977.
Inspire Record 123855 DOI 10.17182/hepdata.37426

None

1 data table

T-DEPENDENCE OF TWO-BODY PROTON DIFFRACTION DISSOCIATION FOR VARIOUS MASS BINS. FOR IDENTIFICATION OF POSSIBLE <P PI0> AND <N PI+> RESONANCES, SEE THE PREVIOUS LETTER, R. R. APPLE ET AL., NCL 18, 167 (1977).


The Pion Electromagnetic Form-Factor in the Timelike Range 1.44-GeV**2-9.0-GeV**2

Bollini, D. ; Giusti, P. ; Massam, T. ; et al.
Lett.Nuovo Cim. 14 (1975) 418, 1975.
Inspire Record 100180 DOI 10.17182/hepdata.37445

None

1 data table

No description provided.


$\pi^+$ $\pi^-$ 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

RELATIVE PRODUCTION OF PION PAIRS WITHOUT RADIATIVE CORRECTIONS.


Search for rho Like Vector Mesons in the Mass Range 1.2-GeV to 3.0-GeV

Bollini, D. ; Giusti, P. ; Massam, T. ; et al.
Lett.Nuovo Cim. 15 (1976) 393, 1976.
Inspire Record 100567 DOI 10.17182/hepdata.37442

None

1 data table

No description provided.


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

No description provided.