HEPData Search

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K*0 and phi Meson Production in Proton-Nucleus Interactions at sqrt(s) = 41.6 GeV

The HERA-B collaboration Abt, I. ; Adams, M. ; Agari, M. ; et al.

Eur.Phys.J.C 50 (2007) 315-328, 2007.

Inspire Record 719788 DOI 10.17182/hepdata.43089

The inclusive production cross sections of the strange vector mesons K*0, K*0bar, and phi have been measured in interactions of 920 GeV protons with C, Ti, and W targets with the HERA-B detector at the HERA storage ring. Differential cross sections as a function of rapidity and transverse momentum have been measured in the central rapidity region and for transverse momenta up to pT=3.5 GeV/c. The atomic number dependence is parametrised as sigma(pA) = sigma(pN)*A**alpha, where sigma(pN) is the proton-nucleon cross section. Within the phase space accessible, alpha(K*0) = 0.86+/-0.03, alpha(K*0bar) = 0.87+/-0.03, and alpha(phi) = 0.96+/-0.02. The total proton-nucleon cross sections, determined by extrapolating the differential measurements to full phase space, are sigma(pN->K*0) = 5.06+/-0.54 mb, sigma(pN->K*0bar) = 4.02+/-0.45 mb, and sigma(pN->phi) = 1.17+/-0.11 mb. The Cronin effect is observed for the first time for vector mesons containing strange quarks/ compared to the measurements of Cronin et al. for K+- mesons, the measured values of alpha for phi mesons coincide with those of K- mesons for all transverse momenta, while the enhancement for K*0 / K*0bar mesons is smaller.

13 data tables

Table 1

Measured rapidity distribution for K*0 production in the accessible phase space.

Table 2

Measured rapidity distribution for K*BAR0 production in the accessible phase space.

Table 3

Measured rapidity distribution for PHI production in the accessible phase space.

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A measurement of K*+- production in the hyperon beam experiment at CERN

The WA89 collaboration Adamovich, M.I. ; Aleksandrov, Yu.A. ; Baranov, S.P. ; et al.

Eur.Phys.J.C 22 (2001) 47-54, 2001.

Inspire Record 569120 DOI 10.17182/hepdata.43223

We report on a measurement of the differential cross sections of inclusive$K^{\pm}_{890}$production in$\sigma^-, pi^-$and ne

8 data tables

Table 1

The production cross sections for K*+- per nucleus and per nucleon for the SIGMA- beam.

Table 2

The production cross sections for K*+- per nucleus and per nucleon for the PI- beam.

Table 3

The production cross sections for K*+- per nucleus and per nucleon for the NEUTRON- beam.

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Threshold structure of the quasifree p + n --> d + eta reaction.

Calen, H. ; Dyring, J. ; Fransson, K. ; et al.

Phys.Rev.Lett. 80 (1998) 2069-2072, 1998.

Inspire Record 468434 DOI 10.17182/hepdata.19524

The quasifree p+n→d+η reaction cross section has been measured at the threshold using 1295 MeV protons in the CELSIUS storage ring and an internal cluster-jet deuterium target. The kinematics is chosen such that the target proton can be assumed to be a spectator. The Fermi momentum of the target neutron is used to extract the energy dependence of the cross section by reconstructing the kinematics on an event-by-event basis. The data cover excess energies from threshold to 10 MeV in the center of mass of the final dη system. Approaching the threshold the cross section is enhanced compared to what is expected from phase space. This behavior is typical for a strong final-state interaction.

1 data table

Table 1

Cross section as a function of the C.M. excess energy.

Forward cross-sections for production of D+, D0, D/s, D*+ and Lambda/c in 250-GeV pi+-, K+-, and p nucleon interactions.

The E769 collaboration Alves, G.A. ; Amato, S. ; Anjos, J.C. ; et al.

Phys.Rev.Lett. 77 (1996) 2388-2391, 1996.

Inspire Record 418771 DOI 10.17182/hepdata.42294

We measure forward cross sections for production of D+, D0, Ds, D*+, and Λc in collisions of π±, K±, and p on a nuclear target. Production induced by different beam particles is found to be the same within statistics. Strange and baryonic final states are seen to contribute appreciably to the total charm cross section, which our measurements indicate is larger than but consistent with QCD predictions. The energy dependence mapped out by these and previous measurements is consistent with theory. Leading-particle asymmetry measurements for K and p-induced charm production are also presented.

8 data tables

Table 1

No description provided.

Table 2

No description provided.

Table 3

No description provided.

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Beam flavor dependence in the hadroproduction of D+- and D(s)+- mesons

The E769 collaboration Wallace, A. ; Alves, G.A. ; Amato, S. ; et al.

FERMILAB-CONF-94-184-E, 1994.

Inspire Record 375038 DOI 10.17182/hepdata.43049

None

10 data tables

Table 1

No description provided.

Table 2

No description provided.

Table 3

No description provided.

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Search for prompt muon neutrinos in 70-GeV proton interactions with iron nuclei

Bozhko, N.I. ; Borisov, A.A. ; Bugorsky, A.P. ; et al.

IFVE-92-110, 1992.

Inspire Record 340114 DOI 10.17182/hepdata.40668

None

1 data table

Table 1

The cross section per nucleon is evaluated with assumption of the linear atomic number dependence. SIG(C=NEUTRINO) and SIG(C=ANTINEUTRINO) are corresponded to the NUMU and NUMUBAR data, respectevly. CLOOP-OVER.

Production of $J / \psi$ via $\psi^{\prime}$ and $X$ Decay in 300-GeV/c Proton and $\pi^{\pm}$ Nucleon Interactions

The E705 collaboration Antoniazzi, L. ; Arenton, M. ; Cao, Z. ; et al.

Phys.Rev.Lett. 70 (1993) 383-386, 1993.

Inspire Record 336204 DOI 10.17182/hepdata.19754

The production of the χ1 and χ2 states of charmonium has been observed in 300 GeV/c π±N and pN interactions. The fraction of the total inclusive J/ψ production due to radiative χ decay has been determined to be 0.40±0.04, 0.37±0.03, and 0.30±0.04 for the π+, π−, and proton data, respectively. Total cross sections have been obtained of 131±18±14 and 188±30±21 nb/nucleon in the 300 GeV/c π−N interactions for χ1 and χ2 production. By measuring the contributions to the J/ψ production due to both ψ’ and radiative χ decay, the cross sections for direct J/ψ production have been determined to be 97±14, 102±14, and 89±12 nb/nucleon for π+, π−, and protons, respectively.

8 data tables

Table 1

Fractions of total J/PSI production due to radiative CHI1 and CHI2 decays.

Table 2

Fractions of total J/PSI production due to radiative CHI1 and CHI2 decays.

Table 3

Fractions of total J/PSI production due to radiative CHI1 and CHI2 decays.