High precision measurement of the associated strangeness production in proton proton interactions

The COSY-TOF collaboration Jowzaee, S. ; Borodina, E. ; Clement, H. ; et al.
Eur.Phys.J.A 52 (2016) 7, 2016.
Inspire Record 1393330 DOI 10.17182/hepdata.70735

A new high precision measurement of the reaction pp -> pK+Lambda at a beam momentum of 2.95 GeV/c with more than 200,000 analyzed events allows a detailed analysis of differential observables and their inter-dependencies. Correlations of the angular distributions with momenta are examined. The invariant mass distributions are compared for different regions in the Dalitz plots. The cusp structure at the N Sigma threshold is described with the Flatt\'e formalism and its variation in the Dalitz plot is analyzed.

9 data tables

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Single-Pion Production in pp Collisions at 0.95 GeV/c (II)

The COSY-TOF collaboration Abd El-Samad, S. ; Bilger, R. ; Brinkmann, K.-Th. ; et al.
Eur.Phys.J.A 39 (2009) 281-289, 2009.
Inspire Record 790164 DOI 10.17182/hepdata.50496

The single-pion production reactions $pp\to d\pi^+$, $pp\to np\pi^+$ and $pp\to pp\pi^0$ were measured at a beam momentum of 0.95 GeV/c ($T_p \approx$ 400 MeV) using the short version of the COSY-TOF spectrometer. The central calorimeter provided particle identification, energy determination and neutron detection in addition to time-of-flight and angle measurements from other detector parts. Thus all pion production channels were recorded with 1-4 overconstraints. Main emphasis is put on the presentation and discussion of the $np\pi^+$ channel, since the results on the other channels have already been published previously. The total and differential cross sections obtained are compared to theoretical calculations. In contrast to the $pp\pi^0$ channel we find in the $np\pi^+$ channel a strong influence of the $\Delta$ excitation already at this energy close to threshold. In particular we find a $(3 cos^2\Theta + 1)$ dependence in the pion angular distribution, typical for a pure s-channel $\Delta$ excitation and identical to that observed in the $d\pi^+$ channel. Since the latter is understood by a s-channel resonance in the $^1D_2$ $pn$ partial wave, we discuss an analogous scenario for the $pn\pi^+$ channel.

6 data tables

Differential cross section for the process P P --> P N PI+ as a function ofthe P PI+ mass.

Differential cross section for the process P P --> P N PI+ as a function ofthe N PI+ mass.

Differential cross section for the process P P --> P N PI+ as a function ofthe P N mass.

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Observation of inverse diproton photodisintegration at intermediate energies

Komarov, V. ; Azaryan, T. ; Chiladze, D. ; et al.
Phys.Rev.Lett. 101 (2008) 102501, 2008.
Inspire Record 787271 DOI 10.17182/hepdata.50532

The reaction pp->{pp}_s\gamma, where {pp}_s is a proton pair with an excitation energy E_{pp}<3 MeV, has been observed with the ANKE spectrometer at COSY-Juelich for proton beam energies of T_p=0.353, 0.500, and 0.550 GeV. This is equivalent to photodisintegration of a free 1S_0 diproton for photon energies E\gamma ~ T_p/2. The differential cross sections measured for c.m. angles 0 deg.<\theta_{pp}<20 deg. exhibit a steep increase with angle that is compatible with E1 and E2 multipole contributions. The ratio of the measured cross sections to those of np->d\gamma is on the 10^{-3}-10^{-2} level. The increase of the pp->{pp}_s\gamma cross section with T_p might reflect the influence of the Delta(1232) excitation.

3 data tables

Differential cross section in the centre of mass system for individual protons of kinetic energy 0.353 GeV. Errors shown are statistics plus uncertainties in background estimation.

Differential cross section in the centre of mass system for individual protons of kinetic energy 0.500 GeV. Errors shown are statistics plus uncertainties in background estimation.

Differential cross section in the centre of mass system for individual protons of kinetic energy 0.550 GeV. Errors shown are statistics plus uncertainties in background estimation.


Comparison of Isoscalar Vector Meson Production Cross Sections in Proton-Proton Collisions

The COSY-TOF collaboration Abdel-Bary, M. ; Abdel-Samad, S. ; Brinkmann, K.-Th. ; et al.
Phys.Lett.B 647 (2007) 351-357, 2007.
Inspire Record 745517 DOI 10.17182/hepdata.31471

The reaction $ pp\to pp\bf \omega$ was investigated with the TOF spectrometer, which is an external experiment at the accelerator COSY (Forschungszentrum Julich, Germany). Total as well as differential cross sections were determined at an excess energy of $93 MeV$ ($p_{beam}=2950 MeV/c$). Using the total cross section of $(9.0\pm 0.7 \pm1.1) \mu b$ for the reaction $ pp\to pp\omega$ determined here and existing data for the reaction $pp\to pp\bf \phi$, the ratio $\mathcal{R}_{\phi/\omega}=\sigma_\phi/\sigma_\omega$ turns out to be significantly larger than expected by the Okubo-Zweig-Iizuka (OZI) rule. The uncertainty of this ratio is considerably smaller than in previous determinations. The differential distributions show that the $\omega$ production is still dominated by S-wave production at this excess energy, however higher partial waves clearly contribute. A comparison of the measured angular distributions for $\omega$ production to published distributions for $\phi$ production at $83 MeV$ shows that the data are consistent with an identical production mechanism for both vector mesons.

5 data tables

Total cross section after acceptance correction and normalization.

Differential cross section as a function of the cosine of the polar angle of the protons in the overall c.m. system.

Differential cross section as a function of the omega meson angle in the overall c.m. system.

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Anisotropy in the pion angular distribution of the reaction pp -> pp pi0 at 400 MeV

Thorngren Engblom, P. ; Negasi Keleta, S. ; Cappellaro, F. ; et al.
Phys.Rev.C 76 (2007) 011602, 2007.
Inspire Record 725409 DOI 10.17182/hepdata.31500

The reaction pp -> pp pi0 was studied with the WASA detector at the CELSIUS storage ring. The center of mass angular distribution of the pi0 was obtained by detection of the gamma decay products together with the two outgoing protons, and found to be anisotropic with a negative second derivative slope, in agreement with the theoretical predictions from a microscopic calculation.

2 data tables

Acceptance corrected centre of mass PI0 angular distribution, normalized to 92.3 +- 7.2 MUB (Bilger et al.).

Acceptance corrected centre of mass PI0 angular distribution for relative proton momenta < 53 MeV, normalized to Bilger et al... Statistical errors only.


Single-pion production in p p collisions at 0.95-GeV/c. I.

The COSY-TOF collaboration El-Samad, S.Abd ; Bilger, R. ; Brinkmann, K. -Th. ; et al.
Eur.Phys.J.A 30 (2006) 443-453, 2006.
Inspire Record 725793 DOI 10.17182/hepdata.43429

The single-pion production reactions $pp\to d\pi^+$, $pp\to np\pi^+$ and $pp\to pp\pi^0$ were measured at a beam momentum of 0.95 GeV/c ($T_p \approx$ 400 MeV) using the short version of the COSY-TOF spectrometer. The implementation of a central calorimeter provided particle identification, energy determination and neutron detection in addition to time-of-flight and angle measurements. Thus all pion production channels were recorded with 1-4 overconstraints. The total and differential cross sections obtained are compared to previous data and theoretical calculations. Main emphasis is put on the discussion of the $pp\pi^0$ channel, where we obtain angular distributions different from previous experimental results, however, partly in good agreement with recent phenomenological and theoretical predictions. In particular we observe very large anisotropies for the $\pi^0$ angular distributions in the kinematical region of small relative proton momenta revealing there a dominance of proton spinflip transitions associated with $\pi^0$ $s$- and $d$-partial waves and emphasizing the important role of $\pi^0$ d-waves.

8 data tables

Total cross section measurements.. Errors are mainly systematic.

Measured angular distribution for elastic P P scattering in the CM system normalised to the data in the SAID database (Arndt et al. PR C62,034005(2000). This measurement is made to determine the luminosity.

The measured pion angular distribution in the CM system in the reaction P P --> DEUT PI+.

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Total and differential cross sections for the p p --> p p eta' reaction near threshold.

Khoukaz, A. ; Geck, I. ; Quentmeier, C. ; et al.
Eur.Phys.J.A 20 (2004) 345-350, 2004.
Inspire Record 642580 DOI 10.17182/hepdata.43699

The eta-prime meson production in the reaction pp-->pp eta-prime has been studied at excess energies of Q = 26.5, 32.5 and 46.6 MeV using the internal beam facility COSY-11 at the cooler synchrotron COSY. The total cross sections as well as one angular distribution for the highest Q-value are presented. The excitation function of the near threshold data can be described by a pure s-wave phase space distribution with the inclusion of the proton-proton final state interaction and Coulomb effects. The obtained angular distribution of the eta-prime mesons is also consistent with pure s-wave production.

2 data tables

Total cross section for the reaction P P --> P P ETAPRIME.

Angular distribution of the ETAPRIME in the CM system at an excess energy of 46.6 MeV. There is an additional systematic error of +24%/-35%.


a0(980)+ resonance production in p p --> d K+ anti-K0 reactions close to threshold.

Kleber, V. ; Buescher, Markus ; Chernyshev, V. ; et al.
Phys.Rev.Lett. 91 (2003) 172304, 2003.
Inspire Record 617741 DOI 10.17182/hepdata.31682

The reaction pp->d K+ Kbar0 has been investigated at an excess energy of Q=46 MeV above the (K+ Kbar0) threshold with ANKE at COSY-Juelich. From the detected coincident dK+ pairs about 1000 events with a missing Kbar0 were identified, corresponding to a total cross section of sigma(pp->d K+ Kbar0)=(38 +/- 2(stat) +/- 14(syst)) nb. Invariant-mass and angular distributions have been jointly analyzed and reveal s-wave dominance between the two kaons, accompanied by a p-wave between the deuteron and the kaon system. This is interpreted in terms of a0+(980)-resonance production.

6 data tables

Total cross section for P P --> DEUT K+ KBAR0.

Centre of mass angular distribution of the deuteron with respect to the direction of the incoming proton.

Centre of mass angular distribution of the vector joining the K+ and KBAR0 with respect to the direction of the incoming proton.

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Analysing power A(y) in the reaction p(pol.) p --> p p eta close to threshold.

Winter, P. ; Adam, H.H. ; Bauer, F. ; et al.
Phys.Lett.B 544 (2002) 251-258, 2002.
Inspire Record 599591 DOI 10.17182/hepdata.31686

Measurements of the eta meson production with a polarised proton beam in the reaction p(pol) p --> p p eta have been carried out at an excess energy of Q = 40 MeV. The dependence of the analysing power A_y on the polar angle theta^*_q of the eta meson in the center of mass system (CMS) has been studied. The data indicate the possibility of an influence of p- and d-waves to the close to threshold eta production.

1 data table

Averaged value of the analyzing power and cross section as a function of the emmission angle of the ETA meson is the CM system.


Measurement of the eta production in proton proton collisions with the COSY time of flight spectrometer.

The COSY-TOF collaboration Abdel-Bary, M. ; Abdel-Samad, S. ; Bilger, R. ; et al.
Eur.Phys.J.A 16 (2003) 127-137, 2003.
Inspire Record 587236 DOI 10.17182/hepdata.43626

The reaction pp -> pp eta was measured at excess energies of 15 and 41 MeV at an external target of the Juelich Cooler Synchrotron COSY with the Time of Flight Spectrometer. About 25000 events were measured for the excess energy of 15 MeV and about 8000 for 41 MeV. Both protons of the process pp eta were detected with an acceptance of nearly 100% and the eta was reconstructed by the missing mass technique. For both excess energies the angular distributions are found to be nearly isotropic. In the invariant mass distributions strong deviations from the pure phase space distributions are seen.

6 data tables

Angular distribution of the ETA in the CM frame.

Angular distribution of the P P momentum in the CM frame.

Squared P P invariant mass distribution.

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