Zalikhanov, B.Zh.
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The Investigation of the $\pi^- p \to \pi^0 \pi^0 n$ Reaction Near the Threshold

Belkov, A.A. ; Bunyatov, S.A. ; Zalikhanov, B.Zh. ; et al.
Sov.J.Nucl.Phys. 31 (1980) 96, 1980.
Inspire Record 142916 DOI 10.17182/hepdata.18169

None

2 data tables
Table 1

FIRST VARIANT OF INSTALLATION.

Table 2

SECOND VARIANT OF INSTALLATION.


Determination of form-factor parameters lambda+ and lambda0 in K(mu3) decay.

Artemov, V.M. ; Volkov, A.D. ; Emelyanenko, G.A. ; et al.
Phys.Atom.Nucl. 60 (1997) 218-223, 1997.
Inspire Record 404831 DOI 10.17182/hepdata.38592

None

1 data table
Table 1

Formfactors F+ and F0 are parameterized as usual F+(0) = F(0)*(1 + CONST*(T/M(PI)**2)).


Forward K+ production in subthreshold p A collisions at 1.0-GeV.

The ANKE collaboration Koptev, V. ; Buescher, Markus ; Junghans, H. ; et al.
Phys.Rev.Lett. 87 (2001) 022301, 2001.
Inspire Record 556676 DOI 10.17182/hepdata.31765

K+ meson production in pA (A = C, Cu, Au) collisions has been studied using the ANKE spectrometer at an internal target position of the COSY-Juelich accelerator. The complete momentum spectrum of kaons emitted at forward angles, theta < 12 degrees, has been measured for a beam energy of T(p)=1.0 GeV, far below the free NN threshold of 1.58 GeV. The spectrum does not follow a thermal distribution at low kaon momenta and the larger momenta reflect a high degree of collectivity in the target nucleus.

3 data tables
Table 1

Double differential K+ production cross section for forward K+ angles < 12 degs. Statistical errors only.

Table 2

The invariant cross section for K+ production. Statistical errors only.

Table 3

Ratio of K+ production cross sections for CU/C and AU/C.


Proton induced deuteron breakup at GeV energies with forward emission of a fast proton pair.

Komarov, V. ; Dymov, S. ; Kacharava, A. ; et al.
Phys.Lett.B 553 (2003) 179-185, 2003.
Inspire Record 599592 DOI 10.17182/hepdata.31711

A study of the deuteron breakup reaction $pd \to (pp)n$ with forward emission of a fast proton pair with small excitation energy $E_{pp}<$ 3 MeV has been performed at the ANKE spectrometer at COSY--J\ulich. An exclusive measurement was carried out at six proton--beam energies $T_p=$~0.6,~0.7,~0.8,~0.95,~1.35, and 1.9 GeV by reconstructing the momenta of the two protons. The differential cross section of the breakup reaction, averaged up to $8^{\circ}$ over the cm polar angle of the total momentum of the $pp$ pairs, has been obtained. Since the kinematics of this process is quite similar to that of backward elastic $pd \to dp$ scattering, the results are compared to calculations based on a theoretical model previously applied to the $pd \to dp$ process.

1 data table
Table 1

The measured cross section of the process P DEUT --> P P N in the interval E(PP) < 3 MeV versus the proton beam energy.


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
Table 1

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

Table 2

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

Table 3

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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Near-threshold production of omega mesons in the p n --> d omega reaction.

Barsov, S. ; Lehmann, I. ; Schleichert, R. ; et al.
Eur.Phys.J.A 21 (2004) 521-527, 2004.
Inspire Record 619755 DOI 10.17182/hepdata.43593

The first measurement of the p n -> d omega total cross section has been achieved at mean excess energies of Q = 28 and 57 MeV by using a deuterium cluster-jet target. The momentum of the fast deuteron was measured in the ANKE spectrometer at COSY-Juelich and that of the slow spectator proton p(sp) from the p d -> p(sp) d omega reaction in a silicon telescope placed close to the target. The cross sections lie above those measured for p p -> p p omega but seem to be below theoretical predictions.

1 data table
Table 1

Total cross sections after the P N --> DEUT OMEGA reaction just above threshold.


Observation of an ABC effect in proton-proton collisions

Dymov, S. ; Hartmann, M. ; Kacharava, A. ; et al.
Phys.Rev.Lett. 102 (2009) 192301, 2009.
Inspire Record 812534 DOI 10.17182/hepdata.51593

The cross section for inclusive multipion production in the pp->ppX reaction was measured at COSY-ANKE at four beam energies, 0.8, 1.1, 1.4, and 2.0 GeV, for low excitation energy in the final pp system, such that the diproton quasi-particle is in the 1S0 state. At the three higher energies the missing mass Mx spectra show a strong enhancement at low Mx, corresponding to an ABC effect that moves steadily to larger values as the energy is increased. Despite the missing-mass structure looking very different at 0.8 GeV, the variation with Mx and beam energy are consistent with two-pion production being mediated through the excitation of two Delta(1232) isobars, coupled to S-- and D-- states of the initial pp system.

4 data tables
Table 1

The P P --> P P X differential cross section as a function of the square ofthe missing mass (X) at incident beam energy of 0.8 GeV.

Table 2

The P P --> P P X differential cross section as a function of the square ofthe missing mass (X) at incident beam energy of 1.1 GeV.

Table 3

The P P --> P P X differential cross section as a function of the square ofthe missing mass (X) at incident beam energy of 1.4 GeV.

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