The study of the J ψ transverse momentum distribution in oxygen-uranium reactions at 200 GeV/nucleon shows that 〈 P T 〉 and 〈 P T 2 〉 increase with the transverse energy of the reaction. Muon pairs in the mass continuum do not exhibit the same behaviour. The comparison of the J ψ production rates in central and peripheral collisions shows a significant diminution for low P T central events.
Two parametrization of the D(SIG)/D(PT) are used: first is : PT*exp(-SLOPE*PT**CONST(C=PT)) and second is : PT*exp(-2*MT/CONST(C=MT)).
D(SIG)/D(PT) is parameterized as PT*exp(-SLOPE*PT**CONST).
D(SIG)/D(PT) is parameterized as PT*exp(-SLOPE*PT**CONST).
A single-spin asymmetry in the inclusive π 0 production at small x F was measured. In the experiment 40 GeV/c π − mesons were incident on transversely polarized protons and deutrons. An asymmetry of (40–50)% has been revealed in the hard scattering region.
No description provided.
The C12(28Si,X)11C cross section was measured for 13.4-GeV/nucleon Si28 ions. Beam intensities were determined with a two-element counter telescope, and the C11 activity induced in thin and thick plastic scintillator targets was assayed by internal scintillation counting. The cross section corrected to zero target thickness is 73.5±3.5 mb. This value is compared with similar measurements for relativistic projectiles at 1–2 GeV/nucleon.
No description provided.
Results are presented for the charge-symmetry superratio R, simple ratios r1 and r2, and the differential cross sections of π+ and π− elastic scattering on H3 and He3: R=r1r2, r1=σ(θ)[π+ π+3 ]3/σ(θ)[π− π−3 ]3, and r2=σ(θ)[π− π−3 ]3/σ(θ)[π+ He3 →π+ ]3. The measurements were made at Tπ=180 MeV and θπ(lab)=40°–90°; some data were obtained at Tπ=143 MeV also. At all angles, R>1 and r2>1 indicative of a violation of charge symmetry; however, we also find that r1≃1. Our data are consistent with Fp(3H)≃Fn(3He) and Fn(3H)>Fp(3He), where Fp and Fn are the proton and neutron matter form factors. σ(θ)[π± π±3 ]3 decreases with increasing magnitude of the four-momentum transfer t up to θc.m.≃70°; the t dependence of the F ’s is comparable to that of the electromagnetic form factors. σ(θ)[π− π−33H] has a non-spin-flip dip at θc.m.≃78°.
No description provided.
No description provided.
No description provided.
We have made the first systematic precision measurement of the deuteron-deuteron total cross sections at 12 incident momenta in the range of 1.5–4.0 GeV/c on a proton synchrotron. The data were obtained by means of the transmission method covering the momentum transfer squared range of 0.001 to 0.009 (GeV/c)2 at each momentum. Our data show no anomalous structure in the excitation function and are in good agreement with Glauber model calculations including the effect of the Fermi motion of the nucleons in the deuteron except at 1.5 GeV/c, where the datum is lower than the calculated value.
Errors contain both statistics and systematics.
An analysis has been performed of neutrino and antineutrino interactions with protons and neutrons in a deuterium bubble chamber. The interactions under study are quasielastic neutrino-neutron scattering and one-, two- and three-pion production reactions. Results are presented on cross sections, effective mass distributions, resonance production, momentum transfer distributions and coefficients of the decay angular distributions. Where possible, comparisons are made with existing theoretical models and predictions.
No description provided.
Numerical values supplied by A.Tenner.
Numerical values supplied by A.Tenner.
We present data on inclusive (e,p) scattering for electron beam energies of 460, 505, 647, 686, 698, and 800 MeV. Proton momentum spectra were obtained at fixed proton angles and for momenta from 300–1000 MeV/c. The data are compared to a popular parametrization that includes quasifree knockout, a quasideuteron mechanism, and pion production through the Δ.
No description provided.
No description provided.
No description provided.
The pion induced pion production (π, 2π) reaction on deuterium has been studied at an incident pion energy of 280 MeV. The outgoing pions were detected in coincidence and the measured four-fold cross sections were compared with a πN → ππ N microscopic model, and, upon integration, with the available experimental total cross sections from the same reaction on H and 2 H. Finally, the results were directly compared with recent data from the 16 O(π + , π + π − ) reaction at the same incident energy.
No description provided.
This work represents the results of an experimental investigation of the electromagnetic dissociation of 200 GeV/nucleon 16 O and 32 S ions in nuclear emulsions. Exclusive channels involving charged fragments have been studied as a function of the energy released, and, assuming a Weizsäcker-Williams spectrum of virtual photons, there is a good agreement with results for the (γ, p) processes obtained with real photons. However, the rates found for other processes are larger, in particular for the (γ, α) on both nuclei. The values of the total integrated absorption cross sections are generally larger than those obtained from real photon experiments but the extent of the discrepancy depends strongly upon which photon results are used in the comparison.
ELECTROMAGNETIC DISSOCIATION IN NUCLEAR EMULSION.
ELECTROMAGNETIC DISSOCIATION IN NUCLEAR EMULSION.
NUCLEUS IS THE EMULSION.
The basic characteristics of the quasi-elastic charge exchange reaction p 3 He→ n F ppp are investigated using the 80 cm ITEP liquid-hydrogen bubble chamber, which is exposed to beams of 3 He nuclei with momenta of 2.5 and 5 GeV/ c (the kinetic energy of primary protons in the rest system of the nucleus are, respectively, T p = 0.318 and 0.978 GeV). The experimental data are compared with the predictions of the Glauber-Sitenko multiple scattering theory and of the pole model, taking into account the interaction between spectator nucleons in the final state. In the mass spectrum of the 3p system at 3.05 GeV a clearly denned structure has been revealed, which is not described within the pole model. A possible resonance origin of the given structure is discussed.
No description provided.
THE EVENTS WITH THE FASTEST NEUTRON: P(P=3),P(P=4),P(P=5),P(P=6).
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