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NA28 100 GeV data.
NA28 100 GeV data.
NA28 100 GeV data.
Structures of hadron-induced showers observed by the Pamir thick lead chambers are compared with simulations. The simulations are made for several models, VENUS, QGSJET, HDPM and the modified UA5 model, for hadron–nucleus interactions. A parameter Z , which is related to the inelasticity of hadron–Pb interactions, is defined and the Z -distribution of experimental data is compared with those of the simulations applying the same procedure of data processing to both sets of data. The Z -distribution for single-isolated hadrons is well reproduced by the models (VENUS, QGSJET and modified UA5) which give an average inelasticity 〈K h – Pb 〉=0.7 –0.8, whereas that for multi hadrons is close to the HDPM model which gives a smaller inelasticity of 〈K h – Pb 〉=0.5 –0.6. The difference of the characteristics between the two categories of hadron-induced showers is discussed.
Inelasticity of the first interaction, which defined by Kinel=1-Es/E0, where Es is the energy of the surviving particle and E0 is the incident hadron energy.
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IN 'YN' OF THIS TABLE 'A' MEANS CHEMICAL WEIGHT OF TANTALUM NUCLEUS.
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A search for stableH-dibaryon ofI=0,Y=0,JP=0+ was undertaken in negative pion-, neutron-,12C-nucleus- and proton-propane interactions at 4.0, 7.0, 50.4 and 10 GeV/c, respectively, using 55 cm and 2 m propane bubble chambers. This technique permite one to examine the whole range of possibleH-mass value. In the range ofMH>2MΛ=2231.2 MeV/c2 an enhancement ofMΛΛ=(2365.3±9.6) MeV/c2, ΓΛΛ=(47.2±15.1) MeV/c2 with production cross section σ=(24.2±7.0) μb per carbon nucleus was found. The mass rangeMΣ−p<MH<2MΛ was explored via the search for a weak decay modeH→Σ−+p. AV0-particle was found pointing to a two-prong interaction and satisfying the kinematics of the above two-body decay mode with a high confidence level. The possibility of imitation of the observed event by background processes was investigated for a series of two-step strong reactions and weak decays. We succeeded to show the significance of theH-production hypothesis on a deuteron-mass nuclear fluctuon via thepd→HpK+K0 reaction. The mass of the event treated as aH→Σ−+p weak decay appeared to be (2173.94±1.32) MeV/c2, its life-time being 0.668·10−10 s. Both are in agreement with predictions of the MIT Bag Model for the so-calledH-dihyperon. The formally determined production cross section of theH in proton-propane interactions at 10 GeV/c is estimated to be 40 nb. Perhaps, this event can be considered as a first evidence for a six-quark bound state-H-dihyperon. An independent way for the search for theH-particle, based on a specific conversion processHN→YYN, peculiar to its intranuclear strong interactions was proposed and tried. For this purpose all events with two Λ-hyperons and identified protons were tested for the hypothesesHp→ΛΛp at three fixed masses:MH=1880.00, 2173.94 MeV/c2 and the ΛΛ invariant mass for the event in question. The kinematics of this reaction fits successfully only one event and only atMH=2173.94 MeV/c2. It seems worthy of note that the final state ΛΛ invariant massMΛΛ=2344 MeV/c2 is rather close to the observed peak at 2365 MeV/c2. It is shown that the intranuclear conversion processes Ξ−p→ΛΛ and Ξ0n→ΛΛ fail to imitate the observed event. The ΛΛp invariant mass of this event equal to 3363 MeV/c2 is out of a 3568 MeV/c2 peak region of the ΛΛp invariant mass spectrum observed earlier. TheH conversion cross section exceeds the production one. Thus, we consider this event as providing a new evidence for the stableH-dibaryon ofMH=(2173.94±1.32) MeV/c2.
Claime of DIBARYON(S=-2) with mass M=(2365.3+-9.6) MeV and width G=(47.2+-15.1) MeV.
Forum