Sample records for mesoatoms

  1. Cosmic Rays and Clouds, 1. Formation of Lead Mesoatoms In Neutron Monitor By Soft Negative Muons and Expected Atmospheric Electric Field Effect In The Cosmic Ray Neutron Component (United States)

    Dorman, L. I.; Dorman, I. V.

    We extend our model (Dorman and Dorman, 1995) of cosmic ray atmospheric electric field effect on the case of neutron monitor. We take into account that about 0.07 of neu- tron monitor counting rate caused by negative soft muons captured by lead nucleons and formed mesoatoms with generation of several MeV energy neutrons from lead. In this case the neutron monitor or neutron supermonitor works as analyzer which de- tects muons of only one, negative sign. It is very important because the atmospheric electric field effect have opposite signs for positive and negative muons that main part of this effect in the muon telescope or in ionization chamber is compensated and we can observe only small part of total effect of one sign muons. On the basis of our gen- eral theory of cosmic ray meteorological effects with taking into account of negative soft muon acceleration and deceleration in the Earth atmosphere (in dependence of di- rection and intensity of electric field) we discuss the possibility of existing this effect in cosmic ray neutron component and made some rough estimations. REFERENCES: Dorman L.I. and Dorman I.V., 1995. "Cosmic-ray atmospheric electric field effects". Canadian J. of Physics, Vol. 73, pp. 440-443.

  2. Fission probability of nucleus of sup(232)Th mesoatom

    International Nuclear Information System (INIS)

    Cojocaru, V.; Gavrilov, Yu.K.; Kim Si wan; Krogulski, T.; Kuznetsov, V.D.; Ortlepp, H.-G.; Polikanov, S.M.


    The fission probability of the nucleus of the sup(232)Th muonic atom has been measured. The fission yield was measured simultaneously with the intensity of 5g-4f transition in the muonic atom sup(232)Th. A good agreement with previous result obtained in measurements with the fission chamber and evident disagreement with the photoemulsion data have been obtained

  3. Kinetics of muon catalysis processes in a deuterium-tritium mixture

    International Nuclear Information System (INIS)

    Men'shikov, L.I.; Fajfman, M.P.; Somov, L.N.


    A quasistationary mode of muon catalysis in a D 2 +T 2 mixture, established in the time region t >> λ eff -1 (λ eff -1 is the lifetime of the mesomolecule dtμ). Energy distribution functions are calculated for tμ atoms in the 1s state. The calculated spectrum of tμ mesoatoms differs from the Maxwell distribution by no more than 10 per cent. Difference between the values of the resonance dtμ production rate averaged by the calculated and Maxwell functions is 5%

  4. Explanation od sudden temperature dependence of muon catalysis in solid deuterium

    CERN Document Server

    Gershtejn, S S


    It is indicated, that the elastic scattering of the d mu-meson atoms in the solid deuterium at sufficiently low temperatures (as well as of slow neutrons) occurs on the whole crystalline lattice practically without energy loss, and the inelastic collision with the phonon excitation is low.Therefore, the resonance formation of the dd mu-molecules in the solid deuterium takes place before the d mu mesoatoms thermalization and it explains practically observed independence of the dd mu-molecules formation rate and muon catalysis of the temperatures

  5. Monopole excitation of nucleus in the bound muon decay

    International Nuclear Information System (INIS)

    Sabirov, B.M.; Abazov, V.M.; Kutuzov, S.A.


    The work is aimed at theoretical and experimental investigation into the possibility of nucleus excitation under the muon decay on mesic atom K-shell. The process of mesic atom formation is briefly considered. The stage of muon presence in the mesic atom orbit is completed by mesoatomic cascade, muon decay or muon nuclear capture. Recording of electron coincidences from decay of muon with nuclear transition γ-quanta makes up the base of experiment on the search for the nucleus excitation under the bound muon decay. Muon 158 Sm atom is considered in detail. The experimental data obtained allow one to ascertain the upper limit of probability of the first 152 SmO + level excitation under the bound muon decay W -3