A. Halsteinslid
University of Bergen
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Physics Letters B | 1984
D. Allasia; C. Angelini; A. Baldini; S. Barlag; L. Bertanza; A. Bigi; V. Bisi; F. Bobisut; T. Bolognese; A. Borg; E. Calimani; P. Capiluppi; R. Casali; S. Ciampolillo; J. Derkaoui; M. L. Faccini-Turluer; R. Fantechi; V. Flaminio; A. G. Frodesen; D. Gamba; G. Giacomelli; G. Graziani; A. Halsteinslid; A. Hornaes; H. Huzita; B. Jongejans; I. Lippi; M. Loreti; C. Louedec; G. Mandrioli
Abstract Data from an exposure of the BEBC bubble chamber filled with deuterium to neutrino and antineutrino wide band beams have been used to extract the x dependence of the structure functions for scattering on protons and neutrons and the fractional momentum distributions of the valence quarks and the antiquarks of different flavours. The difference F n 2 − F p 2 is compared with recent data from high energy μD scattering. A result is also obtained on the sum rule giving the difference between the number of up and down quarks in the nucleon.
Nuclear Physics | 1979
N. Armenise; O. Erriquez; M.T. Fogli Muciaccia; S. Nuzzo; F. Ruggieri; A. Halsteinslid; K. Myklebost; A. Rognebakke; O. Skjeggestad; S. Bonetti; Donatella Cavalli; M.C. Pernigoni; A. Pullia; M. Rollier; J.P. Engel; B. Escoubes; J.L. Guyonnet; D. Huss; J.L. Riester; M. Schaeffer; D. Allasia; V. Bisi; D. Gamba; A. Marzari Chiesa; L. Riccati; A. Romero; F.W. Bullock; R.C.W. Henderson; T. W. Jones; F. Ramzan
Abstract A sample of 766 antineutrino charged current elastic events has been used to extract the variation of the elastic cross section with antineutrino energy and the distribution of d N /d q 2 . The best fit value for the parameter M A obtained from these measurements is M A = 0.91 ± 0.04 GeV/ c 2 for M V = 0.84 GeV/ c 2 . A simultaneous determination of M A and M V gives M A = 0.94 ± 0.07, M V = 0.81
Physics Letters B | 1987
F. Balestra; M.P. Bussa; L. Busso; L. Fava; L. Ferrero; D. Panzieri; G. Piragino; F. Tosello; G. Bendiscioli; A. Rotondi; P. Salvini; A. Zenoni; Yu. A. Batusov; I. V. Falomkin; G. B. Pontecorvo; M.G. Sapozhnikow; V.I. Tretyak; C. Guaraldo; A. Maggiora; E. Lodi Rizzini; A. Haatuft; A. Halsteinslid; K. Myklebost; J.M. Olsen; F.O. Breivik; T. Jacobsen; S.O. Sørensen
Abstract The Λ 0 and K 0 s production cross sections have been measured at 607 MeV/ c for the reaction p + 20 Ne → V 0 + X ( V 0 =Λ, 0 , K 0 s ) . The Λ 0 /K 0 s production ratio is found to be (2.3±0.7). The data are consistent with an evaporative character of the emission mechanism from a multinucleon system for Λ 0 and from one nucleon for K 0 s . The rapidity distributions of negative tracks in K 0 x events are different from those in Λ 0 events without V 0 .
Physics Letters B | 1989
F. Balestra; Riccardo Barbieri; Yu. A. Batusov; G. Bendiscioli; S. Bossolasco; F.O. Breivik; M.P. Bussa; L. Busso; C. Guaraldo; I. V. Falomkin; L. Ferrero; V. Filiipini; A. Haatuft; A. Halsteinslid; Torben K. Jacobsen; E. Lodi Rizzini; A. Maggiora; M. Masala; K. Myklebost; J.M. Olsen; D. Panzieri; G. Piragino; G. B. Pontecorvo; A. Rotondi; A.M. Rozhdestvensky; P. Salvini; M.G. Sapozhnikov; S.O. Sørensen; F. Tosello; V.I. Tretyak
Abstract The p ¯ 4 He annihilation cross section averaged over the interval 40–50 MeV/c has been measured using a streamer chamber in a magnetic field. The measured value is 1342±250 mb. It agrees with a behaviour like 1/p of the annihilation cross section. Our result has been obtained at the lowest momentum achieved till now in measurements of antiproton annihilation in flight.
Nuclear Physics | 1991
F. Balestra; Yu. A. Batusov; G. Bendiscioli; S. Bossolasco; F.O. Breivik; M.P. Bussa; L. Busso; K M Danielsen; C. Guaraldo; I. V. Falomkin; L. Fava; L. Ferrero; V. Filippini; A. Haatuft; A. Halsteinslid; T. Jacobsen; E. Lodi Rizzini; A. Maggiora; K. Myklebost; J.M. Olsen; D. Panzieri; G. Piragino; G. B. Pontecorvo; A. Rotondi; A.M. Rozhdestvensky; P. Salvini; M.G. Sapozhnikov; S.O. Sørensen; F. Tosello; V.I. Tretyak
Abstract New data are reported on antiproton annihilations at rest with production of Λ and K s 0 , using a streamer chamber with 3 He, 4 He and 20 Ne as gas targets. The data include Λ, K s 0 , ΛK s 0 and K s 0 K S 0 production rates and momentum distributions, π − momentum spectra, mean numbers of charged particles generally and of negatively charged particles separately for different reaction channels. The yields are compared to simple combinatorial calculations based on the extreme assumptions of Λ production via B = 1 or via B = 0 ( K rescattering) annihilations. Λ and K s 0 momentum spectra are compared to simple model calculations where B = 0 and B = 1 annihilations with and without final-state interactions are considered. A review of existing data on Λ and K s 0 production is presented, showing the dependence on the p momentum and on the mass number of the target.
Nuclear Physics | 1984
D. Allasia; C. Angelini; A. Baldini; S. Barlag; L. Bertanza; A. Bigi; V. Bisi; F. Bobisut; T. Bolognese; R. Bonarelli; E. Calimani; R. Casali; P. Capiluppi; S. Ciampolillo; J. Derkaoui; E. A. De Wolf; M.L. Faccini-Turleur; R. Fantechi; V. Flaminio; A. G. Frodesen; D. Gamba; G. Giacomelli; A. Halsteinslid; A. Hornaes; H. Huzita; B. Jongejans; M. Loreti; C. Louedec; G. Mandrioli; A. Marzari-Chiesa
Abstract The total νμ and ν μ nucleon charged-current cross sections have been measured in BEBC filled with deuterium and exposed to the wide-band neutrino and antineutrino beams at the CERN-SPS. Assuming a linear energy dependence for the cross sections, σ = aE(−ν, we obtained the coefficients a ν N = 0.62 ± 0.05 and a ν N = 0.33 ± 0.03 (in units of 10 −38 cm 2 /GeV) , where the quoted error is mainly systematic. The ratio of the cross sections is σ ν N /σ ν N = 0.53 ± 0.03 . We also determined the ratio of the charged-current cross section for neutrino interactions on neutrons and protons R = σνn/σνp = 2.10 ± 0.08 (statistical) ±0.22 (sysetmatic). The dependence of R on the variables x, y and Eν is discussed.
Nuclear Physics | 1989
F. Balestra; S. Bossolasco; M.P. Bussa; L. Busso; L. Ferrero; D. Panzieri; G. Piragino; F. Tosello; R. Barbieri; G. Bendiscioli; A. Rotondi; P. Salvini; A. Zenoni; Yu. A. Batusov; I. V. Falomkin; G. B. Pontecorvo; M.G. Sapozhnikov; V.I. Tretyak; C. Guaraldo; A. Maggiora; E. Lodi Rizzini; A. Haatuft; A. Halsteinslid; K. Myklebost; J.M. Olsen; F.O. Breivik; T. Jacobsen; S.O. Sørensen
Abstract The analysis is based upon pNe annihilation events at rest and at 607 MeV/c detected with a self-shunted streamer chamber exposed to the LEAR beams. The main measured quantities are the following: charged-prong multiplicity, negative pion multiplicity; momentum, angular and rapidity distributions. General distributions are given as well as distributions as functions of charged prong multiplicity. A correlation is found between high multiplicity and depth of the annihilation point. The data are compared with recent theoretical analyses.
Nuclear Physics | 1978
O. Erriquez; M.T. Fogli Muciaccia; S. Natali; S. Nuzzo; A. Halsteinslid; C. Jarlskog; K. Myklebost; A. Rognebakke; O. Skjeggestad; B. Tvedt; S. Bonetti; Donatella Cavalli; A. Pullia; M. Rollier; G. Bonneaud; B. Escoubes; J.L. Guyonnet; D. Huss; M. Paty; C. Racca; J.L. Riester; M. Schaeffer; D. Allasia; V. Bisi; C. Franzinetti; D. Gamba; A. Marzari-Chiesa; L. Riccati; A. Romero; R. Sacco
Abstract We have studied neutral strange particle production in the bubble chamber Gargamelle filled with propane and exposed to antineutrinos from the CERN PS. Cross sections are presented for Λ, Σ0 and K0 production. Associated production reactions (ΔS = 0) have been observed in the charged and the neutral current channels. From 45 candidates for the quasi-elastic reaction ν p → μ + Λ , on bound and free protons, estimates of the axial transition form factor MA have been made using the total cross section and the t distribution. The weighted average from the two methods is MA = 862 ± 190 MeV. From a subsample of 15 candidates for ν interactions on free protons in propane, with (28±6)% background from ν interactions on bound protons, we obtain MA = 883 ± 243 MeV. The polarization of the Λ hyperons has been studied for the quasi-elastic reaction. We observe a significant Λ polarization in the production plane, normal to the Λ line of flight. The observed polarizations agree well with the predicted theoretical polarizations without any contribution from second-class axial coupling.
Physics Letters B | 1983
D. Allasia; C. Angelini; A. Baldini; M. Baldo-Ceolin; S. Barlag; L. Bertanza; A. Bigi; V. Bisi; F. Bobisut; T. Bolognese; A. Borg; E. Calimani; P. Capiluppi; R. Casali; S. Ciampolillo; J. Derkaoui; M. L. Faccini-Turluer; R. Fantechi; V. Flaminio; A. G. Frodesen; D. Gamba; G. Giacomelli; A. Halsteinslid; A. Hornaes; H. Huzita; B. Jongejans; I. Lippi; M. Loreti; C. Louedec; G. Mandrioli
Abstract We have measured neutral and charged current interactions of ν μ and ν μ on proton and neutron. From a combination of ratios we determine the neutral current chiral coupling constants. The results are u 2 L = 0.13 ± 0.03, d 2 L = 0.19 ± 0.03, u 2 R = 0.02 ± 0.02 and d 2 R = 0.00 ± 0.02. These results agree with the predictions of the standard SU(2) × U(1) model. The corresponding value of sin 2 θ W is 0.20 ± 0.04.
Nuclear Physics | 1990
G. Bendiscioli; V. Filippini; A. Rotondi; P. Salvini; A. Venaglioni; S. Bossolasco; M.P. Bussa; L. Busso; L. Fava; L. Ferrero; A. Maggiora; D. Panzieri; G. Piragino; R. Piragino; F. Tosello; Yu. A. Batusov; I. V. Falomkin; G. B. Pontecorvo; A.M. Rozhdestvensky; M.G. Sapozhnikov; V.I. Tretyak; C. Guaraldo; E. Lodi Rizzini; A. Haatuft; A. Halsteinslid; K. Myklebost; J.M. Olsen; F.O. Breivik; T. Jacobsen; S.O. Sørensen
Abstract The pionic annihilation of antiprotons stopped on 3 He nuclei in a self-shunted streamer chamber exposed to the antiproton beam of LEAR is studied. The data concern charged-particle multiplicity distributions, branching ratios for different final states, the probability of final-state interaction, π − , π + , p and d momentum spectra, like and unlike pion angular correlations, π and other charged-particle angular correlations. The comparison of the 3 He data with those obtained on 1 H, 2 H and 4 He does not reveal relevant effects due to the increase of the nucleon number; the small differences can be seen as due to a weak final-state interaction.