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Nuclear Physics | 1983

Multiplicities of Secondary Hadrons Produced in Neutrino

H. Grässler; D. Lanske; R. Schulte; G. Jones; R.P. Middleton; S. W. O'Neale; K. Böckmann; W. Gebel; C. Geich-Gimbel; B. Nellen; A. Grant; D.R.O. Morrison; P. Schmid; H. Wachsmuth; J.S. Chima; M.M. Mobayyen; M. Talebzadeh; O. Villalobos-Baillie; M. Aderholz; L. Deck; N. Schmitz; R. Settles; K.L. Wernhard; W. Wittek; G. Corrigan; G. Myatt; D. Radojicic; B. Saitta; J. Wells

In an experiment with the hydrogen bubble chamber BEBC at CERN multiplicities of hadrons produced in νp and vp interactions have been investigated. Results are presented on the multiplicities of charged hadrons and neutral pions, forward and backward multiplicities of charged hadrons and correlations between forward and backward multiplicities. Comparisons are made with hadronic reactions and e+e− annihilation. In the framework of the quark-parton model the data imply similar charged multiplicities for the fragments of a u- and a d-quark, and a larger multiplicities for the fragments of a uu- than for a ud-diquark. The correlation data suggest independent fragmentation of the quark and diquark for hadronic masses above ∼ 7 GeV and local charge compensation within an event.


Nuclear Physics | 1981

p

P. Allen; J. Blietschau; H. Grässler; D. Lanske; R. Schulte; H.H. Seyfert; K. Böckmann; C. Geich-Gimbel; T. P. Kokott; B. Nellen; R. Pech; H. Saarikko; P. Bosetti; V.T. Cocconi; B. Conforto; A. Grant; P.O. Hulth; G. Kellner; D. R. O. Morrison; R. Orava; L. Pape; P. Schmid; W.G. Scott; H. Wachsmuth; M. Aderholz; N. Schmitz; R. Settles; K.L. Wernhard; W. Wittek; R. Batley

Abstract Multiplicity distributions of charged hadrons produced in νp interactions are studied using a sample of 7850 charged current interactions in BEBC. Multiplicity moments are studied as functions of the invariant mass of the hadronic system, W , and a comparison is made with other lepton- and hadron-induced reactions. The mean charged multiplicity 〈 n ch 〉 is found to increase linearly with ln W 2 . The other multiplicity moments indicate a close similarity between the neutrino scattering and the class of annihilation processes. A study of the multiplicity distributions in the forward and backward directions in the hadronic c.m.s. gives results in qualitative agreement with the quark parton model.


Nuclear Physics | 1983

and Anti-neutrino

P. Allen; H. Grässler; D. Lanske; R. Schulte; K. Böckmann; C. Geich-Gimbel; B. Nellen; H. Saarikko; A. Grant; D. R. O. Morrison; P. Schmid; H. Wachsmuth; M. Aderholz; T. Coghen; N. Schmitz; K.L. Wernhard; W. Wittek; G. Corrigan; G. Myatt; D. Radojicic; B. Saitta; J. Wells

Abstract Distributions of the Feynman x variable have been determined for positive and negative pions in charged current neutrino-proton and antineutrino-proton reactions with hadronic energy W > 3 GeV and Bjorken x B > 0.1. The distributions have been corrected for experimental effects such as measurement errors, uncertainties in estimating the neutrino energy and particle misidentification. In the framework of the quark-parton model, the distributions yield information about the fragmentation of forward going u and d quarks and backward going uu and ud diquarks. Approximate Feynman scaling is observed for the invariant Feynman x F distributions. They can be fitted by a power law of the form (1 − | x F |) n as suggested by the dimensional counting rules. Simple isospin relations predicted by the quark-parton model are fulfilled. The fragmentation of diquarks is compared with that of protons into π ± .


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2003

p

M. Killenberg; S. Lotze; J. Mnich; S. Roth; R. Schulte; B. Sobloher; W. Struczinski; M. Tonutti

Measurements and numerical simulations on the charge transfer in Gas Electron Multiplier (GEM) foils are presented and their implications for the usage of GEM foils in Time Projection Chambers are discussed. A small test chamber has been constructed and operated with up to three GEM foils. The charge transfer parameters derived from the electrical currents monitored during the irradiation with an Fe-55 source are compared with numerical simulations. The performance in magnetic fields up to 2 T is also investigated.Measurements and numerical simulations on the charge transfer in Gas Electron Multiplier (GEM) foils are presented and their implications for the usage of GEM foils in Time Projection Chambers are discussed. A small test chamber has been constructed and operated with up to three GEM foils. The charge transfer parameters derived from the electrical currents monitored duringthe irradiation with an 55 Fe source are compared with numerical simulations. The performance in magnetic fields up to 2 T is also investigated. r 2002 Elsevier Science B.V. All rights reserved. PACS: 29.40.Cs; 29.40.Gx


Nuclear Physics | 1986

Charged Current Interactions

P. Allen; F. Hamisi; G. Jones; K.W.J. Barnham; E.F. Clayton; P. Schmid; N. Schmitz; E. Hoffmann; W. Wittek; R. Schulte; D. Radojicic; M. Aderholz; D.R.O. Morrison; G. Corrigan; G. Myatt; W. Gebel; H. Wachsmuth; S.J. Towers; B. Saitta; J. Mittendorfer; S. W. O'Neale; L. Deck; D.B. Miller; B. W. Kennedy; M. M. Mobayyen; P.N. Shotton; H. Grässler

Abstract We present results on exclusive single-charged pion and kaon production in neutrino and antineutrino interactions on protons in the energy range from 5 to 120 GeV. The data were obtained from exposures of BEBC to wide band beams at the CERN SPS. For invariant masses of the (pπ) system below 2 GeV, the pions originate predominantly from decays of baryon resonances excited by the weak charged current. Similarly, we observe the production of Λ(1520) decaying into p and K−. For invariant masses above 2 GeV pion production becomes peripheral by interaction of the weak current with a virtual π0. We establish a contribution of longitudinally polarised intermediate vector bosons to this process.


Nuclear Physics | 1980

Multiplicity distributions in neutrino-hydrogen interactions

K. Böckmann; J. Hofmann; U. Idschok; J. Lowsky; B. Schröder; V. Blobel; H. Fesefeldt; R. Schulte; G. Kellner; D.R.O. Morrison; H. Saarikko; T. Coghen

A study is presented of the inclusive production cross sections of K∗±(892) vector mesons in pp interactions at 12 and 24 GeV/c and in π+p interactions at 16 GeV/c. The K∗± inclusive cross section is ∼0.9 mb for both pp at 24 GeV/c and π+p interactions at 16 GeV/c. For pp interactions, σ(K∗+) and σ(K∗−) are seen to rise with energy, showing a threshold behaviour. In both pp and π+p interactions, σ(K∗+) largely exceeds σ(K∗−) at these energies and this excess is interpreted as K∗+ production by beam and target fragmentations. The decays of K∗±0 yield ∼30% of the K0 observed in the final states. The pT2 dependence of both K∗+ and K∗− cross sections is described by an exponential with slope of ∼3.3 (GeV/c)−2. The longitudinal momentum spectra for K∗+ in 16 GeV/c π+p and 24 GeV/c pp interactions are similar in shape in the target hemisphere. The K∗− spectra are similar over the whole kinematic region when viewed in the quark c.m.s. and point to a central production mechanism. Comparing K∗+ and ρ0 production, striking similarities are found.


Nuclear Physics | 1982

An investigation of quark and diquark fragmentation in νp and νp charged current interactions in BEBC

H. Grässler; C. Geich-Gimbel; R. Settles; R. Pech; P. Schmid; N. Schmitz; R. Batley; W. Wittek; R. Schulte; P. Grossmann; H.H. Seyfert; D. Radojicic; M. Aderholz; D.R.O. Morrison; G. Myatt; A. Grant; D. Lanske; V.T. Cocconi; B. Nellen; H. Wachsmuth; B. Saitta; P.O. Hulth; K.L. Wernhard; E. Simopoulou; R.H. Giles; K. Böckmann; H. Saarikko; L. Pape; P. Bosetti

In a selected sample of 6770 charged current (CC) events of νp interactions with 〈Eν〉 = 43 GeV and 〈W〉 = 4.6 GeV, 359 K0, 180 Λ and 13 Λ have been observed, which corresponds to a corrected production rate at least one neutral strange particle in (17.4±0.8)% of the CC events. The ratio of the inclusive Λ to K0 production cross section is found to be 0.26±0.03. The number of CC events containing at least one K0 increases with increasing Eν and Q2, while the CC events containing at least one Λ remain practically constant. The fractions of the total hadronic energy carried by K0 and Λ are found to be approximately the same in νp as in ep and μp interactions. In the hadronic c.m.s., the K0 are produced mostly forwards, the Λ mostly backwards, with asymmetry parameters of +0.32±0.02 and −0.45±0.06, respectively. The total strange particle production cross section is estimated to be (25±4)% of the cross section for production of CC events with W>1.5 GeV and that for charm production (10±2)% of the CC cross section well above charm threshold (W>3 GeV). The production of the resonances K∗+ (890) and Σ+ (1385) has been observed. The production rate of K∗+ (890) is comparable to that of D∗+ (2009), above the corresponding thresholds.


Physics Letters B | 1982

Modelling and measurement of charge transfer in multiple GEM structures

P. Bosetti; K.W.J. Barnham; P. Fritze; C. Peyrou; D.H. Perkins; D. Cundy; R. Schulte; E. Pagiola; J. Velasco; D.R.O. Morrison; C. Albajar; I. Butterworth; B. Tallini; G. Iaselli; B. Nellen; M. M. Mobayyen; H. Wachsmuth; A. Vayaki; C. Penfold; A. Petridis; D. Radojicic; B. Saitta; P.O. Hulth; E. Simopoulou; K. Böckmann; D. Vignaud; D.B. Miller; L. Pape; W.G. Scott; B. Wünsch

Abstract Exposures of the Ne/H 2 filled Big European Bubble Chamber (BEBC) to a dichromatic neutrino (antineutrino) beam produced by 400 GeV protons of the CERN SPS yielded ∼ 3100 events with a negative, and ∼ 1100 with a positive, muon. The neutrino flux is determined from the muon flux in the shielding. Assuming a linear energy dependence of the cross section, the values σ E between 20 and 200 GeV are found to be 0.657 ± 0.012 (stat.) ± 0.027 (syst.) and 0.309 ± 0.009 (stat.) ± 0.013 (syst.) cm 2 (GeV nucleon) −1 , for neutrinos and antineutrinos, respectively. The scaling variable q 2 E decreases significantly with increasing energy both for neutrinos and antineutrinos.


Physics Letters B | 1979

A study of single-meson production in neutrino and antineutrino charged-current interactions on protons

J. Blietschau; H. Grässler; W. Krenz; D. Lanske; R. Schulte; H.H. Seyfert; K. Böckmann; P. Checchia; C. Geich-Gimbel; H.G. Heilmann; T. P. Kokott; B. Nellen; R. Pech; L. Bacci; P. Bosetti; D. Cundy; A. Grant; P.O. Hulth; D.R.O. Morrison; R. Orava; L. Pape; Ch. Peyrou; H. Saarikko; W.G. Scott; E. Simopoulou; A. Vayaki; H. Wachsmuth; M. Aderholz; N. Schmitz; R. Settles

Abstract An analysis is presented of the z distributions of secondary hadrons produced in 5600 charged current events from a BEBC neutrino-hydrogen experiment. Evidence is presented for scaling deviations in the z distributions and a breakdown of factorization in the single particle inclusive cross sections. The results are consistent with the leading order QCD predictions on the q 2 dependence of nonsinglet moments of quark fragmentation functions, yielding a value of Λ ≈ 0.6 GeV.


Nuclear Physics | 1982

Inclusive K∗±(892) production in pp and π+p interactions

P. Bosetti; C. Geich-Gimbel; W. Glimpf; B. Wünsch; J. Wells; M. Bloch; R. Schulte; M. Mermikides; J. Velasco; D.R.O. Morrison; C. Albajar; I. Butterworth; G. Iaselli; B. Nellen; H. Wachsmuth; A. Vayaki; A. Petridis; P.O. Hulth; E. Simopoulou; P. Fritze; K. Schultze; T. Bolognese; L. Pape; M. M. Mobayyen; E.F. Clayton; A. Grant; J.S. Chima; H. Grässler

The inclusive production of K0s and Λs has been investigated in neutrino and antineutrino interactions in BEBC, filled with a neon-hydrogen mixture. The inclusive rates for the 3083 (1022) ν (ν) induced charged current events are (23.0 ± 1.7)% ((21.9 ± 2.8)%) for K0s and (5.7 ± 0.7)% ((6.5 ± 1.2)%) for Λs. The general behaviour of the K0s and Λs is found to be similar to that in νp interactions and π+p interactions at lower 〈W〉. In the hadronic c.m.s. K0s are produced mostly forwards, Λs predominantly in the backward hemisphere. The data indicate that K0s produced in ν interactions on average carry a larger fraction of the total available momentum than those in ν induced reactions. The dependences of the average transverse momentum on the variables Q2, W2 and Bjorken x are presented.

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