The vertex and large angle detectors of a spectrometer system for high energy muon physics

Davis, A.C.; Dobinson, R.; Dosselli, U.; Edwards, A.; Gabathuler, E.; Kellner, G.; Montgomery, H. E.; Mueller, H.; Osborne, A.M.; Scaramelli, A.; Watson, E.; Brasse, F.W.; Falley, G.; Flauger, W.; Gayler, J.; Goessling, C.; Koll, J.; Korbel, V.; Nassalski, J.; Singer, Gonen; Thiele, K.; Zank, P.; Figiel, J.; Janata, F.; Rondio, E.; Studt, M.; Torre, A. de la; Bernaudin, B.; Blum, D.; Heusse, P.; Jaffré, M.; Noppe, J.M.; Pascaud, C.; Bertsch, Y.; Bouard, X. De; Broll, C.; Coignet, G.; Favier, Jean; Jansco, G.; Lebeau, M.; Maire, M.; Minssieux, H.; Montanet, F.; Moynot, M.; Nagy, E.; Payre, P.; Perrot, G.; Pessard, H.; Ribarics, P.; Schneegans, M.; Thénard, J.M.; Botterill, D.; Carr, J.; Clifft, R. W.; Edwards, M.; Norton, P. R.; Rousseau, Martine; Sproston, M.; Thompson, J.C.; Albanèse, J.P.; Allkofer, O.C.; Arneodo, M.; Aubert, J.J.; Becks, K. H.; Bee, C. P.; Benchouk, C.; Bianchi, F.; Bibby, J.H.; Bird, I.; Boehm, E.; Braun, H. M.; Brown, S.; Brueck, H.; Callebaut, D. K.; Cobb, J.H.; Combley, F.; Cornelssen, M.; Costa, F.; Coughlan, J. A.; Court, G.R.; D’Agostini, G.; Dau, W.D.; Davies, Joshua; Dengler, F.; Derado, I.; Drees, J.; Dumont, J. J.; Eckardt, V.; Ferrero, M. I.; Gamet, R.; Gebauer, H. J.; Haas, J.; Hasert, F.J.; Hayman, P.; Johnson, A.; Kabuß, E. M.; Kahl, Th.; Krueger, Julia J.; Landgraf, U.; Lanske, D.; Loken, J.; Manz, A.; Mermet-Guyennet, Michel; Mohr, W.; Moser, K.; Mount, R.; Paul, Larissa; Peroni, C.; Pettingale, J.; Poetsch, M.; Preissner, H.; Renton, P.; Rith, Klaus; Roehner, F.; Schlagboehmer, A.; Schmitz, N.; Schultze, K.; Shiers, J.; Sloan, T.; Smith, Rita; Stier, H. E.; Stockhausen, W.; Wahlen, H.; Wallucks, W.; Whalley, M. A.; Williams, D.; Williams, W. S. C.; Wimpenny, S.; Windmolders, R.; Winkmueller, G.; Wolf, G.

doi:10.1016/0167-5087(83)90682-8

Cited by 34 publications

(4 citation statements)

References 10 publications

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“…It has never been documented except in an NAS internal note [Sey86]. The NA5 streamer chamber was also used by the EMC collaboration for experiment NA9 [Alb83] but with different optics.…”

Section: Optical Constants and Distortion Correctionmentioning

confidence: 99%

“…The distortion correction procedure will be represented by the mapping DC : R2 -+ R2 from the film plane to itself. The fiducial system consists of a square distortion grid above the chamber at z ~ +43 cm and a set of fiducial marks below it at z ~ -40 cm [Alb83]. The need for distortion correction is evident from a CCD picture of the distortion grid.…”

Section: Optical Constants and Distortion Correctionmentioning

confidence: 99%

“…The projectile nuclei strike nuclear targets positioned", 8 cm upstream of the streamer chamber entrance window. 1 The streamer chamber, constructed inside a large superconducting magnet, was previously employed in experiments NA5 [DeM82a] and NA9 [Alb83]. It can measure exclusive, final state charged particle multiplicities, inclusive charged particle spectra, charged particle correlations, and strange particle spectra and yields from V O decays and from the charged K decays K± -+ 1I'"±1I'"0 , K± -+ 1I'"±1I'"±1I'"T in its fiducial volume.…”

Section: Na35 Experimental Overviewmentioning

confidence: 99%

“…The NA35 streamer chamber [Alb83] is a large chamber with a sensitive volume of 2.0 x 1.2 x .72 m 3 • It rests in a superconducting vertex magnet with a central magnetic field strength B of 1.5 Tesla. Because of the size of the chamber the field varies by as much as 20% near the edges of the fiducial volume.…”

Section: Streamer Chambermentioning

confidence: 99%

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Charged particle spectra in [sup 32]S + [sup 32]S interactions at 200 GeV/nucleon from CCD-imaged nuclear collisions in a streamer chamber

Teitelbaum¹

1992

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“…It has never been documented except in an NAS internal note [Sey86]. The NA5 streamer chamber was also used by the EMC collaboration for experiment NA9 [Alb83] but with different optics.…”

Section: Optical Constants and Distortion Correctionmentioning

confidence: 99%

Section: Optical Constants and Distortion Correctionmentioning

confidence: 99%

Section: Na35 Experimental Overviewmentioning

confidence: 99%

Section: Streamer Chambermentioning

confidence: 99%

See 2 more Smart Citations

Charged particle spectra in [sup 32]S + [sup 32]S interactions at 200 GeV/nucleon from CCD-imaged nuclear collisions in a streamer chamber

Teitelbaum¹

1992

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Review of Deep Inelastic Charged Lepton Scattering

Nowak

1986

Fortschr. Phys.

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The present situation in deep inelastic lepton-nucleon scattering is reviewed from an experimenter's point of view . After describing. in some detail. the quark-parton model (QPM) predictions the basic ideas of Quantum Chromodynamics (QCD) are illustrated . The perturbative QCD predictions for deep inelastic scattering are summarised discussing also their theoretical uncertainties of today .Past and present experiments on deep inelastic electron and muon scattering are compared regarding their ability to test these predictions . It is shown that all data is in very good agreement with the QPM and fully consistent with perturbative QCD . New results on lepton scattering off nuclei are discussed and confronted to recently invented phenomenological models .

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Review of Deep Inelastic Charged Lepton Scattering

Nowak¹

1986

Fortschr. Phys.

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The vertex and large angle detectors of a spectrometer system for high energy muon physics

Cited by 34 publications

References 10 publications

Charged particle spectra in [sup 32]S + [sup 32]S interactions at 200 GeV/nucleon from CCD-imaged nuclear collisions in a streamer chamber

Charged particle spectra in [sup 32]S + [sup 32]S interactions at 200 GeV/nucleon from CCD-imaged nuclear collisions in a streamer chamber

Review of Deep Inelastic Charged Lepton Scattering

Review of Deep Inelastic Charged Lepton Scattering

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