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Featured researches published by C. Arndt.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1997

The H1 lead/scintillating-fibre calorimeter

R.D. Appuhn; C. Arndt; E. Barrelet; R. Barschke; U. Bassler; V. Boudry; R. Buchholz; F. Brasse; D. Bruncko; S. Chechelnitski; B. Claxton; G. Cozzika; J. Cvach; S. Dagoret-Campagne; W.D. Dau; H. Deckers; T. Deckers; F. Descamps; M. Dirkmann; J. Dowdell; V. Efremenko; E. Eisenhandler; A. Eliseev; G. Falley; J. Ferencei; B. Fominykh; K. Gadow; U. Goerlach; L.A. Gorbov; I. Gorelov

Abstract The backward region of the H1 detector has been upgraded in order to provide improved measurement of the scattered electron in deep inelastic scattering events. The centerpiece of the upgrade is a high-resolution lead/scintillating-fibre calorimeter. The main design goals of the calorimeter are: good coverage of the region close to the beam pipe, high angular resolution and energy resolution of better than 2% for 30 GeV electrons. The calorimeter should be capable of providing coarse hadronic energy measurement and precise time information to suppress out-of-time background events at the first trigger level. It must be compact due to space restrictions. These requirements were fulfilled by constructing two separate calorimeter sections. The inner electromagnetic section is made of 0.5 mm scintillating plastic fibres embedded in a lead matrix. Its lead-to-fibre ratio is 2.3:1 by volume. The outer hadronic section consists of 1.0 mm diameter fibres with a lead-to-fibre ratio of 3.4:1. The mechanical construction of the new calorimeter and its assembly in the H1 detector are described.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1996

Performance of an electromagnetic lead/scintillating-fibre calorimeter for the H1 detector

T.C. Nicholls; L. Hajduk; W. Janczur; K. Rybicki; B. Claxton; J. Dowdell; H. Deckers; T. Deckers; M. Dirkmann; M. Hütte; H. Hutter; H. Kolanoski; R. Poschl; A. Schuhmacher; K. Wacker; A. Walther; D. Wegener; T. Wenk; G. Cozzika; B. Laforge; Jean-Francois Laporte; E. Perez; C. Royon; G. Villet; R.D. Appuhn; C. Arndt; R. Barschke; R. Buchholz; U. Goerlach; V. Korbel

Abstract The properties of final modules of a high resolution lead/scintillating-fibre calorimeter to upgrade the backward region of the H1 detector were studied with electrons in the energy range from 2–60 GeV. The electromagnetic calorimeter consists of scintillating fibres with a diameter of 0.5 mm embedded in a lead matrix. This small fibre radius, in combination with a lead-to-fibre ratio of 2.27:1, ensures excellent energy resolution which has been measured to be δ/E=7.1%/ E/GeV ⊕ 1.0% . The spatial resolution as a function of energy for impact points at the center of a cell is given by 4.4 mm/ E/GeV + 1.0 mm . The time resolution was found to be better than 0.4 ns.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1996

Hadronic response and e / pi separation with the H1 lead / fiber calorimeter

R.D. Appuhn; C. Arndt; E. Barrelet; R. Barschke; U. Bassler; R. Buchholz; D. Bruncko; S. Chechelnitski; B. Claxton; G. Cozzika; J. Cvach; S. Dagoret-Campagne; W.D. Dau; H. Deckers; T. Deckers; F. Descamps; M. Dirkmann; J. Dowdell; V. Efremenko; E. Eisenhandler; A. Eliseev; J. Ferencei; B. Fominykh; U. Goerlach; L.A. Gorbov; I. Gorelov; L. Hajduk; I. Herynek; J. Hladký; M. Hütte

Hadronic response and electron identification performance of the new H1 lead-scintillating fibre calorimeter are investigated in the 1 to 7 GeV energy range using data taken at the CERN Proton Synchrotron. The energy response to minimum ionizing particles and interacting pions are studied and compared to Monte Carlo simulations. The measured energy of pions interacting either in the electromagnetic or in the hadronic section is found to scale linearly with the incident energy, providing an energy resolution σE ∼ 38% within a depth of one interaction length and σE ∼ 29% for a total depth of two interaction lengths. Several electron identification estimators are studied and combined as a function of energy and impact point. The probability for pions to be misidentified as electrons of any measured energy above 1 GeV ranges from 5% (for 2 GeV incident pions) to 0.4% (at 7 GeV) for an electron detection efficiency of 90%. The probability for pions of a given energy to be misidentified as electrons of the same energy falls to 0.25% at 7 GeV.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1998

Series tests of fine mesh photomultiplier tubes in magnetic fields of up to 1.2 Tesla

R.D. Appuhn; C. Arndt; E. Barrelet; R. Barschke; U. Bassler; T. Bipp; V. Boudry; F. Brasse; D. Bruncko; R. Buchholz; S. Chechelnitski; B. Claxton; G. Cozzika; J. Cvach; S. Dagoret-Campagne; W.D. Dau; H. Deckers; T. Deckers; F. Descamps; M. Dirkmann; J. Dowdell; V. Efremenko; E. Eisenhandler; A. Eliseev; G. Falley; J. Ferencei; M. Fleischer; B. Fominykh; K. Gadow; U. Goerlach

Abstract The new lead/scintillating-fibre calorimeter (“SpaCal”) for the backward region of the H1 experiment at HERA (DESY) is equipped with fine mesh phototubes which operate in a magnetic field close to 1 T. A large sample of these tubes of the types Hamamatsu R5505 and R5506, and Hamamatsu R2490-05, have been tested in fields of up to 1.2T. We have investigated the cathode homogeneity with and without magnetic field, the gain loss under the influence of the magnetic field, and stability with time. For a subsample of tubes, we have performed additional studies on stability with respect to temperature changes, variation of gain as a function of the magnetic field, high voltage discharges, single photo-electron response, and linearity. We finally summarize the experience with these tubes after one year of operation in the experiment.

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H. Deckers

Technical University of Dortmund

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M. Dirkmann

Technical University of Dortmund

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R.D. Appuhn

Technical University of Dortmund

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T. Deckers

Technical University of Dortmund

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B. Claxton

Rutherford Appleton Laboratory

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