The tracking, calorimeter and muon detectors of the H1 experiment at HERA

Abt, I.; Ahmed, T.; Aïd, S.; Andreev, V.; Andrieu, Bernard; Appuhn, R. D.; Arnault, C.; Arpagaus, M.; Babaev, A.; Bärwolff, H.; Bán, J.; Banaś, E.; Baranov, P.; Barrelet, E.; Bartel, W.; Barth, M.; Bassler, U.; Basti, F.; Baynham, D.E.; Baze, J.M.; Beck, G. A.; Beck, H. P.; Bédérède, D.; Behrend, H. J.; Beigbeder, C.; Belousov, A.; Berger, Ch.; Bergstein, H.; Bernard, R.; Bernardi, G.; Bernet, R.; Bernier, R.; Berthon, U.; Bertrand-Coremans, G.; Besançon, M.; Beyer, R.; Biasci, Jean-Claude; Biddulph, P.; Bidoli, V.; Binder, E.; Binko, P.; Bizot, J.C.; Blobel, V.; Blouzon, F.; Blume, H. T.; Borras, K.; Boudry, V.; Bourdarios, C.; Brasse, F.W.; Braunschweig, W.; Bretón, D.; Brettel, H.; Brisson, V.; Bruncko, D.; Brune, C. R.; Buchner, U.; Büngener, L.; Bürger, J.; Büsser, F.W.; Buniatian, A.; Bürke, S.; Burmeister, P.; Busata, A.; Buschhorn, G.; Campbell, A.; Carli, T.; Charles, F.; Charlet, M.; Chase, R. 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C.; Savitski, M.; Schacht, P.; Schiek, S.; Schirm, N.; Schleif, S.; Schleper, P.; Schlippe, W. von; Schmidt, C.; Schmidt, D.; Schmidt, G.; Schmitz, W.; Schmücker, H.; Schröder, V.; Schütt, J.; Schuhmann, E.; Schulz, M.; Schwind, A.; Scobel, W.; Seehausen, U.; Sefkow, F.; Sell, Raivo; Seman, M.; Semenov, A.; Shatalov, P.; Shekelyan, V.; Sheviakov, I.; Shooshtari, H.; Shtarkov, L. N.; Siegmon, G.; Siewert, U.; Sirois, Y.; Sirous, A.; Skillicorn, I. O.; Škvařil, P.; Smirnov, P.; Smith, J.; Smolík, L.; Solé, Domingo Biel; Soloviev, Y.; Spałek, J.; Spitzer, H.; Staa, R. von; Staeck, J.; Staroba, P.; Šťastný, J.; Steenbock, M.; Stefan, P.M.; Steffen, P.; Steinberg, R.; Steiner, H.; Stella, B.; Stephens, K.; Stier, J.; Stiewe, J.; Stößlein, U.; Strachota, J.; Straumann, U.; Strowbridge, A.; Struczinski, W.; Sutton, J. P.; Szkutnik, Zbigniew; Tappern, G.; Tapprogge, S.; Taylor, Richard E.; Tchernyshov, V.; Tchudakov, V.; Thiebaux, Ch; Thiele, K.; Thompson, G.; Thompson, R. J.; Tichomirov, I.; Trenkel, C.; Tribanek, W.; Tröger, K.; Truöl, P.; Turiot, M.; Turnau, J.; Tutas, J.; Urbán, L.; Urban, M.; Usik, A.; Valkár, Š.; Valkárová, A.; Vallée, C.; Beek, G. Van; Vanderkelen, Mark; Lancker, L. Van; Mechelen, P. Van; Vartapetian, A.; Vazdik, Y.; Vecko, M.; Verrecchia, P.; Vick, R.; Villet, G.; Vogel, E.; Wacker, K.; Wagener, M.; Walker, I. W.; Walther, A.; Weber, G.; Wegener, D.; Wegner, A.; Weissbach, P.; Wellisch, H. P.; West, L.R.; White, David J.; Willard, S.; Winde, M.; Winter, G. G.; Wolff, Th.; Womersley, L.A.; Wright, A.E.; Wünsch, E.; Wulff, N.; Wyborn, B. E.; Yiou, T. P.; Žáček, J.; Zarbock, D.; Závada, P.; Zeitnitz, C.; Zhang, Z.; Ziaeepour, H.; Zimmer, M.; Zimmermann, W.; Zomer, F.; Zuber, Κ.

doi:10.1016/s0168-9002(96)00894-7

Cited by 234 publications

(72 citation statements)

References 34 publications

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“…A detailed description of the H1 detector can be found elsewhere [15][16][17]. The right-handed coordinate system of H1 is defined such that the positive z-axis is in the direction of the proton beam (forward direction), and the nominal interaction point is located at z = 0.…”

Section: The H1 Detectormentioning

confidence: 99%

Measurement of multijet production in $${e\!\!\;p}$$ e p collisions at high $$\varvec{Q^2}$$ Q 2 and determination of the strong coupling $$\varvec{{\alpha _s}} $$ α s

et al. 2015

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Inclusive jet, dijet and trijet differential cross sections are measured in neutral current deep-inelastic scattering for exchanged boson virtualities 150 < Q 2 < 15 000 GeV 2 using the H1 detector at HERA. The data were taken in the years 2003 to 2007 and correspond to an integrated luminosity of 351 pb −1 . Double differential jet cross sections are obtained using a regularised unfolding procedure. They are presented as a function of Q 2 and the transverse momentum of the jet, P

show abstract

Section: The H1 Detectormentioning

confidence: 99%

Measurement of multijet production in $${e\!\!\;p}$$ e p collisions at high $$\varvec{Q^2}$$ Q 2 and determination of the strong coupling $$\varvec{{\alpha _s}} $$ α s

et al. 2015

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“…A detailed description of the H1 detector can be found elsewhere [36][37][38]. Here only the detector components most relevant to the present analysis are briefly described.…”

Section: The H1 Detectormentioning

confidence: 99%

Diffractive dijet production with a leading proton in ep collisions at HERA

Andreev¹,

Baghdasaryan²,

Begzsuren³

et al. 2015

J. High Energ. Phys.

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Abstract:The cross section of the diffractive process e + p → e + Xp is measured at a centre-of-mass energy of 318 GeV, where the system X contains at least two jets and the leading final state proton p is detected in the H1 Very Forward Proton Spectrometer. The measurement is performed in photoproduction with photon virtualities Q 2 < 2 GeV 2 and in deep-inelastic scattering with 4 GeV 2 < Q 2 < 80 GeV 2 . The results are compared to nextto-leading order QCD calculations based on diffractive parton distribution functions as extracted from measurements of inclusive cross sections in diffractive deep-inelastic scattering.

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“…The H1 detector [18] combines tracking in a solenoidal magnetic field of 1.15 T with nearly hermetic calorimetry to investigate high energy ep interactions at HERA. For polar angles θ e > 153 o the scattered positron energy E ′ e is measured in the backward electromagnetic lead-fibre scintillator calorimeter (SPACAL) [19] which has an integrated timing function to veto proton beam induced background interactions.…”

Section: H1 Detectormentioning

confidence: 99%