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Related papers: D0 Silicon Microstrip Tracker fro Run IIa

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With a total area of 210 squaremeters and about 15000 single silicon modules the silicon strip tracker of the CMS experiment at the LHC will be the largest silicon strip detector ever built. While the performance of the individual…

Instrumentation and Detectors · Physics 2019-08-14 Katja Klein

The XAA1.2 is a custom ASIC chip for silicon microstrip detectors adapted by Ideas for the SuperAGILE instrument on board the AGILE space mission. The chip is equipped with 128 input channels, each one containing a charge preamplifier,…

To fully exploit the HERA-II upgrade,the ZEUS experiment has installed a Micro Vertex Detector (MVD) using n-type, single-sided, silicon micro-strip sensors with capacitive charge division. The sensors have a readout pitch of 120…

High Energy Physics - Experiment · Physics 2009-11-07 D. Dannheim , U. Koetz , C. Coldewey , E. Fretwurst , A. Garfagnini , R. Klanner , J. Martens , E. Koffeman , H. Tiecke , R. Carlin

We present the results of an upgrade to the D0 muon system. Scintillating counters have been added to the existing central D0 muon system to provide rejection for cosmic ray muons and out-of-time background, and to provide additional fast…

High Energy Physics - Experiment · Physics 2012-08-27 D0 Collaboration

A next generation silicon vertex detector is planned at CDF for the 1998 Tevatron collider run with the Main Injector. The SVX~II silicon vertex detector will allow high luminosity data-taking, enable online triggering of secondary vertex…

High Energy Physics - Experiment · Physics 2019-08-14 J. Skarha

A central tracker based on silicon microstrip sensors has been envisaged for the e+e- linear collider experiments. A full simulation program based on GEANT4 has been developed to study performance of the tracker. We report some preliminary…

High Energy Physics - Experiment · Physics 2007-05-23 M. Iwasaki

Very compact 70 MeV pulse race-track microtron is under construction now. To acquire outputs of beam-current transformers on every orbit and pulses of high voltage and RF field a distributed multi-channel beam diagnostic system was…

Accelerator Physics · Physics 2007-05-23 A. Chepurnov , I. Gribov , V. Shvedunov , F. Nedeoglo , O. Novojilov , S. Dudnikov

Several future high-energy physics facilities are currently being planned. The proposed projects include high energy $e^+ e^-$ circular and linear colliders, hadron colliders and muon colliders, while the Electron-Ion Collider (EIC) has…

New data on jet production obtained by the CDF and D0 Collaborations at the Tevatron in Run II are analyzed in the framework of z-scaling. Properties of data z-presentation are discussed. Physics interpretation of the scaling function…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. V. Tokarev , T. G. Dedovich

The HERA-B Outer Tracker is a large system of planar drift chambers with about 113000 read-out channels. Its inner part has been designed to be exposed to a particle flux of up to 2.10^5 cm^-2 s^-1, thus coping with conditions similar to…

Instrumentation and Detectors · Physics 2009-11-11 H. Albrecht

The 1992-1995 running of the Fermilab Tevatron ended with many important physics goals accomplished, including the discovery of the top quark, and the anticipation of many further questions to be answered in the future. After many upgrades…

High Energy Physics - Experiment · Physics 2019-08-14 Arnd Meyer

The Tevatron experiments, CDF and D0, have produced a wealth of new B-physics results since the start of Run II in 2001. We've observed new B-hadrons, seen new effects, and increased many-fold the precision with which we know the properties…

High Energy Physics - Experiment · Physics 2019-08-14 Harold G Evans

Preliminary results on the top pair production cross section measurements by the D0 and CDF experiments in Run II at the Tevatron are presented. The measurements are obtained using various final state signatures.

High Energy Physics - Experiment · Physics 2019-08-14 Reinhard Schwienhorst

The evolution of particle detectors has always pushed the technological limit in order to provide enabling technologies to researchers in all fields of science. One archetypal example is the evolution of silicon detectors, from a system…

Instrumentation and Detectors · Physics 2017-07-04 Hartmut F. -W. Sadrozinski , Abraham Seiden , Nicolò Cartiglia

After a hiatus of almost 6 years and an extensive upgrade, Tevatron, the world largest proton--antiproton collider, has resumed the operation for the so called RUN II. In this paper we give a brief overview of the many new features of the…

High Energy Physics - Experiment · Physics 2016-08-31 M. Rescigno

We calculate the cross section for eta_b production at the Tevatron at next-to-leading order in the strong coupling and find that more than two millions of eta_b's are expected per inverse picobarn of integrated luminosity. We discuss the…

High Energy Physics - Phenomenology · Physics 2009-11-10 F. Maltoni , A. D. Polosa

Run II of the Tevatron collider at Fermilab is well under way and data samples larger than those of Run I are at hand. In this contribution I summarize the current status of cross-section measurements for top-quark pair production at the…

High Energy Physics - Experiment · Physics 2009-11-10 Wolfgang Wagner

Two MiniPlug calorimeters, designed to measure the energy and lateral position of particles in the pseudorapidity region of 3.6<|eta|<5.1 of the CDF detector, have been installed as part of the Run II CDF upgrade at the Tevatron collider.…

Instrumentation and Detectors · Physics 2014-11-18 K. Goulianos , M. Gallinaro , K. Hatakeyama , S. Lami , C. Mesropian , K. Terashi

MiniMax (Fermilab T-864) was a small test/experiment at the Tevatron designed to search for disoriented chiral condensates (DCC) in the forward direction. The MiniMax detector at the C0 collision region of the Tevatron was a telescope of 24…

High Energy Physics - Experiment · Physics 2007-05-23 Mary E Convery

The STAR Silicon Strip Detector (SSD) completes the three layers of the Silicon Vertex Tracker (SVT) to make an inner tracking system located inside the Time Projection Chamber (TPC). This additional fourth layer provides two dimensional…

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