نتایج جستجو برای: track detector
تعداد نتایج: 121041 فیلتر نتایج به سال:
Computer programs have been developed to calculate track parameters and to plot track openings and wall pro$les. The programs are based on equations derived for three-dimensional consideration of track development. All possible cases of track openings and wall pro$les are obtainable from these equations. Results are given for lengths of major and minor axes, track depths and surface areas of tr...
Since 2001 the CDF II detector has been collecting data used to carry out a rich physics program at the Fermilab Tevatron pp̄ collider. The quality and purity of the data relies heavily on the high performance and efficiency of the CDF trigger system. The online trigger most heavily relied on for physics analyses is the eXtremely Fast Tracker (XFT), a track trigger system used to identify charge...
A new instrument was developed to measure radon exposure with the use of passive monitors like nuclear track etch detectors. It is based on a device to be switched on and off to permit accurate measurements of timed exposures. The detector arrangement consists of a small cylindrical chamber, a mobile piston inside, a filter holder, a detector holder. The internal sampling volume is variable. Th...
In this work, the empirical parameterization describing the alpha particles’ track depth in CR-39 detectors is extended to describe longitudinal track profiles against etching time for protons and alpha particles. MATLAB based software is developed for this purpose. The software calculates and plots the depth, diameter, range, residual range, saturation time, and etch rate versus etching time. ...
Accurate measurements of the muon component in EAS are particularily important for determination of the primary CR spectrum and composition. Multiparameter analysis possibilities in KASCADE have been recently enhanced by starting the operation of a large area streamer tube muon tracking detector. With its acceptance of about 500 m·sr it identifies EAS muons with energy exceeding 0.8 GeV. The re...
The nuclear track detector CR39 was calibrated with different ions of different energies. Due to the low detection threshold (Z/β ∼ 6e) and the good charge resolution (σZ ∼ 0.2e for 6e ≤ Z/β ≤ 83e with 2 measurements), the detector was used for different purposes: (i) fragmentation of high and medium energy ions; (ii) search for magnetic monopoles, nuclearites, strangelets and Q-balls in the co...
We describe the construction and performance of a scintillating fiber detector used in the near detector for the K2K (KEK to Kamioka, KEK E362) long baseline neutrino oscillation experiment. The detector uses 3.7 m long and 0.692 mm diameter scintillating fiber coupled to image-intensifier tubes (IIT), and a CCD camera readout system. Fiber sheet production and detector construction began in 19...
The D0 Run II silicon microstrip tracker (SMT) has 3 square meters of Si area. There are 792,576 channels read out by 6192 SVXIIe chips on 912 read out modules. The SMT provides track and vertex reconstruction capabilities over the full pseudorapidity coverage of the D0 detector. The full detector has been running successfully since April 2002. This presentation covers the experience in commiss...
With an effective telescope area of order 10 m for TeV neutrinos, a threshold near ∼50 GeV and a pointing accuracy of 2.5 degrees per muon track, the AMANDA detector represents the first of a new generation of high energy neutrino telescopes, reaching a scale envisaged over 25 years ago. We describe early results on the calibration of natural deep ice as a particle detector as well as on AMANDA...
We have studied the impact of charged track resolution on Higgs mass and production cross section measurement in the process ee → ZH,Z → ll,H → X for Higgs masses between 120 and 160 GeV, and on smuon mass measurement using smuon pair production for three different mass pairs, assuming the International Linear Collider(ILC) is operated at 500 GeV center of mass energies (CME) with integrated lu...
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