Abstract

Drift tube chambers are commonly used in many experiments in High EnergyPhysics (HEP). This paper addresses the problem of particle track finding in a drift tubechamber. Although drift tubes have, in general, a high efficiency to detect the passage ofparticles, in a high radiation background some of the particle hits will be masked by backgroundhits. Under the assumption of high tube efficiency, a novel track finding algorithm, denoted asthe Drift Tube Hough Transform (DTHT) algorithm, is presented. The DTHT algorithm usesthe possible explanations for a lack of particle hits as additional information, and takes intoaccount all possible scenarios that may occur in the tubes. The DTHT is implemented with anovel extension of the Hough transform and employs a ``detect before estimate'' approach thatfirst finds the track candidates and then estimates the track parameters. In order to evaluate theperformance of the DTHT algorithm, the algorithm was applied to the Monitored Drift Tube(MDT) of the ATLAS experiment and tested using a muon test beam in a high radiationbackground. It is shown that the use of the additional information reduces the number of faketrack rate significantly. A comparison between the DTHT algorithm and the currently bestperformed program in the ATLAS software, demonstrated that the DTHT algorithm can achievehigher efficiency while reducing the algorithm complexity.

Highlights

  • Background radiation levelFigure 11 depicts the efficiency as a function of the different background rates for the Muonboy and the Drift Tube Hough Transform (DTHT) algorithms

  • The DTHT algorithm has been applied to the data of test beam for background rate varying from 0 kHz per tube till 400 kHz per tube

  • It is defined as −1, where nMDT is the total number of tracks reconstructed by the algorithm assuming that in each event there is one real muon track

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Summary

Introduction

The efficiency values taken for the DTHT algorithm are those with approximately the same fake track rate as the MuonBoy algorithm. For both algorithms the efficiency decreases where the background level increases. It can be seen that the performance of the DTHT algorithm is slightly better than the MuonBoy algorithm for a high radiation background. It is possible to adjust the efficiency and fake rate values of the DTHT algorithm by changing the 2 and parameters and get a better efficiency while χ λ increasing the fake track rate. As for the MuonBoy algorithm, higher efficiencies could not be achieved, even for higher fake track rate

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