Two-dimensional position sensitive transition radiation detector

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Abstract

A new transition radiation detector (TRD) prototype foreseen to fulfill the requirements of the TRD subdetector of the CBM experiment at FAIR has been designed, constructed and tested with electrons and pions of a few GeV/c. The detector prototype was build with the original TRD architecture which preserves the high conversion efficiency of transition radiation in a single TRD layer. This TRD architecture is based on two multiwire proportional chambers readout by a common double-sided pad read-out electrode. The triangular shape of the readout pads gives access to the position information in both coordinates which defines the readout electrode plane. Pion efficiency as a function of number of TRD layers and position resolution were studied using electron and pion beams delivered by PS at CERN. Dedicated front-end electronics, designed for high counting rate environment was used. An extrapolated pion efficiency of 0.5% for a six layer TRD configuration at 90% electron efficiency using a regular foil radiator was obtained. The position resolution across the pads is of the order of 320μm and along the pads of 5.5 mm.

Highlights

► Two-dimensional position sensitive TRD. ► Highly efficient dedicated front-end electronics. ► Very good pion rejection of 200 for six TRD layers.

Introduction

The CBM (Compressed Baryonic Matter) experiment [1] at the future Facility for Antiproton and Ion Research (FAIR) [2] is designed to measure hadrons, multi-strange hyperons, lepton pairs and charmed particles produced in nuclear collisions at up to 10 MHz; it is a large acceptance and high-rate detection system. The CBM experiment includes a transition radiation detector (TRD) for identification of high-momentum electrons with a pion efficiency better than 1% for 90% electron efficiency. At the same time it will perform intermediate tracking with a position resolution of 200μm400μm in order to match tracks reconstructed in the silicon tracking system (STS) to the time-of-flight (TOF) system. Being a fixed target experiment, the most forward angles of CBM have to cope with a counting rate up to 100 kHz/cm2. Therefore a fast detector is required.

The original TRD architecture for electron discrimination in a high counting rate environment is based on two multiwire proportional chambers with a common double-sided pad structure read-out electrode [3], [4]. The detector maintains the timing properties of a single multiwire proportional chambers (MWPC) [5] while the gas thickness for transition radiation (TR) absorption is doubled. An extrapolated pion efficiency better than 1% for a six layer configuration [3] and position resolution of the order of 160μm [4] were obtained. Negligible gain drop and less than 20μm position resolution degradation were observed up to an average particle rate of 200 kHz/cm2. In order to cope with the requirement of a reasonable geometrical efficiency, a larger size prototype using the same architecture, but increasing the size of the rectangular pads of the central double sided read-out electrode was built. With the aim to access the position information in both coordinates of the readout electrode pad-plane (across and along the pads) with a single TRD layer, the rectangular pads of the read-out electrode were split diagonally, each triangular pad being readout separately. The paper is focused on the e/π discrimination and position resolution of two such TRD prototypes which were tested in a mixed secondary beam at the CERN PS.

Section snippets

Detector design

As mentioned in the Introduction, the structure of prototypes is based on two MWPC read out by a common double-sided central pad structure electrode [6]. A schematic view is shown in Fig. 1. In the upper part we present a cross-section through the detector parallel to the direction of the wires and in the lower part a cross-section perpendicular to the direction of the wires. The central readout electrode separates the detector into two identical sections. The two multiwire anode planes, below

Experimental setup

Both detectors were tested in the detector laboratory of the Hadron Physics Department of IFIN-HH with a 5.9 keV X-ray 55Fe source using 80%Ar+20%CO2 gas mixture flushed trough the counters at atmospheric pressure. The energy resolution was measured using both anode and pad signals. The anode signals were amplified by a charge sensitive preamplifier followed by a shaping amplifier.

For pad signal processing a new dedicated front-end electronics (FEE) called fast analog signal processor (FASP) [8]

Detector simulation

The maximum drift time is an important parameter for the optimization of the counter geometry for a minimum drift time required by the operation in a high counting rate environment and for the choice of the front-end electronics parameters (i.e. shaping time).

The drift time of an ionization cluster produced by a charged particle crossing the detector depends on its position relative to the anode wire and the electric field configuration. We used the Garfield/Magboltz [11] software package for

Experimental setup

The detectors were tested with a mixed electron/pion beam of 1–5 GeV/c momenta at T10 beam line of the CERN PS accelerator in a joint measurement campaign of the CBM Collaboration [10].

In the common beam test, prototypes of three CBM subsystems were tested as shown in Fig. 6: upstream, the first in the beam line, was a STS prototype, followed by a ring imaging Cherenkov detector (RICH) prototype and nine TRD prototypes from four research sites (Bucharest, Dubna, Frankfurt and Münster). The

Conclusions

We have investigated the electron–pion discrimination and two-dimensional position resolution of the developed TRD prototypes operated with the dedicated new front-end electronics—FASP. The design based on two MWPC readout by a common pad plane electrode with a negligible absorption of TR improves the rejection power of a single TRD layer while conserving the timing properties of a single MWPC with the same anode–cathode distance [5]. The readout electrode with triangular shaped pads allows for

Acknowledgments

We acknowledge V. Aprodu, L. Prodan and A. Radu for their skillful contributions to the construction of the detectors. This work was supported by EU-FP7/HP2-WP18 Grant no. 227431, EU-FP7/HP3-WP19 Grant no. 283286, NASR/CAPACITATI 42EU Project and NASR/NUCLEU Project.

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