E. Cerron Zeballos
CERN
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Featured researches published by E. Cerron Zeballos.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1996
E. Cerron Zeballos; I. Crotty; D. Hatzifotiadou; J. Lamas Valverde; S. Neupane; M.C.S. Williams; A. Zichichi
Abstract This Letter describes the multigap resistive plate chamber (RPC). The goal is to obtain a much improved time resolution, keeping the advantages of the wide gap RPC in comparison with the conventional narrow gap RPC (smaller dynamic range and thus lower charge per avalanche which gives higher rate capability and lower power dissipation in the gas gap).
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2000
A. Akindinov; F Anselmo; M. Basile; E. Cerron Zeballos; L Cifarelli; F. Cindolo; Jinhyuk Choi; B Cozzoni; A. De Caro; S. De Pasquale; D. W. Kim; N.Y Kim; W. Klempt; Alexander Kluge; G. Laurenti; S. Lee; V. Golovine; D. Hatzifotiadou; A.N. Martemiyanov; P. Martinengo; Alessandro Pesci; E. Platner; J. Roberts; A Seganti; A Semak; A.V. Smirnitski; M Spegel; P. Szymanski; G. Valenti; D. Vicinanza
Abstract The goal of this R&D has been to reach the time resolution needed for Time-of-Flight detectors using the Multigap Resistive Plate Chamber (MRPC). We present here a MRPC with a time resolution of 70 ps. This prototype has been studied within the R&D program for the very large area TOF array of the ALICE experiment at the CERN LHC.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1995
I. Crotty; E. Cerron Zeballos; J. Lamas Valverde; D. Hatzifotiadou; M.C.S. Williams; A. Zichichi
Abstract The resistive plate chamber (RPC) has good time and position resolution; these factors (coupled to its simple construction) make it an attractive candidate for muon trigger systems at future colliders. However, operated in spark mode, the RPC has severe rate problems that make it unusable above 10 Hz/cm 2 . We have previously published our results concerning the operation of the RPC in spark and in avalanche mode; we have shown that the rate limit can be increased to 150 Hz/cm 2 if the RPC is operated in avalanche mode. Here, we discuss the performance of chambers with 6 and 8 mm gas gaps (compared to the more usual 2 mm gap). We outline the reasons for this choice, and also discuss anode versus cathode strip readout. We have measured the efficiency versus flux, and also show that an enhanced rate limit can be obtained if only a small region of the chamber is exposed to the beam (spot illumination). Finally we have tested the performance of chambers constructed with other materials for the resistive plate and compare it to chambers constructed with our preferred plastic, melamine laminate.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1997
E. Cerron Zeballos; I. Crotty; D. Hatzifotiadou; J. Lamas Valverde; M.C.S. Williams; A. Zichichi; P. Fonte; V. Peskov
Abstract We describe our attempt to develop Resistive Plate Chambers (RPCs). One study involves the use of secondary electron emitters that consist of porous photosensitive materials (CsI, diethylferocenil-mercury, SbCs and others) deposited on a cathode; this enhances efficiency, thus allowing the use of light, non-flammable gas mixtures. The other study concerns the operation of an RPC with a narrow strip readout - the “microstrip RPC”.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1997
E. Cerron Zeballos; I. Crotty; D. Hatzifotiadou; J. Lamas Valverde; M.C.S. Williams; A. Zichichi
Abstract It is necessary to operate the resistive plate chamber (RPC) in avalanche mode to obtain high efficiency at elevated particle fluxes. We examine this mode of operation with a 2 mm gap RPC using gas mixtures containing C 2 F 4 H 2 and C 2 F 5 H. In order to explain the data we propose that the avalanche growth is strongly limited by space charge effects.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1996
E. Cerron Zeballos; I. Crotty; D. Hatzifotiadou; J. Lamas Valverde; S. Neupane; V. Peskov; S. Singh; M.C.S. Williams; A. Zichichi
Abstract In this paper we study the performance of a wide gap RPC and compare it with that of a narrow gap RPC, both operated in avalanche mode. We have studied the total charge produced in the avalanche. We have measured the dependence of the performance with rate. In addition we have considered the effect of the tolerance of gas gap and calculated the power dissipated in these two types of RPC. We find that the narrow gap RPC has better timing ability; however the wide gap has superior rate capability, lower power dissipation in the gas volume and can be constructed with less stringent mechanical tolerances.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1995
E. Cerron Zeballos; I. Crotty; D. Hatzifotiadou; J. Lamas Valverde; S. Neupane; S. Singh; M.C.S. Williams; A. Zichichi
Abstract In this paper we consider some factors that could improve the high rate performance of the RPC; we consider the role of freon in the operation of RPCs; we present results with an asymmetric RPC with one glass and one melamine resistive plate.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1998
E. Cerron Zeballos; D. Hatzifotiadou; D.W. Kim; S.C. Lee; J Lamas-Valverde; J. Roberts; E. Platner; M.C.S. Williams; A. Zichichi
Abstract We have developed a type of resistive plate chamber known as the multigap resistive plate chamber. In this paper we examine the performance when SF6 is added to the gas mixture.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1996
E. Cerron Zeballos; I. Crotty; D. Hatzifotiadou; J. Lamas Valverde; R. Veenhof; M.C.S. Williams; A. Zichichi
Abstract The multigap resistive plate chamber (MRPC) was originally designed to have improved time resolution (compared to the wide gap RPC), but also to keep the good high rate behaviour and ease of construction associated with the wide gap RPC. However in addition we observed a very long efficiency plateau, even at high rates. Here we consider fluctuations in avalanche growth, and show that the inherent “averaging” of these fluctuations can account for the enhanced performance of the multigap RPC.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1997
E. Cerron Zeballos; I. Crotty; D. Hatzifotiadou; J. Lamas Valverde; M.C.S. Williams; A. Zichichi
We present the current status of the multigap resistive plate chamber. Our device has resistive plates made of melamine and is operated in avalanche mode with argon-based gases with a small percentage of quencher (CO2, isobutane, etc). It has excellent time resolution (σ = 1.5−2 ns) and rate capability (>98% efficiency at 1 kHzcm2); in addition, it has a long efficiency plateau and low dark current.