T. Speer
University of Zurich
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Featured researches published by T. Speer.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2008
Y. Allkofer; C. Amsler; D. Bortoletto; V. Chiochia; L. Cremaldi; S. Cucciarelli; A. Dorokhov; Ch. Hörmann; Roland Horisberger; D. W. Kim; M. Konecki; Danek Kotlinski; K. Prokofiev; C. Regenfus; Tilman Rohe; David A Sanders; S. Son; M. Swartz; T. Speer
The CMS experiment at the LHC includes a hybrid silicon pixel detector for the reconstruction of charged tracks and of the interaction vertices. The barrel region consists of n-in-n sensors with 100X150 um^2 cell size processed on diffusion oxygenated float zone silicon. A biasing grid is implemented and pixel isolation is achieved with the moderated p-spray technique. An extensive test program was carried out on the H2 beam line of the CERN SPS. In this paper we describe the sensor layout, the beam test setup and the results obtained with both irradiated and non-irradiated prototype devices. Measurements of charge collection, hit detection efficiency, Lorentz angle and spatial resolution are presented.
IEEE Transactions on Nuclear Science | 2005
V. Chiochia; M. Swartz; D. Bortoletto; L. Cremaldi; S. Cucciarelli; A. Dorokhov; Christoph Hörmann; D. Kim; M. Konecki; Danek Kotlinski; K. Prokofiev; C. Regenfus; Tilman Rohe; David A Sanders; S. Son; T. Speer
Charge collection measurements performed on heavily irradiated p-spray DOFZ pixel sensors with a grazing angle hadron beam provide a sensitive determination of the electric field within the detectors. The data are compared with a complete charge transport simulation of the sensor which includes free carrier trapping and charge induction effects. A linearly varying electric field based upon the standard picture of a constant type-inverted effective doping density is inconsistent with the data. A two-trap double junction model implemented in the ISE TCAD software can be tuned to produce a double peak electric field which describes the data reasonably well. The modeled field differs somewhat from previous determinations based upon the transient current technique. The model can also account for the level of charge trapping observed in the data.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2006
M. Swartz; V. Chiochia; Y. Allkofer; D. Bortoletto; L. Cremaldi; S. Cucciarelli; A. Dorokhov; Ch. Hörmann; D. Kim; M. Konecki; Danek Kotlinski; K. Prokofiev; C. Regenfus; Tilman Rohe; David A Sanders; S. Son; T. Speer
Abstract We show that doubly peaked electric fields are necessary to describe grazing-angle charge collection measurements of irradiated silicon pixel sensors. A model of irradiated silicon based upon two defect levels with opposite charge states and the trapping of charge carriers can be tuned to produce a good description of the measured charge collection profiles in the fluence range from 0.5 × 10 14 to 5.9 × 10 14 n eq / cm 2 . The model correctly predicts the variation in the profiles as the temperature is changed from - 10 to - 25 ∘ C . The measured charge collection profiles are inconsistent with the linearly varying electric fields predicted by the usual description based upon a uniform effective doping density. This observation calls into question the practice of using effective doping densities to characterize irradiated silicon.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2004
A. Dorokhov; C. Amsler; D. Bortoletto; V. Chiochia; L. Cremaldi; S. Cucciarelli; M. Konecki; K. Prokofiev; C. Regenfus; Tilman Rohe; David A Sanders; S. Son; T. Speer; M. Swartz
The tracking system of the CMS experiment, currently under construction at the Large Hadron Collider (LHC) at CERN (Geneva, Switzerland), will include a silicon pixel detector providing three spacial measurements in its final configuration for tracks produced in high energy pp collisions. In this paper we present the results of test beam measurements performed at CERN on irradiated silicon pixel sensors. Lorentz angle and charge collection efficiency were measured for two sensor designs and at various bias voltages.
IEEE Transactions on Nuclear Science | 2004
Tilman Rohe; D. Bortoletto; V. Chiochia; L. Cremaldi; S. Cucciarelli; A. Dorokhov; M. Konecki; K. Prokofiev; C. Regenfus; David A Sanders; S. Son; T. Speer; M. Swartz
This paper reports on the sensor R&D activity for the CMS pixel detector. Devices featuring several design and technology options have been irradiated up to a proton fluence of 1/spl times/10/sup 15/ n/sub eq//cm/sup 2/ at the CERN PS. Afterward, they were bump bonded to unirradiated readout chips and tested using high energy pions in the H2 beam line of the CERN SPS. The readout chip allows a nonzero suppressed full analogue readout and therefore a good characterization of the sensors in terms of noise and charge collection properties. The position dependence of signal is presented and the differences between the two sensor options are discussed.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2003
Rudolf Frühwirth; K. Prokofiev; T. Speer; P. Vanlaer; Wolfgang Waltenberger
Abstract Presently, two kinds of least-squares (LS) vertex fits are implemented in the ORCA reconstruction program ( http://cmsdoc.cern.ch/orca ) of the CMS experiment ( http://cmsinfo.cern.ch ): a full Kalman filter, and an iterative fit working with the impact points of the tracks with respect to an expansion point. In this contribution we concentrate on nonlinear, robust estimators which are insensitive to outlying observations. The aim is to improve the recognition of outliers, to lower the bias in the final fit, and to achieve a better separation between primary vertices and secondary vertices. Robust vertex estimates should also be good starting points for more complex algorithms, such as a multivertex fit.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2005
Tilman Rohe; D. Bortoletto; V. Chiochia; L. Cremaldi; S. Cucciarelli; A. Dorokhov; Ch. Hörmann; D. Kim; M. Konecki; Danek Kotlinski; K. Prokofiev; C. Regenfus; David A Sanders; S. Son; T. Speer; M. Swartz
Abstract The barrel region of the CMS pixel detector will be equipped with “n-in-n” type silicon sensors. They are processed on diffusion oxygenated float zone (DOFZ) material, use the moderated p-spray technique for inter pixel isolation and feature a bias grid. The latter leads to a small fraction of the pixel area to be less sensitive to particles. In order to quantify this inefficiency prototype pixel sensors irradiated to particle fluences between 4.7 × 10 13 and 2.6 × 10 15 n eq / cm 2 have been bump bonded to un-irradiated readout chips and tested using high energy pions at the H2 beam line of the CERN SPS. The readout chip allows a non-zero suppressed analog readout and is therefore well suited to measure the charge collection properties of the sensors. In this paper we discuss the fluence dependence of the collected signal and the particle detection efficiency. Further the position dependence of the efficiency is investigated.
ieee nuclear science symposium | 2001
W. Ashmanskas; A. Barchiesi; A. Bardi; M. Bari; M. Baumgart; S. Belforte; A. Belloni; J. Berryhill; Mircea Bogdan; R. Carosi; A. Cerri; G. Chlachidze; R. Culberston; M. Dell'Orso; S. Donati; I. Fiori; Henry J. Frisch; S. Galeotti; P. Giannetti; V. Glagolev; Yanwen Liu; E. Meschi; L. Moneta; F. Morsani; T. Nakaya; D. Passuello; G. Punzi; A. Rescigno; L. Ristori; H. Sanders
The Online Silicon Vertex Tracker (SVT) is the new trigger processor dedicated to the 2-D reconstruction of charged particle trajectories at the Level 2 of the CDF trigger. The SVT links the digitized pulse heights found within the Silicon Vertex detector to the tracks reconstructed in the Central Outer Tracker by the Level 1 Fast Track finder. Preliminary tests of the system took place during the October 2000 commissioning run of the Tevatron Collider. During the April-October 2001 data taking SVT was fully assembled and it was possible to obtain clearer and more important results on the performance of the system. In this paper we review the tracking algorithms implemented in the SVT and we report on the performance achieved during the early phase of run II.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2006
V. Chiochia; M. Swartz; Y. Allkofer; D. Bortoletto; L. Cremaldi; S. Cucciarelli; A. Dorokhov; Ch. Hörmann; D. Kim; M. Konecki; Danek Kotlinski; K. Prokofiev; C. Regenfus; Tilman Rohe; David A Sanders; S. Son; T. Speer
In this paper, we discuss the measurement of charge collection in irradiated silicon pixel sensors and the comparison with a detailed simulation. The simulation implements a model of radiation damage by including two defect levels with opposite charge states and trapping of charge carriers. The modeling proves that a doubly peaked electric field generated by the two defect levels is necessary to describe the data and excludes a description based on acceptor defects uniformly distributed across the sensor bulk. In addition, the dependence of trap concentrations upon fluence is established by comparing the measured and simulated profiles at several fluences and bias voltages.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2006
A. Dorokhov; Y. Allkofer; C. Amsler; D. Bortoletto; V. Chiochia; L. Cremaldi; S. Cucciarelli; Ch. Hörmann; D. Kim; M. Konecki; Danek Kotlinski; K. Prokofiev; C. Regenfus; Tilman Rohe; David A Sanders; S. Son; T. Speer; M. Swartz
A new method for the extraction of the electric field in the bulk of heavily irradiated silicon pixel sensors is presented. It is based on the measurement of the Lorentz deflection and mobility of electrons as a function of depth. The measurements were made at the CERN H2 beam line, with the beam at a shallow angle with respect to the pixel sensor surface. The extracted electric field is used to simulate the charge collection and the Lorentz deflection in the pixel sensor. The simulated charge collection and the Lorentz deflection is in good agreement with the measurements both for non-irradiated and irradiated up to 1E15 neq/cm2 sensors.