Dr
Adrian Fiergolski
(CERN)
03/02/2016, 09:30
The vertex- and tracking detectors at the proposed high-energy CLIC electron-positron collider will be based on small-pitch silicon pixel- or strip detectors. Time stamping with an accuracy of approximately 10 ns is required to suppress hits from beam-induced backgrounds. Tests with particle beams are needed to assess the performance of existing and future prototype assemblies. To this end a...
Mr
Lennart Huth
(PI Uni Heidelberg - mu3e)
03/02/2016, 09:50
This talk will give an overview over the MuPix Telescope. After a short introduction, the results from the Mu3e MuPix testbeam campaigns 2015, covering the DESY II, SPS and PSI tetsbeams, focusing on efficiency measurements are presented.
Ms
Dorothea vom Bruch
(Johannes Gutenberg-Universität Mainz)
03/02/2016, 10:10
In the context of the Mu3e experiment, High Voltage Monolithic Active Pixel
Sensors (HV-MAPS) are developed as constituents of a highly efficient tracking
detector with good momentum, vertex and timing resolution. The MuPix HV-MAPS prototypes were arranged in a telescope setup
with four layers as an integration test and for efficiency measurements. For high-rate data taking, fast data...
Dr
Vladimir Cindro
(Jožef Stefan Institute)
03/02/2016, 11:00
The upgrade scenario of the LHC to a luminosity of 1035 cm-2 represents a challenge for development of detector components as well as for their tests after irradiations under realistic conditions. Fluences of fast hadrons above 1016 cm-2 are expected in the most exposed regions of detectors.
Spectra of particles cover a wide range with energies up to tens of GeV.
Irradiation facilities...
Dr
Federico Ravotti
(CERN)
03/02/2016, 11:20
The proton and mixed-field irradiation facilities at the CERN PS East Area (known as IRRAD1 and IRRAD2), have been heavily exploited for irradiation of particle detectors, electronic components and materials since 1992. With the increasing demand of irradiation experiments, and in view of the High-Luminosity upgrade of the CERN Large Hadron Collider (HL-LHC), these facilities suffered of a...
Dr
Alexander Dierlamm
(Karlsruher Institut für Technologie)
03/02/2016, 11:40
At KIT we conduct irradiations with 23MeV protons and X-rays. We present the facilities, irradiation procedures and how to apply. Few examples of performed irradiations will be show as well.
Mr
Branislav Ristic
(CERN / University of Geneva)
03/02/2016, 14:00
In 2014 an ATLAS FE-I4 based telescope was built and operated in various CERN PS and SPS testbeams. The 6 plane system consists of IBL like 150um planar pixel sensors (250x50um2 pitch) which are read out by the RCE DAQ system. This ensures fully synchronized data for FE-I4 compatible devices under test. The telescope triggers itself and allows for defining a region of interest, which...
Mr
Michael Reichmann
(ETHZ)
03/02/2016, 14:20
We present the design, the commissioning, and the performance of a modular pixel telescope, which was equipped with the CMS PSI46v2 pixel chip. The telescope was designed with a primary goal of testing pad and pixel diamond detectors in the high flux beam line at the High Intensity Proton Accelerator in PSI. This beam line is able to provide intensities up to 10 MHz/cm2. The unique features of...
Dr
Jan Dreyling-Eschweiler
(DESY)
03/02/2016, 14:40
This talk will give an overview about the EUDET-type telescopes and its user infrastructure. Hardware components and DUT integration will be presented. Furthermore, a EUDAQ status will be shown as well as ongoing development.
Dr
Andrej Gorisek
(J. Stefan Institute, Ljubljana)
03/02/2016, 15:00
I will present KarTel, a telescope build in Ljubljana and based on Mimosa 26 sensors.
As an illustration of KarTel operation - a novel method will be presented that can be used to investigate the properties of silicon and CVD diamond detectors for High Energy Physics experiments. The method is similar to the already well established E-TCT technique using laser beam. In the proposed method...
Mr
Marcel Stanitzki
(DESY)
03/02/2016, 15:20
The DESY-II Test Beam Facility will resume operations in March 2016
The recent improvements and enhancements of the facility will be highlighted.
Dr
Davide Reggiani
(Paul Scherrer Institut)
03/02/2016, 16:10
This contribution will give an overview of the secondary beam lines of the PSI High Intensity Proton Accelerator (HIPA). Particular emphasis will be given to those facilities currently available for tests. Moreover, the Proton Irradiation Facility (PIF) located at the PSI PROSCAN protontherapy centre will be presented.
Mandy Rominsky
(Fermi National Accelerator Laboratory)
03/02/2016, 16:30
The Fermilab Test Beam Facility is a world class facility for testing and characterizing particle detectors. The facility has been in operation since 2005 and has undergone significant upgrades in the last two years. A second beam line with cryogenic support has been added and the facility has adopted a data acquisition system. The facility also recently added a cosmic telescope test stand and...
Dr
Carsten Hast
(SLAC National Accelerator Laboratory)
03/02/2016, 16:50
In 2015 the Caladium silicon telescope of Carleton University, Canada was loaned to SLAC and installed at the End Station Test Beam facility (ESTB). Caladium is a member of the EUDET/AIDA beam telescopes family and is now available to Users at SLAC. We will present the available infrastructure, DAQ, cooling, moving stages, etc. as well as first results of our commissioning runs.
Dr
Henric Wilkens
(CERN)
03/02/2016, 17:10
The status of the PS/SPS Testbeam Facilities are presented.
Dr
Kenneth Wraight
(University of Glasgow)
04/02/2016, 09:00
The UK has produced a number of pixel sensors based on the FEI4b chip for ATLAS ITk. These sensors vary in pixel dimension and coupling technology. This talk will present progress in characterising these devices, including a comparison of pixel geometries based on cluster parameters and resolution at CERN and DESY testbeams.
Dr
Andreas Nürnberg
(CERN)
04/02/2016, 09:20
Hybrid pixel-detector prototypes with small pitch (25-55 microns) and thin sensors (50-300 microns) are currently under study for the vertex detector at the proposed high-energy CLIC electron-positron collider. Test-beam campaigns with hybrid assemblies of planar and active HV-CMOS sensors on CLICpix ASICs and with active edge sensors on Timepix3 ASICs have been performed at the CERN SPS H6...
Mr
Simon Spannagel
(DESY - CMS)
04/02/2016, 10:00
Based on the strong performance of the LHC accelerator, it is anticipated that peak luminosities of two times the design luminosity of L = 2 x10^34 cm^-2s^-1 are likely to be reached before 2018 and probably significantly exceeded in the so-called Phase I period until 2022. At this higher luminosity and increased hit occupancies the current CMS pixel detector would be subject to severe dead...
Mr
Fabian Foerster
(IFAE Barcelona)
04/02/2016, 10:20
3D FEI4 pixel detectors from the IBL production were non-uniformly irradiated at CERN-PS with 23 GeV protons up to a maximum fluence of 9e15 neq/cm2. The devices have been studied in beam tests at CERN SPS and good efficiencies of >97% have been achieved at the highest fluence already at 170 V. Especially interesting is the option to study a vast range of fluences on a single pixel device due...
Dr
Jens Dopke
(STFC Rutherford Appleton Laboratory)
04/02/2016, 11:10
A description of why and how to re-time test beam data, based on limited length timestamps.
Dr
Carlos Chavez
(University of Sussex)
04/02/2016, 11:50
In this talk I will present plans and future developments of a generic online monitoring system for EUDAQ software package. The current monitoring system of EUDAQ was developed and designed for beam telescopes detectors. We present plans to develop a general purposed monitoring system within EUDAQ that will serve different type of detectors.
Mr
Tobias Bisanz
(Uni Göttingen - ATLAS)
04/02/2016, 12:30
The EUTelescope reconstruction framework will be introduced. Focus is put on recent developments as well as new features which are currently under development.
Tobias Bisanz
(Uni Göttingen - ATLAS)
04/02/2016, 14:20
Mr
Alexander Morton
(University of Glasgow)
05/02/2016, 09:00
A versatile implementation of the GBL algorithm within EUTelescope is introduced. Features of the implementation and current developments are highlighted. Current analyses are briefly described as an aid for further reconstruction work.
Mr
David Vázquez Furelos
(IFAE - Barcelona)
05/02/2016, 09:20
3D pixel sensors before and after irradiation have been tested in the September 2015 ATLAS Pixel testbeam at CERN. Both the latest Eutelescope version and a stable previous release have been used for track reconstruction. This talk will present the experience installing and working with both software versions.
Mr
Alejandro Perez Perez
(IPHC)
05/02/2016, 10:50
The DAFNE Beam Test Facility (BTF) is a beam transfer line optimized to produce single electrons/positrons for detector performances assessment. This contribution will describe the implementation in this facility of an ultra-thin and high spatial resolution beam telescope for the performances assessment of large pixel CMOS sensors designed to instrument the outer layers of an inner tracker.
Dr
Andy Blue
(Univesrity of Glasgow)
05/02/2016, 11:10
A micro-focused (2.5um spot size) 15keV X ray beam has been used to study silicon micro-strip and pixelated detectors that utilise reduced edge or edgeless designs.
Scans were taken across the physical edges of devices to measure the charge collection as well as study the electric field line behaviour.
We will show the methods used for alignment, DAQ integration, triggering and data...
Dr
Hendrik Jansen
(DESY)
05/02/2016, 11:30
The intrinsic resolution of the MIMOSA26 sensors used in the DATURA beam telescope are extracted deploying an iterative method using GBL track fits. The data was taken at the DESY-II test beam facilities. Additionally, the applicability of the Highland formula to electron beams is tested against data.
Mr
Joern Lange
(IFAE Barcelona)
05/02/2016, 11:50
The ATLAS Forward Proton (AFP) project intends to measure protons scattered under a small angle from the ATLAS proton-proton interaction point.
To this end, it is planned to install 3D Silicon pixel and Quartz-Cherenkov time-of-flight detectors 210 m away from the interaction point.
Beam tests with a first unified AFP prototype detector combining tracking and timing sub-detectors and a...
12.
Characterization of thin irradiated epitaxial silicon sensors for the CMS phase II pixel upgrade
Mr
Matteo Centis Vignali
(University of Hamburg)
05/02/2016, 12:10
The high-luminosity upgrade of the Large Hadron Collider, foreseen for 2025, neces-
sitates the replacement of the tracker of the CMS experiment. The innermost layer of
the new pixel detector will be exposed to severe radiation corresponding to a 1 MeV
neutron equivalent fluence up to Φ eq = 2 · 10 16 cm −2 and an ionizing dose of ≈ 10 MGy
after an integrated luminosity of 3000 fb −1 ....
Ms
Elena Dall'Occo
(NIKHEF)
05/02/2016, 12:30
The upgrade of the LHCb experiment, planned for 2019, will transform the experiment
to a trigger-less system reading out the full detector at the LHC collision rate
and up to $2\times 10^{33}cm^{−2} s^{-1}$ instantaneous luminosity.
The Vertex Locator (VELO) is the silicon detector surrounding the interaction region.
The upgraded VELO is based on a hybrid pixel system equipped...
