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Dr Maria Margherita Obertino (Universita' del Piemonte Orientale)24/05/2012, 13:31P5 - Solid State DetectorsPosterSilicon 3D detectors consist of an array of columnar electrodes (radius โผ 5ยตm) of both doping types which penetrate entirely in the detector bulk, perpendicularly to the surface. This structure decouples the electrode distance from the sensor substrate thickness. The close electrode spacing provides several advantages compared to the planar sensor design: low full depletion voltage (โผ 10 V),...Go to contribution page
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Prof. Anna Di Ciaccio (INFN ROMA Tor Vergata and University)24/05/2012, 13:31P5 - Solid State DetectorsPosterCVD diamond particle detectors are presently in use in the CERN experiments ATLAS, CMS, LHCb and ALICE and at particle accelerator laboratories in USA and Japan. This is a proven technology with very fast signal read-out and a very high radiation tolerance suitable for measurements in high radiation environment zones. The properties of CVD diamonds make them a prime candidate for measuring...Go to contribution page
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Dr Stefano Zucca (Universitร di Pavia)24/05/2012, 13:31P5 - Solid State DetectorsPosterApsel4well is a chip prototype intended for application to the Layer0 of the SuperB SVT. Physics studies set stringent requirements on the Layer0 design: radius of about 1.5 cm, high granularity (50 ฮผm pixel pitch), fast readout techniques to comply with a high background rate, low material budget and an adequate radiation resistance. The considered approach is based on a planar 180 nm CMOS...Go to contribution page
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Prof. Gianvito Matarrese (DEE - Politecnico di Bari)24/05/2012, 13:31P5 - Solid State DetectorsPosterThe shape of the current pulse produced by a SiPM in response to an incident photon is affected by the characteristics of the FE used to read out the detector. Thus, an accurate modeling of the SiPM is mandatory to identify the best solutions for the architecture and the most relevant design parameters of the FE electronics. When the application requires to approach the best theoretical time...Go to contribution page
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Mr Jonathan Stahlman (University of Pennsylvania)24/05/2012, 13:31P5 - Solid State DetectorsPosterThe ATLAS detector is equipped with a tracking system (Inner Detector) built using different technologies: silicon planar sensors (pixel and microstrip) and gaseous drift-tubes, all embedded in a 2T solenoidal field. Quality tracking requires to determine its almost 700,000 geometrical degrees of freedom (DoF) with high accuracy. ATLAS physics goals require high resolution, unbiased...Go to contribution page
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Peter Lundgaard Rosendahl (University of Bergen (NO))24/05/2012, 13:31P5 - Solid State DetectorsPosterThe Semi-Conductor Tracker (SCT) is a silicon strip detector and one of the key precision tracking devices in the Inner Detector of the ATLAS experiment at CERN LHC. In the talk the current status of the SCT will be reviewed. We will report on the operation of the detector including an overview of the issues we encountered and the observation of signi๏ฌcant increases in leakage currents (as...Go to contribution page
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Dr Andrej Gorisek (J. Stefan Institute, Ljubljana)24/05/2012, 13:31P5 - Solid State DetectorsPosterBeam conditions and the potential detector damage resulting from their anomalies have pushed the LHC experiments to build their own beam monitoring devices. The ATLAS Experiment decided to build two independent systems based on Chemical Vapor Deposition (CVD) diamond material. The ATLAS Beam Conditions Monitor (BCM) consists of two stations (forward and backward) of detectors each with four...Go to contribution page
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Laura Fabbri (INFN - Bologna)24/05/2012, 13:31P5 - Solid State DetectorsPosterThe SuperB Silicon Vertex Tracker will be made of 5 layers of double sided silicon strip sensors plus an additional innermost layer (Layer0) at a radius of about 1.5 cm, very close to the beam pipe. For the first phase of the experiment the baseline option for the Layer0 is a high resistivity thin (200 $\mu$m) double sided silicon detector, with short strips ("Striplets") at 45ยฐ angle to...Go to contribution page
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Dr Mauro Menichelli (INFN Sez. di Perugia)24/05/2012, 13:31P5 - Solid State DetectorsPosterPixel sensors have been calibrated using both fluorescence X-ray photons and a narrow X-ray beam obtained by transmission technique. The X-rays were generated by a Amptek EDIX 40 X-ray tube (Maximum voltage 40 kV). During the fluorescence calibration the pixel sensor was placed in front of the target in a off-beam position, the resulting photons hitting the detector were emitted by...Go to contribution page
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Dr Gianpiero Gervino (Dipartimento di Fisica and INFN Torino)24/05/2012, 13:31P5 - Solid State DetectorsPosterWe report for several tests carried on Chemical Vapour Deposition (CVD) diamonds to be used as ionizing radiation detectors. The unique properties of diamond makes it one of the most promising wide band-gap materials not only in the already established field of high luminosity X-ray detection for medical applications but also in modern high energy physics. CVD diamonds can be built in two...Go to contribution page
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Dr Irina Rashevskaya (INFN โ Sezione di Trieste)24/05/2012, 13:31P5 - Solid State DetectorsPosterThe Silicon Vertex Tracker for the SuperB detector will be an evolution of the BaBar SVT, based on double-sided strip detectors. The wider acceptance in polar angle (down to 300 mr) will entail larger incidence angles (up to 73 degrees) on the sensors and a larger number of z-side strips. For optimum performance it would be desirable to continuously vary the sensor pitch on z-side versus...Go to contribution page
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Dr Petra Merkel (Purdue University)24/05/2012, 13:31P5 - Solid State DetectorsPosterThe CMS silicon pixel and strip tracker is at the core of every physics analysis in CMS. We present its performance during the first three years of LHC data taking. From the monitoring of its basic observables to the vertexing and tracking performance at analysis level we give a broad overview of the tracker's behavior. Special focus will be put on the dependence of its performance on the...Go to contribution page
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Prof. Norbert Wermes (University of Bonn)24/05/2012, 13:31P5 - Solid State DetectorsPosterMeasurements on irradiated diamond pixel detectors (poly-crystalline and single crystal) equipped with the ATLAS FE-I4 pixel readout chip are confronted with similar silicon pixel detectors regarding their performance at high radiation fluences as expected at an HL-LHC. Within the competition of CVD diamond detectors with silicon the question of the expected S/N โ ratio (SNR) after...Go to contribution page
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Prof. Arie Ruzin (Tel Aviv University)24/05/2012, 13:31P5 - Solid State DetectorsPosterThe issue of contacts to high resistivity semiconductors in general and to II-VI group, in particular, has always been a great challenge. Such is the case for semiconductor radiation detectors based on CdTe and Cd1-xZnxTe. Interpretation of experimental results is always based on some physical model of the device. Thus, incorrect modeling is bound to lead to misleading conclusions. In modeling...Go to contribution page
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Mr Maurizio Boscardin (FBK)24/05/2012, 13:31P5 - Solid State DetectorsPosterThe foreseen luminosity of the new experiments in High Energy Physics will require that the next generation of vertex detectors will be able to sustain fluencies up to $1\times10^{16}$ cm$^{โ2}$. Moreover, in many experiments there is a demand for the minimization of the material budget of the detectors. Therefore, thin pixel devices on epitaxial material are a natural choice to fulfill these...Go to contribution page
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Dr Claudio Piemonte (Fondazione Bruno Kessler)24/05/2012, 13:31P5 - Solid State DetectorsPosterIn the framework of the HyperImage and Sublima EU projects we are developing a SiPM-based high-performance TOF-PET system to be integrated in a MRI. It has already been shown that single-element FBK SiPMs coupled to LYSO scintillator and read out by an optimized discrete circuit provide excellent energy and timing information. In this paper we demonstrate that a very good performance can be...Go to contribution page
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Dr Alessandro Tarolli (Fondazione Bruno Kessler)24/05/2012, 13:31P5 - Solid State DetectorsPosterIn this contribution we show selected results on the first release of UV-enhanced SiPM technology (NUV-SiPM) produced at FBK. In particular, we focus our attention on the photo-detection efficiency (PDE) performance. The PDE in the near-UV part of the light spectrum is mainly limited by the quantum efficiency term since the photo-generation takes place in a very shallow region of the silicon....Go to contribution page
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Mr Marco Povoli (Universitร di Trento/INFN)24/05/2012, 13:31P5 - Solid State DetectorsPosterIn the framework of our R&D activities oriented to 3D detectors, which finally led to the first production for the ATLAS Insertable B layer, we have also developed planar sensors with active edge. First proposed by C. Kenney et al., this type of edge termination consists of a deep trench etched all around the active area and doped as an ohmic electrode. One batch of these devices was...Go to contribution page
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Prof. Gian-Franco Dalla Betta (University of Trento and INFN and RSENS)24/05/2012, 13:31P5 - Solid State DetectorsPosterA battery-powered, wireless Radon sensor has been designed and realized using a Bipolar Junction Transistor a radiation detector fabricated on a high-resistivity-silicon substrate. Radon daughters are collected on the detector surface electrostatically. Thanks to the BJT excellent signal-to-noise ratio and internal amplification, real-time alpha particle detection is possible using a simple...Go to contribution page
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Dr Fabian Huegging (University of Bonn)24/05/2012, 13:31P5 - Solid State DetectorsPosterChemical Vapour Deposition (CVD) diamond has a number of properties that make it an attractive alternative for high energy physics detector applications like tracking detectors, luminosity monitors and beam monitors. Its large band-gap (5.5 eV) and large displacement energy (42 eV/atom) make it a material that is inherently radiation tolerant with very low leakage currents and high thermal...Go to contribution page
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Prof. Peter Fischer (Heidelberg University)24/05/2012, 13:31P5 - Solid State DetectorsPosterWe present the novel {\bf I}nterpolating {\bf Si}licon {\bf P}hoto{\bf M}ultiplier (ISiPM) topology which provides the spatial position of photon clusters with high resolution. Individual APD cells of the ISiPM area are not connected to a {\em common} readout electrode, but each cell is connected to {\em one of several} output channels. The most straight forward embodiment is a...Go to contribution page
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Dr Mark Cooke (LBNL)24/05/2012, 13:31P5 - Solid State DetectorsPosterThe record breaking instantaneous luminosities of $10^{33} cm^{-2} s^{-1}$ recently surpassed at the Large Hadron Collider generate a rapidly increasing particle fluence in the ATLAS Pixel Detector. As the radiation dose accumulates, the first effects of radiation damage are now observable in the silicon sensors. A regular monitoring program has been conducted and reveals an increase in the...Go to contribution page
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Ms Karoline Selbach (University of Edinburgh)24/05/2012, 13:31P5 - Solid State DetectorsPosterThe read-out from individual pixels on planar semi-conductor sensors are grouped into clusters to reconstruct the location where a charged particle passed through the sensor. The resolution given by individual pixel sizes is significantly improved by using the information from the charge sharing between pixels. Such analog cluster creation techniques have been used for many years to obtain an...Go to contribution page
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Mr Benoรฎt Caylar (CEA-LIST, Diamond Sensor Laboratory)24/05/2012, 13:31P5 - Solid State DetectorsPosterIn order to push forward the state-of-the art of device radiation hardness, we propose to use so called 3D electrode geometry: where the collecting electrodes are implemented within the bulk of the diamond and separated by a few tens of microns (limited by the processing techniques). The reduced distance between the buried electrodes enables higher electric fields to be applied, thus faster...Go to contribution page
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Alessandro La Rosa (DPNC, Universitรฉ de Geneve)24/05/2012, 13:31P5 - Solid State DetectorsPosterIn view of the LHC upgrade phases towards HL-LHC the ATLAS experiment plans to upgrade the Inner Detector with an all silicon system.\\ The n-in-p silicon technology is a promising candidate for the pixel upgrade thanks to its radiation hardness and cost effectiveness, that allow for enlarging the area instrumented with pixel detectors.\\ We present the characterization and performance of...Go to contribution page
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Mr Iurii Sorokin (Goethe University Frankfurt)24/05/2012, 13:31P5 - Solid State DetectorsPosterThe goal of the Compressed Baryonic Matter~(CBM) experiment is study the phase diagram of strongly interacting matter at high baryonic densities. It is going to be done by colliding proton and heavy ion beams of energy up to 35~AGeV with fixed carbon and heavy element targets. The physics program of the experiment requires to reconstruct all charged products, measure their momenta with high...Go to contribution page
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Mr David Dossett (University of Warwick)24/05/2012, 13:31P5 - Solid State DetectorsPosterLHCb is a dedicated experiment to study new physics in the decays of beauty and charm hadrons at the Large Hadron Collider (LHC) at CERN. The beauty and charm hadrons are identified through their flight distance in the Vertex Locator (VELO), and hence the detector is critical for both the trigger and offline physics analyses. The VELO is the highest resolution vertex detector at the...Go to contribution page
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Mr Christian Gallrapp (CERN)24/05/2012, 13:31P5 - Solid State DetectorsPosterThe ATLAS Planar Pixel Sensor (PPS) R&D Project is a collaboration of 17 institutes and more than 80 scientists, started to explore the feasibility of employing planar pixel sensors for the upgraded tracker at HL-LHC. Different pixel concepts are investigated for the inner and outer layers. In the first case the focus is on extreme radiation hardness, with the use of very thin pixel sensors...Go to contribution page
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Mr David Dossett (University of Warwick)24/05/2012, 13:31P5 - Solid State DetectorsPosterThe VELO is the silicon detector surrounding the LHCb interaction point. The sensors have an inner radius of only 7mm from the LHC beam and an outer radius of 42 mm. Consequently the sensors receive a large and non-uniform radiation dose. A dose of $0.5\times10^{13}$ 1 MeV neutron equivalents /cm$^2$ per fb$^{-1}$ of data is predicted at the tip of the sensors. The sensors are fabricated...Go to contribution page
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Mr Alberto Potenza (Torino University)24/05/2012, 13:31P5 - Solid State DetectorsPosterThe LePix project aims at developing monolithic detectors integrating reverse biased detecting diodes and readout circuitry in 90 nm CMOS. In this framework we are investigating the radiation tolerance of the base material, which is an order of magnitude more doped than standard high resistivity detectors, and which underwent the full advanced CMOS process. This investigation is carried out...Go to contribution page
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Dr Daniele M. Trucchi (CNR-IMIP)24/05/2012, 13:31PosterSeveral medical applications rely on the interaction between high-energy radiation and human tissue. Radiotherapy, radiography, and mammography as well as high-energy physics experiments need a very precise measurement of the radiation dose imparted to the target volume. These techniques differ in the radiation energy content, but all of them require reliable, precise, and sensitive detectors...Go to contribution page
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Mr Maurizio Boscardin (FBK)24/05/2012, 13:31P5 - Solid State DetectorsPosterThe support and cooling structures add an important contribution to the total material of vertex detectors. In order to minimize the material budget of pixel sensors, we developed a new approach to integrate the cooling - into the silicon devices โ based on the microchannel technology. The microchannels are formed in silicon using isotropic SF6 plasma etching in a DRIE (deep reactive ion...Go to contribution page
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Mr Xiaopeng Wu (VTT)24/05/2012, 13:31P5 - Solid State DetectorsPosterSilicon Sensor Alliance (SSA) gathers European institutes together to answer for the large need of silicon sensors for CERNโs LHC upgrade. Currently more than 90% of the LHCโs sensors were fabricated outside European countries. The aim of the SSA is to be a qualified and reliable union in Europe to manufacture and provide uniform and high quality radiation detectors to meet the requirement of...Go to contribution page
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Dr Dean Andrew Hidas (Rutgers/CERN)24/05/2012, 13:31P5 - Solid State DetectorsPosterThe Pixel Luminosity Telescope (PLT) is a compact single-crystal diamond pixel based tracking detector. The PLT is designed to measure both the instantaneous luminosity and the relative bunch-to-bunch luminosity with high precision and speed at CMS at the much higher instantaneous luminosities the LHC will provide starting in 2015. One quarter of the full detector has been installed in a...Go to contribution page
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Dr Andrea Favareto (INFN - Milano)24/05/2012, 13:31P5 - Solid State DetectorsPosterThe ATLAS Pixel Detector is the innermost detector of the ATLAS experiment at the Large Hadron Collider at CERN, providing high-resolution measurements of charged particle tracks in the high radiation environment close to the collision region. This capability is vital for the identification and measurement of proper decay times of long-lived particles such as b-hadrons, and thus vital for the...Go to contribution page
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Dr Lorenzo Uplegger (Fermilab)24/05/2012, 13:31P5 - Solid State DetectorsPosterDiamond sensors are studied as an alternative to silicon sensors to withstand the high radiation doses that are expected in future upgrades of the pixel detectors for the SLHC. Diamond pixel sensors are intrinsically radiation hard and are considered as a possible solution for the innermost tracker layers close to the interaction point where current silicon sensors cannot cope with the harsh...Go to contribution page
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Dr Ashutosh Bhardwaj (University of Delhi)24/05/2012, 13:31P5 - Solid State DetectorsPosterThe CMS all-silicon tracker consists of 16588 modules. Aligning these with the desired precision of a few micrometers is only feasable using track based alignment procedures. Ultimate local precision is now achieved by the determination of sensor curvatures. This faces the algorithms with about 200k parameters to be calculated simultaneously. This can be well handled using the Millepede II...Go to contribution page
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Peter Kodys (Charles University)24/05/2012, 13:31P5 - Solid State DetectorsPosterDetectors for experiments at future colliders โ e.g. the Super B-factories or the ILC โ require excellent vertexing performance for the layers close to primary interaction region. These detectors need to enable excellent vertex reconstruction, achievable by a highly granular pixel detector, together with fast readout and minimum material budget to reduce the impact on the measurement due to...Go to contribution page
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Mr Filippo Bosi (INFN Pisa)24/05/2012, 13:31P5 - Solid State DetectorsPosterPixel detectors require that high power density in the sensitive area should be carried away by thermal systems, eventually integrated in the light mechanical support structures. The micro-channel cooling technology is characterized by a highly efficient thermal exchange. It can profit of the miniaturization techniques employed on composite materials, allowing important advantage in terms of...Go to contribution page
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Mr Michael Deveaux (Goethe University Frankfurt)24/05/2012, 13:31P5 - Solid State DetectorsPosterThe Compressed Baryonic Matter Experiment (CBM) is one of the core experiments of the future FAIR facility at Darmstadt/Germany. The experiment will explore the phase diagram of hadronic matter in the regime of highest baryon densities. Nuclear fireballs created in heavy ion collisions of 8-45 AGeV beam energy will be studied with numerous probes, among them open charm. Reconstructing those...Go to contribution page
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Mr Christopher Heidt (University of California Riverside)24/05/2012, 13:31P5 - Solid State DetectorsPosterThe Muon Ionization Cooling Experiment (MICE) will be the first experiment to demonstrate muon ionization cooling in the momentum range of 140 MeV/c < p$_{\mu}$ < 240 MeV/c. The experiment is a single-particle experiment where the input and output beam emittances are made from an ensemble of selected single-muon candidates. The two fiber trackers in a solenoidal field of 4T (one before and...Go to contribution page
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Dr Federico Meloni (University of Milano and INFN)24/05/2012, 13:31P5 - Solid State DetectorsPosterThe track and vertex reconstruction algorithms of the ATLAS Inner Detector have demonstrated excellent performance in the early data from the LHC. However, the rapidly increasing number of interactions per bunch crossing introduces new challenges both in computational aspects and physics performance. The combination of both silicon and gas based detectors provides high precision...Go to contribution page
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Mr Christian Koffmane (Max-Planck-Institut fรผr Physik)24/05/2012, 13:31P5 - Solid State DetectorsPosterPrototype DEPFET active pixel sensors designed for the vertex detector at the Belle-II experiment at KEK, Japan, and for experiments at a future linear collider have been produced on thin silicon-on-insulator (SOI) material. The DEPFET (DEpleted P-channel FET) is field effect transistor with an additional implantation beneath the transistorโs channel integrated on a fully depleted substrate....Go to contribution page
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Alexandre Rachevski (INFN - Trieste)24/05/2012, 13:31P5 - Solid State DetectorsPosterUsing $^{55}$Fe and $^{241}$Am sources we characterized the spectroscopic performance of a matrix of Silicon Drift Diodes (SDD). The matrix consists of a completely depleted volume of silicon wafer subdivided into 5 identical hexagonal cells. The back side is 5 implanted arrays of increasingly negatively biased concentric p+ rings. The front side, common to all 5 cells, is a shallow and...Go to contribution page
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