Peter Weilhammer
Ohio State University
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Featured researches published by Peter Weilhammer.
Nuclear Instruments and Methods in Physics Research | 1983
E. Belau; R. Klanner; G. Lutz; E. Neugebauer; H.J. Seebrunner; Andrew Wylie; T. Böhringer; L. Hubbeling; Peter Weilhammer; Josef Kemmer; U. Kötz; M. Riebesell
Abstract The charge collection in silicon detectors has been studied, by measuring the response to high-energy particles of a 20 μ pitch strip detector as a function of applied voltage and magnetic field. The results are well described by a simple model. The model is used to predict the spatial resolution of silicon strip detectors and to propose a detector with optimized spatial resolution.
Physics in Medicine and Biology | 2004
A. Braem; M Chamizo Llatas; E. Chesi; J. G. Correia; F Garibaldi; C. Joram; S Mathot; E. Nappi; M Ribeiro da Silva; F Schoenahl; J. Séguinot; Peter Weilhammer; Habib Zaidi
A novel concept for a positron emission tomography (PET) camera module is proposed, which provides full 3D reconstruction with high resolution over the total detector volume, free of parallax errors. The key components are a matrix of long scintillator crystals and hybrid photon detectors (HPDs) with matched segmentation and integrated readout electronics. The HPDs read out the two ends of the scintillator package. Both excellent spatial (x, y, z) and energy resolution are obtained. The concept allows enhancing the detection efficiency by reconstructing a significant fraction of events which underwent Compton scattering in the crystals. The proof of concept will first be demonstrated with yttrium orthoaluminate perovskite (YAP):Ce crystals, but the final design will rely on other scintillators more adequate for PET applications (e.g. LSO:Ce or LaBr3:Ce). A promising application of the proposed camera module, which is currently under development, is a high resolution 3D brain PET camera with an axial field-of-view of approximately 15 cm dedicated to brain research. The design philosophy and performance predictions based on analytical calculations and Monte Carlo simulations are presented. Image correction and reconstruction tools required to operate this transmissionless device in a research environment are also discussed. Better or similar performance parameters were obtained compared to other known designs at lower fabrication cost. The axial geometrical concept also seems to be promising for applications such as positron emission mammography.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1994
A. Holmes-Siedle; M. Robbins; S. Watts; Phillip Allport; R. Brenner; H.G. Moser; S. Roe; J. Straver; Peter Weilhammer; P. Chochula; I. Mikulec; S. Moszczynski; M. Turala; W. Dabrowski; P. Grybos; M. Idzik; D. Loukas; K. Misiakos; I. Siotis; K. Zachariadou; W. Dulinski; J. Michele; M. Schaeffer; R. Turchetta; P.S.L. Booth; J. Richardson; N.A. Smith; K. Gill; G. Hall; R. Sachdeva
Abstract The RD20 collaboration is investigating the design and operation of an LHC inner tracking detector based on silicon microstrips. Measurements have been made on prototype detectors after irradiation with electrons, neutrons, photons, and protons for doses up to 5 Mrad and fluences up to 10 15 particles/cm 2 . The annealing of effective doping changes caused by high neutron fluences, one of the major limits to detector lifetime at the LHC, is shown to be strongly inhibited by cooling below room temperature. Detailed results are presented on the critical issue of microstrip capacitance. We have also investigated bulk damage caused by high-energy protons, interstrip isolation after neutron irradiation, and MOS capacitors irradiated with electrons and photons.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1990
V. Chabaud; H. Dijkstra; M. Gröne; Michael Flohr; R. Horisberger; L. Hubbeling; G. Maehlum; A. Peisert; Anders W. Sandvik; Peter Weilhammer; A. Czermak; Pawel Jalocha; P. Kapusta; M. Turala; A. Zalewska; E. Sundell; T. Tuuva; M. Battaglia; M. Caccia; W. Kucewicz; C. Meroni; N. Redaelli; R. Turchetta; A. Stocchi; C. Troncon; G. Vegni; G. Barichello; M. Mazzucato; M. Pegoraro; F. Simonetto
Abstract Results are presented from a test in the CERN SPS North Area of a prototype of the DELPHI microvertex detector. Full-sized modules built up from prototype ac-coupled detectors and VLSI readout electronics were used. The spatial resolution of the detectors equipped with prototype VLSI chips was measured to be 6.5 μm. The system aspects, including the readout, were found to work well. Extrapolating to the final components we expect to achieve a measurement precision of 5 μm with the DELPHI microvertex detector.
Physics in Medicine and Biology | 2007
Sang June Park; W. Leslie Rogers; Sam S. Huh; H. Kagan; K. Honscheid; D. Burdette; E. Chesi; C. Lacasta; G. Llosa; Marko Mikuz; A. Studen; Peter Weilhammer; Neal H. Clinthorne
A very high resolution positron emission tomography (PET) scanner for small animal imaging based on the idea of inserting a ring of high-granularity solid-state detectors into a conventional PET scanner is under investigation. A particularly interesting configuration of this concept, which takes the form of a degenerate Compton camera, is shown capable of providing sub-millimeter resolution with good sensitivity. We present a Compton PET system and estimate its performance using a proof-of-concept prototype. A prototype single-slice imaging instrument was constructed with two silicon detectors 1 mm thick, each having 512 1.4 mm x 1.4 mm pads arranged in a 32 x 16 array. The silicon detectors were located edgewise on opposite sides and flanked by two non-position sensitive BGO detectors. The scanner performance was measured for its sensitivity, energy, timing, spatial resolution and resolution uniformity. Using the experimental scanner, energy resolution for the silicon detectors is 1%. However, system energy resolution is dominated by the 23% FWHM BGO resolution. Timing resolution for silicon is 82.1 ns FWHM due to time-walk in trigger devices. Using the scattered photons, time resolution between the BGO detectors is 19.4 ns FWHM. Image resolution of 980 microm FWHM at the center of the field-of-view (FOV) is obtained from a 1D profile of a 0.254 mm diameter (18)F line source image reconstructed using the conventional 2D filtered back-projection (FBP). The 0.4 mm gap between two line sources is resolved in the image reconstructed with both FBP and the maximum likelihood expectation maximization (ML-EM) algorithm. The experimental instrument demonstrates sub-millimeter resolution. A prototype having sensitivity high enough for initial small animal images can be used for in vivo studies of small animal models of metabolism, molecular mechanism and the development of new radiotracers.
Radiation Protection Dosimetry | 2010
A. Studen; D. Burdette; E. Chesi; V. Cindro; Neal H. Clinthorne; E. Cochran; Borut Grosicar; H. Kagan; C. Lacasta; Vladimir Linhart; M. Mikuž; Vera Stankova; Peter Weilhammer; D. Žontar
Simulation indicates that PET image could be improved by upgrading a conventional ring with a probe placed close to the imaged object. In this paper, timing issues related to a PET probe using high-resistivity silicon as a detector material are addressed. The final probe will consist of several (four to eight) 1-mm thick layers of silicon detectors, segmented into 1 x 1 mm(2) pads, each pad equivalent to an independent p + nn+ diode. A proper matching of events in silicon with events of the external ring can be achieved with a good timing resolution. To estimate the timing performance, measurements were performed on a simplified model probe, consisting of a single 1-mm thick detector with 256 square pads (1.4 mm side), coupled with two VATAGP7s, application-specific integrated circuits. The detector material and electronics are the same that will be used for the final probe. The model was exposed to 511 keV annihilation photons from an (22)Na source, and a scintillator (LYSO)-PMT assembly was used as a timing reference. Results were compared with the simulation, consisting of four parts: (i) GEANT4 implemented realistic tracking of electrons excited by annihilation photon interactions in silicon, (ii) calculation of propagation of secondary ionisation (electron-hole pairs) in the sensor, (iii) estimation of the shape of the current pulse induced on surface electrodes and (iv) simulation of the first electronics stage. A very good agreement between the simulation and the measurements were found. Both indicate reliable performance of the final probe at timing windows down to 20 ns.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1989
M. Burns; H. Dijkstra; R. Horisberger; L. Hubbeling; B. Hyams; G. Maehlum; A. Peisert; J.P. Vanuxem; Peter Weilhammer; A. Zalewska; W. Krupinski; H. Palka; M. Turala; T. Palenius; E. Sundell; T. Tuuva; M. Caccia; W. Kucewicz; C. Meroni; M. Pegoraro; N. Redaelli; R. Turchetta; A. Stocchi; C. Troncon; G. Vegni; M. Mazzucato; F. Simonetto; G. Zumerle; Phillip Allport; G. Kalmus
Abstract The design and progress in the construction of the DELPHI microvertex detector are presented. The layout is described, together with results on precision mounting of silicon detectors. The development of ac-coupled silicon microstrip detectors was an important contribution to the design. The use of low-power CMOS readout chips facilitates the cooling of the detector. A description of the fourth-generation readout processor for silicon strip detectors, the SIROCCO IV, implemented in FASTBUS, is given. Finally, two complementary systems for in-situ position monitoring of the detectors are described.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1996
Peter Weilhammer; E. Chesi; Wladyslaw Dabrowski; W. Dulinski; J.P. Jobez; J. Kaplon; P. Martinengo; Einar Nygard; P. Riedler; S. Roe; J. Séguinot; T. Ypsilantis
Abstract Si pad sensors with 256 cells have been used to detect single photoelectrons from a CsI photocathode. These sensors are part of a Hybrid Photon Detector (HPD) to be used in a RICH detector in the LHC-B experiment. The I - V and C - V measurements are presented. The pad sensors are read out with the low-noise VA2 chip. Results from tests with these detectors with a 90 Sr source are reported. Measurements of photoelectrons created by 160 nm wavelength photons in a CsI cathode in a test set-up are also reported. Finally, the prospects of using such sensors with fast LHC readout electronics are discussed.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2003
W. Adam; E. Berdermann; P. Bergonzo; W. de Boer; F. Bogani; E. Borchi; A. Brambilla; M. Bruzzi; C. Colledani; J. Conway; P. D’Angelo; W. Dabrowski; P. Delpierre; J. Doroshenko; W. Dulinski; B. Van Eijk; A. Fallou; P. Fischer; F. Fizzotti; C. Furretta; K. K. Gan; N. Ghodbane; E. Grigoriev; G. Hallewell; S. Han; F. Hartjes; J. Hrubec; D. Husson; H. Kagan; J. Kaplon
Abstract Diamond is a promising sensor material for future collider experiments due to its radiation hardness. Diamond pixel sensors have been bump bonded to an ATLAS pixel readout chip using PbSn solder bumps. Single chip devices have been characterised by lab measurements and in a high-energy pion beam at CERN. Results on charge collection, spatial resolution, efficiency and the charge carrier lifetime are presented.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1999
Peter Weilhammer
Abstract Ring Imaging Cherenkov detectors will be the backbone of future experiments searching for direct CP violation in B decays. Highly efficient photodetectors are important for a good RICH performance. VLSI front-end ASICs are developed for the readout of high-granularity photodetectors. Design criteria and performance requirements for such front ends are discussed. Some examples of applications and results on performance of several chips are presented.