Daniel Dobos
(CERN)
01/06/2015, 09:10
Clemens Lange
(Universitaet Zuerich (CH))
01/06/2015, 09:40
Domenico Colella
(Universita e INFN, Bari (IT))
01/06/2015, 10:10
Kurt Rinnert
(University of Liverpool (GB))
01/06/2015, 11:10
Stefano Gallorini
(Universita e INFN, Padova (IT))
01/06/2015, 11:40
Richard Bates
(University of Glasgow (GB))
01/06/2015, 13:30
Robert Stringer
(University of Kansas (US))
01/06/2015, 14:00
Sophie Elizabeth Richards
(University of Bristol (GB))
01/06/2015, 14:30
Monika Kofarago
(NIKHEF (NL))
01/06/2015, 15:30
Dr
Zhijun Liang
(University of California,Santa Cruz (US))
01/06/2015, 16:00
Marko Dragicevic
(HEPHY Vienna)
01/06/2015, 16:30
Jianchun Wang
(Syracuse University (US))
01/06/2015, 17:00
Dr
Gene Van Buren
(Brookhaven National Laboratory)
02/06/2015, 09:00
Marca Josep Boronat Arevalo
(Consejo Superior de Investigaciones Cientificas (CSIC)-Universi)
02/06/2015, 09:30
Christoph Schwanda
(Austrian Academy of Sciences)
02/06/2015, 10:00
Lea Michaela Caminada
(Universitaet Zuerich (CH))
02/06/2015, 11:30
Bora Akgun
(Rice University (US))
02/06/2015, 12:00
Chris Kenney
(SLAC)
02/06/2015, 14:00
Alan Litke
(University of California,Santa Cruz (US))
02/06/2015, 14:30
Oliver Kirstein
(European Spallation Source ESS AB)
02/06/2015, 15:00
Prof.
Martin Pohl
(Universite de Geneve (CH))
02/06/2015, 16:00
Eric Charles
(SLAC National Accelerator Laboratory (US))
02/06/2015, 16:30
Angela Gligorova
(University of Bergen (NO))
02/06/2015, 17:00
Abraham Seiden
(University of California,Santa Cruz (US))
03/06/2015, 09:00
Joern Lange
(IFAE Barcelona)
03/06/2015, 09:30
Roberto Mendicino
(UNITN)
03/06/2015, 10:00
Herve Marie Xavier Grabas
(University of California,Santa Cruz (US))
03/06/2015, 11:00
Steven Worm
(STFC - Rutherford Appleton Lab. (GB))
03/06/2015, 11:30
Timo Hannu Tapani Peltola
(Helsinki Institute of Physics (FI))
04/06/2015, 09:00
Marta Baselga Bacardit
(Instituto de Fisica Corpuscular (ES))
04/06/2015, 09:30
Gregor Kasieczka
(Eidgenoessische Tech. Hochschule Zuerich (CH))
04/06/2015, 10:00
Vladimir Cindro
(Jozef Stefan Institute (SI))
04/06/2015, 11:00
Sally Seidel
(University of New Mexico (US))
04/06/2015, 11:30
Szymon Kulis
(CERN)
04/06/2015, 13:30
Marcel Stanitzki
(Deutsches Elektronen-Synchrotron (DE))
04/06/2015, 14:00
Nikolai Sinev
(University of Oregon (US))
04/06/2015, 14:30
Marco De Mattia
(Texas A & M University (US))
04/06/2015, 15:30
Dr
Guido Volpi
(Universita di Pisa & INFN (IT))
04/06/2015, 16:00
Gabriel John Facini
(University of Chicago (US))
04/06/2015, 16:30
Rudolf Fruhwirth
(Austrian Academy of Sciences (AT))
04/06/2015, 17:00
Mauricio Garcia-Sciveres
(Lawrence Berkeley National Lab. (US))
05/06/2015, 09:00
Kurt Rinnert
(University of Liverpool (GB))
05/06/2015, 09:30
Michael Deveaux
(University Frankfurt)
05/06/2015, 10:00
Giulio Dujany
(University of Manchester (GB))
05/06/2015, 11:00
Pierfrancesco Butti
(Nikhef National institute for subatomic physics (NL))
05/06/2015, 11:30
John Stupak
(Purdue University Calumet (US))
05/06/2015, 12:00
Chris Parkes
(University of Manchester (GB))
05/06/2015, 14:00
Dr
Oliver Kirstein
(European Spallation Source)
Neutron scattering science - the study of materials using neutrons - is in an
exciting period, with new large facilities under construction in China (Chinese
Spallation Neutron Source), the US (second target station at the Spallation Neutron
Source) and Europe (European Spallation Source). Additionally, large upgrades in the
numbers of instruments are planned at major facilities in the US,...
Vladimir Cindro
(Jozef Stefan Institute (SI))
Transient Current Technique with a narrow laser beam impinging perpendicularly to the detector edge (Edge-TCT) is a powerful method for investigating properties of silicon detectors. It produces localized ionization in the detector volume. IR light (λ = 1064 nm) has a long penetration depth in silicon and charge carriers are released along the beam path. Drift of electrons and holes can be...
Domenico Colella
(Slovak Academy of Sciences (SK))
The characterization of the Quark-Gluon Plasma (QGP) produced during ultra-relativistic heavy-ion collisions is the main goal of the ALICE experiment at the CERN LHC. The ALICE Inner Tracking System (ITS) plays a key role in the study of the short-living hadrons through the primary and secondary vertex reconstruction. It consists of six cylindrical layers of silicon detectors based on three...
Pierfrancesco Butti
(Nikhef National institute for subatomic physics (NL))
ATLAS is a multipurpose experiment at the LHC proton-proton collider. Its physics goals require high resolution, unbiased measurement of all charged particle kinematic parameters. These critically depend on the layout and performance of the tracking system, notably quality of its offline alignment. ATLAS is equipped with a tracking system built using different technologies, silicon planar...
Prof.
Martin Pohl
(Universite de Geneve (CH))
AMS-02 is a high precision magnetic spectrometer for cosmic rays in the GeV to TeV energy range. Its tracker consists of nine layers of double-sided silicon microstrip sensors. They are used to locate the trajectories of cosmic rays in the 0.14 T field of a cylindrical magnet, thus measuring their rigidity and charge sign. In addition, they deliver a high resolution measurement of the absolute...
Angela Gligorova
(University of Bergen (NO))
AEgIS
(Antimatter
Experiment:
Gravity,
Interferometry,
Spectroscopy)
is
an
antimatter
experiment
based
at
CERN,
whose
primary
goal
is
to
carry
out
the
first
direct
measurement
of
the
Earth’s
gravitational
acceleration
on
antimatter.
AEgIS
will
attempt
to
measure
the
gravitational
acceleration
for
antihydrogen
with
1%
relative
precision,
which
would
...
Dr
Guido Volpi
(Universita di Pisa & INFN (IT))
An overview of the ATLAS Fast Tracker processor is presented, reporting the design of the system, its expected performance, and the integration status. The next LHC runs, with a significant increase in instantaneous luminosity, will provide a big challenge to the trigger and data acquisition systems of all the experiments. An intensive use of the tracking information at the trigger level will...
Dr
Zhijun Liang
(University of California,Santa Cruz (US))
From 2024, the HL-LHC will provide unprecedented pp luminosities to ATLAS, resulting in an additional integrated luminosity of around 2500 fb-1 over ten years. To withstand the much harsher radiation and occupancy conditions of the HL-LHC necessitates a complete replacement of the present ID. The new all-silicon tracker design is driven by the performance requirements that cannot be met by the...
Christoph Schwanda
(Austrian Academy of Sciences)
BELLE II is an experiment in KEK ( Tsukuba, Japan ) that will explore heavy flavour physics (
B, charm and tau ) from early 2018 with unprecedented precision. Charged particles are
tracked ( going from the interaction point to the outside ) by a two-layer DEPFET pixel
device ( PXD ), a four-layer silicon strip detector ( SVD ) and the central drift chamber (
CDC ). The design and the...
Marco De Mattia
(Texas A & M University (US))
The High Luminosity LHC (HL-LHC) is expected to deliver luminosities of 5x10^34 cm^2/s, with an average of about 140 overlapping proton-proton collisions per bunch crossing. These extreme pileup conditions place stringent requirements on the trigger system to be able to cope with the resulting event rates. A key component of the CMS upgrade for HL-LHC is a track trigger system which would...
Robert Stringer
(University of Kansas (US))
In 2023, the LHC will be upgraded to the HL-LHC, increasing the luminosity to 5 x
10^34 cmâ2 sâ1. The increased luminosity will present new challenges in higher data
rates and increased radiation. The CMS Phase 2 Pixel upgrade will require a high
bandwidth readout system and high radiation tolerance for sensors and on-detector
ASICs. Several technologies for the upgrade sensors are being...
Stefano Gallorini
(Universita e INFN, Padova (IT))
The LHCb tracking system consists of a Vertex Locator around the
interaction point, a tracking station with four layers of silicon strip
detectors in front of the magnet, and three tracking stations, using either
straw-tubes or silicon strip detectors, behind the magnet. This system
allows to reconstruct charged particles with a high efficiency (typically >
95% for particles with momentum...
Marcel Stanitzki
(Deutsches Elektronen-Synchrotron (DE))
The International Linear Collider (ILC ) has been very prominently mentioned in the international strategy documents for HEP and here is a strong interest in Japan to become the host country for the ILC. Two detectors have been proposed for the ILC, the SiD and ILD concepts. They have been validated by an international advisory committee and Detailed Baseline Designs have been presented in...
Herve Marie Xavier Grabas
(University of California,Santa Cruz (US))
ATLAS is currently studying the use of CMOS MAPS devices as a replacement for the baseline silicon strip sensors for the Phase-II Strip Tracker Upgrade. One of the key aspects is to establish whether the radiation hardness is suitable for the HL-LHC environment. Two different technologies are being studied: High-Voltage CMOS and High-Resistivity CMOS. Several test chips have already been...
Alan Litke
(University of California,Santa Cruz (US))
The visual system is a remarkable neural network that is able to extract vital information about the external visual world. The conversion of the dynamic visual input into processed electrical signals is performed by the retina, an extraordinary biological pixel detector that lines the back of the eye and transmits coded information to the brain. The brain does further processing and generates...
Steven Worm
(STFC - Rutherford Appleton Lab. (GB))
CMOS Monolithic Active Pixel Sensors (MAPS) are starting to be investigated for particle
physics experiments. In order to make MAPS the solution of choice for more experiments, we
are developing sensors able to withstand high levels of radiation such as those required by
the extremely harsh environments found in the Large Hadron Collider (LHC) experiments. A
very rad-hard MAPS will also...
Eric Charles
(SLAC National Accelerator Laboratory (US))
Designing trackers for future gamma-ray telescopes to operate in the MeV to GeV range requires making tradeoffs for optimizing the scientific performance. In particular, the choice of available detector technologies combined with the limited space and power available to space-based missions suggest that trade-offs between the collecting area, the field of view, and the spatial and spectral...
Kurt Rinnert
(University of Liverpool (GB))
LHCb is a dedicated experiment to study New Physics in the decays of heavy
hadrons at the Large Hadron Collider (LHC) at CERN. The detector includes a
high precision tracking system consisting of a silicon-strip vertex detector
(VELO) surrounding the pp interaction region, a large-area silicon-strip
detector located upstream of a dipole magnet (TT), and three stations of
silicon-strip...
Sophie Elizabeth Richards
(University of Bristol (GB))
The upgrade of the LHCb experiment, planned for 2018, will transform the experiment to a trigger-less system reading out the full detector at 40 MHz event rate. All data reduction algorithms will be executed in a high-level software farm with access to the complete event
information. This will enable the detector to run at luminosities of 2 x 10^33 /cm^2/s and probe physics beyond the...
Michael Deveaux
(Johann-Wolfgang-Goethe Univ. (DE))
After more than a decade of R&D, CMOS Monolithic Active Pixel Sensors (MAPS) have proven to offer concrete answers to the demanding requirements of subatomic physics experiments. Their main advantages result from their low material budget, their very high granularity and their integrated signal processing circuitry, which allows coping with high particle rates. Moreover, they offer a...
Gabriel John Facini
(University of Chicago (US))
Detailed understanding and optimal track reconstruction performance of ATLAS in the core of high pT objects is paramount for a number of techniques such as jet energy and mass calibration, jet flavour tagging, and hadronic tau identification as well as measurements of physics quantities like jet fragmentation functions. These dense environments are characterized by charged particle...
Giulio Dujany
(University of Manchester (GB))
LHCb has introduced a novel real-time detector alignment and calibration strategy for LHC Run 2. Data collected at the start of the fill will be processed in a few minutes and used to update the alignment, while the calibration constants will be evaluated for each run. This procedure will improve the quality of the online alignment. For example, the vertex locator is retracted and reinserted...
John Stupak
(Purdue University Calumet (US))
The phase 1 upgrade of the CMS pixel detector will replace the existing pixel detector at
the end of 2016 in an extended technical stop. The phase 1 upgrade includes four barrel
layers and three forward disks, providing robust tracking and vertexing for LHC
luminosities up to 2.5 x 10^34 cm-2 s-1 prior to the HL-LHC era. The upgrade incorporates
new readout chips and front-end electronics...
Sally Seidel
(University of New Mexico (US))
Radiation damage to the ATLAS pixel detector is measured continuously by a dedicated system for monitoring leakage current in a representative sample of the modules. Measurements for the full 2011-2012 run are presented and compared to predictions by a theoretical model. The data are used to infer the impact of the current upon the lifetime of the detector.
Rainer Wallny
(Eidgenoessische Tech. Hochschule Zuerich (CH))
The RD42 Collaboration at CERN is investigating Chemical Vapor Deposition (CVD) diamond as a material for tracking detectors operating in extreme radiation environments. This talk will present an overview of latest the developments from RD42. Results from diamond sensor based beam monitors in the ATLAS and CMS experiments at the CERN Large Hadron Collider (LHC) will be presented and the...
Marta Baselga Bacardit
(Instituto de Fisica Corpuscular (ES))
The next upgrades of the HL-LHC (High Luminosity-Large Hadron Collider) are scheduled to
reach fluences of 2e16neq/cm2. Silicon detectors will be expose to high fluences of radiation,
and RD50 (Radiation Hard Semiconductor Devices For High Luminosity Colliders) is a CERN R&D collaboration devoted to develop radiation hard silicon detectors for the HL-LHC. The collaboration explore different...
Timo Hannu Tapani Peltola
(Helsinki Institute of Physics (FI))
Mainly due to their outstanding performance the position sensitive silicon detectors are widely used in the tracking systems of High Energy Physics experiments such as the ALICE, ATLAS, CMS and LHCb at LHC, the world’s largest particle physics accelerator at CERN, Geneva. The foreseen upgrade of the LHC to its high luminosity (HL) phase (HL-LHC scheduled for 2023), will enable the use of...
Mauricio Garcia-Sciveres
(Lawrence Berkeley National Lab. (US))
The current status and plans of RD53 will be presented. This will include radiation testing results of the 65nm process, test chip submissions, and plans for a reticle size chip.
Rudolf Fruhwirth
(Austrian Academy of Sciences (AT))
After a long shutdown, LHC is resuming operation with a center-of-mass energy of 13 TeV. In order to reach the target luminosity not only the collision frequency, but also the beam intensity will be higher than in Run 1. As a consequence, the average number of events underlying the signal events (pile-up) will rise from about 15 to about 25. The LHC collaborations have used the shutdown period...
Dr
Eugene Van Buren
(Brookhaven National Laboratory)
A primary goal of the high luminosity era at RHIC will be the study
of heavy quark behavior in Quark Gluon Plasma. The integration
of high precision silicon-based tracking in the form of the Heavy
Flavor Tracker for the STAR Experiment should enable the
reconstruction and identification of charmed hadron decays,
working in concert with STAR's Time Projection Chamber to
determine momenta...
Lea Michaela Caminada
(Universitaet Zuerich (CH))
The present CMS pixel detector was originally designed for a luminosity of 1 x 10^34 cm-2s-1 and a pileup (number of inelastic interaction per bunch crossing) of 25 in 25 ns bunch spacing. These beam parameters will be reached in the middle of the LHC data taking period 2015-2017 (with an additional increase in the center of mass energy up to the value of 13-14 TeV) and then, peak luminosity...
Monika Kofarago
(Nikhef National institute for subatomic physics (NL))
The upgrade of the Inner Tracking System (ITS) of ALICE is planned for the second long shutdown of the LHC in 2018-2019. The main motivation for the upgrade is the fulfillment of the requirements of the ALICE physics program for run 3 and 4 of the LHC, which requires improved tracking capability and impact parameter resolution at very low transverse momentum, as well as a substantial increase...
Abraham Seiden
(University of California,Santa Cruz (US))
Ultra-fast silicon detectors are a recent detector type using high resistivity n-on-p wafers and including an extra implantation step to create a high field region that amplifies drifting electrons. The target gain is approximately a factor of ten, allowing high rate operation and good time resolution at the same time as good position resolution is achieved. The best time resolution is...
Kurt Rinnert
(University of Liverpool (GB))
The LHCb Vertex Detector (VELO) will be upgraded in 2018 along with the other subsystems of LHCb in order to enable full detector readout at 40 MHz. LHCb will run without a hardware trigger and all data will be fed directly to the software triggering algorithms in the CPU farm. The upgraded VELO is a lightweight silicon hybrid pixel detector with 55 um square pixels, operating in vacuum in...
