24 citations · 45 across the 17 of their papers we have counts for
21 papers
Advances in photocathode development for PICOSEC Micromegas precise-timing detectors
M. Lisowska, F. Guerra, A. Gurpinar +46
The PICOSEC Micromegas detector is a~precise-timing gaseous detector that combines a Cherenkov radiator, a~semi-transparent photocathode and a Micromegas amplification stage, targe…
Spatial resolution improvement of PICOSEC Micromegas precise timing detectors
F. M. Brunbauer, R. Aleksan, Y. Angelis +47
The combination of a Cherenkov radiator with a semi-transparent photocathode and a Micromegas based amplification stage allows PICOSEC Micromegas detectors to achieve a time resolu…
Test-beam results from MiniCACTUS-v2: A depleted monolithic CMOS timing sensor prototype
Y. Degerli, R. Aleksan, R. Casanova +9
MiniCACTUS-v2 is a monolithic sensor prototype designed in LF 150 nm CMOS process for time tagging of individual Minimum Ionizing Particles with an accuracy better than 100 ps. The…
Design, simulation and performance of the resistive-anode PICOSEC Micromegas detector
Djunes Janssens, Antonija Utrobicic, Marinko Kovacic +52
The PICOSEC Micromegas detector is a Micro-Pattern Gaseous Detector concept developed to achieve tens of picosecond timing resolution for charged particle detection by combining a…
μRWELL-PICOSEC: Precision Timing with Resistive Micro-Well Detector
Kondo Gnanvo
The PICOSEC detector concept uses a micro-pattern gaseous detector (MPGD) amplification structure combined with a Cerenkov radiator coated with a semi-transparent photocathode to p…
Design and Performance of a 96-channel Resistive PICOSEC Micromegas Detector for ENUBET
A. Kallitsopoulou, S. Aune, Y. Angelis +54
The PICOSEC-Micromegas (PICOSEC-MM) detector is a fast gaseous detector that achieves picosecond-level timing by coupling a Cherenkov radiator, typically an MgF2 crystal, to a Micr…
Performance Optimization and Characterization of 7-pad Resistive PICOSEC Micromegas Detectors
A. Kallitsopoulou, R. Aleksan, S. Aune +49
We present a comprehensive characterization of resistive PICOSEC Micromegas detector prototypes, tested under identical conditions, constant drift gap, field configurations, and ph…
Leptogenesis and Dirac neutrino masses in SO(10)
R. Aleksan, L. Oliver
Within the scheme of Baryogenesis through Leptogenesis in the single flavor approximation, we emphasize the role of the Dirac neutrino mass in the SO(10) Grand Unification sc…
Future Circular Collider Feasibility Study Report: Volume 2, Accelerators, Technical Infrastructure and Safety
M. Benedikt, F. Zimmermann, B. Auchmann +1461
In response to the 2020 Update of the European Strategy for Particle Physics, the Future Circular Collider (FCC) Feasibility Study was launched as an international collaboration ho…
Future Circular Collider Feasibility Study Report: Volume 3, Civil Engineering, Implementation and Sustainability
M. Benedikt, F. Zimmermann, B. Auchmann +1461
Volume 3 of the FCC Feasibility Report presents studies related to civil engineering, the development of a project implementation scenario, and environmental and sustainability asp…
Future Circular Collider Feasibility Study Report: Volume 1, Physics, Experiments, Detectors
M. Benedikt, F. Zimmermann, B. Auchmann +1461
Volume 1 of the FCC Feasibility Report presents an overview of the physics case, experimental programme, and detector concepts for the Future Circular Collider (FCC). This volume o…
PICOSEC Micromegas Precise-timing Detectors: Development towards Large-Area and Integration
Y. Meng, R. Aleksan, Y. Angelis +49
PICOSEC Micromegas (MM) is a precise timing gaseous detector based on a Cherenkov radiator coupled with a semi-transparent photocathode and an MM amplifying structure. The detector…
PICOSEC-Micromegas Detector, an innovative solution for Lepton Time Tagging
A. Kallitsopoulou, R. Aleksan, Y. Angelis +49
The PICOSEC-Micromegas (PICOSEC-MM) detector is a novel gaseous detector designed for precise timing resolution in experimental measurements. It eliminates time jitter from charged…
A Novel Diamond-like Carbon based photocathode for PICOSEC Micromegas detectors
X. Wang, R. Aleksan, Y. Angelis +48
The PICOSEC Micromegas (MM) detector is a precise timing gaseous detector based on a MM detector operating in a two-stage amplification mode and a Cherenkov radiator. Prototypes eq…
Photocathode characterisation for robust PICOSEC Micromegas precise-timing detectors
M. Lisowska, R. Aleksan, Y. Angelis +55
The PICOSEC Micromegas detector is a~precise-timing gaseous detector based on a~Cherenkov radiator coupled with a~semi-transparent photocathode and a~Micromegas amplifying structur…
Single channel PICOSEC Micromegas detector with improved time resolution
A. Utrobicic, R. Aleksan, Y. Angelis +47
This paper presents design guidelines and experimental verification of a single-channel PICOSEC Micromegas (MM) detector with an improved time resolution. The design encompasses th…
Timing-based mass measurement of exotic long-lived particles at the FCC-ee
Roy Aleksan, Emmanuel Perez, Giacomo Polesello +1
The very high luminosity run foreseen at the -pole for the FCC-ee will allow the detection in decays of new particles with very low couplings to the Standard Model. These pa…
Analysis of data on decays into two light vector mesons
Roy Aleksan, Luis Oliver
An important experimental effort has been accomplished in recent years in the measurement of rates, polarization and CP observables in decays into two light vector mesons. On t…
Measuring the angle of the flattest Unitary Triangle with decays
Roy Aleksan, Luis Oliver, Emmanuel Perez
We show that the angle of the ``flattest'' unitarity triange can be directly measured using the decays and $\overline{B}_{s}\to…
decays, a serious problem for the Standard Model
Roy Aleksan, Luis Oliver
We underline the theoretical and experimental interest of the vector-vector penguin decays for which the data show a s…
Measurement of CP Asymmetry in B0 to Ks pi0 pi0 Decays
The BABAR Collaboration, B. Aubert
We present a measurement of the time-dependent CP asymmetry for the neutral B-meson decay into the CP = +1 final state Ks pi0 pi0, with Ks -> pi+ pi-. We use a sample of approximat…