The design of detector concepts has been driven for a long time by requirements on transverse momentum, impact parameter and jet energy resolutions, as well as hermeticity. Only rather recently it has been realised that the ability to identify different types of charged hadrons, in particular kaons and protons, could have important applications at Higgs factories, ranging from improvements in tracking, vertexing and flavour tagging to measurements requiring strangeness-tagging. While detector concepts with gaseous tracking can exploit the specific energy loss, all-silicon-based detectors have to rely on fast timing layers in front of or in the first layers of their electromagnetic calorimeters. This presentation will review the different op...
This paper deals with two major particle identification methods: dE/dx and Cherenkov detection. In t...
This thesis is based on a study of Natural Supersymmetry (SUSY) scenarios at the International Linea...
One of the unique features of the E814 experimental setup at the BNL-AGS, is its nearly 4$ pi$ calor...
The design of detector concepts has been driven since a long time by requirements on transverse mome...
We present an overview of a study on precise mass reconstruction and identification of charged hadro...
At the latest European strategy update in 2020 it has been highlighted that the next highest-priorit...
The International Linear Collider ILC is a planned linear e+ e− collider. With a well defined initia...
For the International Large Detector (ILD) at the planned International Linear Collider (ILC) a Time...
Abstract The kaon identification is crucial for the flavor physics, and also benefits the flavor and...
The kaon identification is crucial for the flavor physics, and also benefits the flavor and charge r...
The particle identification capabilities of the ALICE experiment are unique among the four major LHC...
Equipping an experiment at FCC-ee with particle identification (PID) capabilities, in particular the...
Precision timing has alway been a prominent topic in the instrumentation for high-energy physics exp...
Abstract We study the impact of precision timing detection systems on the LHC experiments’ long-live...
The ATLAS Detector, below the surface of the Swiss-French border, measures the remnants of high-ener...
This paper deals with two major particle identification methods: dE/dx and Cherenkov detection. In t...
This thesis is based on a study of Natural Supersymmetry (SUSY) scenarios at the International Linea...
One of the unique features of the E814 experimental setup at the BNL-AGS, is its nearly 4$ pi$ calor...
The design of detector concepts has been driven since a long time by requirements on transverse mome...
We present an overview of a study on precise mass reconstruction and identification of charged hadro...
At the latest European strategy update in 2020 it has been highlighted that the next highest-priorit...
The International Linear Collider ILC is a planned linear e+ e− collider. With a well defined initia...
For the International Large Detector (ILD) at the planned International Linear Collider (ILC) a Time...
Abstract The kaon identification is crucial for the flavor physics, and also benefits the flavor and...
The kaon identification is crucial for the flavor physics, and also benefits the flavor and charge r...
The particle identification capabilities of the ALICE experiment are unique among the four major LHC...
Equipping an experiment at FCC-ee with particle identification (PID) capabilities, in particular the...
Precision timing has alway been a prominent topic in the instrumentation for high-energy physics exp...
Abstract We study the impact of precision timing detection systems on the LHC experiments’ long-live...
The ATLAS Detector, below the surface of the Swiss-French border, measures the remnants of high-ener...
This paper deals with two major particle identification methods: dE/dx and Cherenkov detection. In t...
This thesis is based on a study of Natural Supersymmetry (SUSY) scenarios at the International Linea...
One of the unique features of the E814 experimental setup at the BNL-AGS, is its nearly 4$ pi$ calor...