Resolution of Longitudinal Profile Measures using Coherent Smith-Purcell Radiation with the Number of Gratings and the Number of Pulses Used

arxiv

Authors:

Mélissa Vieille Grosjean, Joanna Barros, Nicolas Delerue, Faissal Bakkali Taheri, George Doucas, Ivan Vasilyevich Konoplev, Armin Reichold, Christine Isabel Clarke

Abstract:

The E-203 collaboration is testing a device on FACET at SLAC to measure the longitudinal profile of electron bunches using Smith-Purcell radiation. At FACET the electron bunches have an energy of 20~GeV and a duration of a few hundred femtoseconds. Smith-Purcell radiation is emitted when a charged particle passes close to the surface of a metallic grating. We have studied the stability of the measurement from pulse to pulse and the resolution of the measure depending on the number of gratings used.

Search for new phenomena in final states with large jet multiplicities and missing transverse momentum using sqrt s = 7 TeV pp collisions with the ATLAS detector

The Journal of High Energy Physics 2011:11

Authors:

AJ Barr, more than 10, The ATLAS Collaboration

Simulation of LiCAS Error Propagation

ECONF C0705302:MET05,2007

Authors:

G Grzelak, A Reichold, J Dale, M Dawson, J Green, Y Han, M Jones, G Moss, B Ottewell, R Wastie, D Kämptner, J Prenting, M Schlösser

Abstract:

Linear Collider Alignment and Survey (LiCAS) R&D group is proposing a novel automated metrology instrument dedicated to align and monitor the mechanical stability of a future linear high energy e+e- collider. LiCAS uses Laser Straightness Monitors (LSM) and Frequency Scanning Interferometry (FSI) for straightness and absolute distance measurements, respectively. This paper presents detailed simulations of a LiCAS system operating inside a Rapid Tunnel Reference Surveyor (RTRS train). With the proposed design it is feasible to achieve the required vertical accuracy of the order of 200 micons over 600 m tunnel sections meeting the specification for the TESLA collider.

Technical design of the phase I Mu3e experiment

Authors:

K Arndt, H Augustin, P Baesso, N Berger, F Berg, C Betancourt, D Bortoletto, A Bravar, K Briggl, D vom Bruch, A Buonaura, F Cadoux, C Chavez Barajas, H Chen, K Clark, P Cooke, S Corrodi, A Damyanova, Y Demets, S Dittmeier, P Eckert, F Ehrler, D Fahrni, L Gerritzen, J Goldstein

Abstract:

The Mu3e experiment aims to find or exclude the lepton flavour violating decay $\mu \rightarrow eee$ at branching fractions above $10^{-16}$. A first phase of the experiment using an existing beamline at the Paul Scherrer Institute (PSI) is designed to reach a single event sensitivity of $2\cdot 10^{-15}$. We present an overview of all aspects of the technical design and expected performance of the phase~I Mu3e detector. The high rate of up to $10^{8}$ muon decays per second and the low momenta of the decay electrons and positrons pose a unique set of challenges, which we tackle using an ultra thin tracking detector based on high-voltage monolithic active pixel sensors combined with scintillating fibres and tiles for precise timing measurements.

Technical design of the phase I Mu3e experiment

Authors:

K Arndt, H Augustin, P Baesso, N Berger, F Berg, C Betancourt, D Bortoletto, A Bravar, K Briggl, D vom Bruch, A Buonaura, F Cadoux, C Chavez Barajas, H Chen, K Clark, P Cooke, S Corrodi, A Damyanova, Y Demets, S Dittmeier, P Eckert, F Ehrler, D Fahrni, L Gerritzen, J Goldstein

Abstract:

The Mu3e experiment aims to find or exclude the lepton flavour violating decay $\mu \rightarrow eee$ at branching fractions above $10^{-16}$. A first phase of the experiment using an existing beamline at the Paul Scherrer Institute (PSI) is designed to reach a single event sensitivity of $2\cdot 10^{-15}$. We present an overview of all aspects of the technical design and expected performance of the phase~I Mu3e detector. The high rate of up to $10^{8}$ muon decays per second and the low momenta of the decay electrons and positrons pose a unique set of challenges, which we tackle using an ultra thin tracking detector based on high-voltage monolithic active pixel sensors combined with scintillating fibres and tiles for precise timing measurements.