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Related papers: Muon Identification without Iron

200 papers

The magnetized Iron CALorimeter detector (ICAL) which is proposed to be built in the India-based Neutrino Observatory (INO) laboratory, aims to study atmospheric neutrino oscillations primarily through charged current interactions of muon…

Instrumentation and Detectors · Physics 2015-06-24 R. Kanishka , Meghna K. K. , Vipin Bhatnagar , D. Indumathi , Nita Sinha

A short summary of the LHCb muon identification procedure is given in this article. First, the muon system of LHCb is presented, together with some examples of physics measurements of the experiment where the muon identification is crucial.…

High Energy Physics - Experiment · Physics 2010-05-17 X. Cid Vidal

The first acceleration stage for this muon collider scenario includes twenty passes through a single two GeV Linac. Teardrop shaped arcs of 1.8 Tesla fixed field magnets are used at each end of the Linac. This dogbone geometry minimizes…

High Energy Physics - Experiment · Physics 2008-11-26 D. J. Summers

The relative immunity of muons to synchrotron radiation suggests that they might be used in place of electrons as probes in fundamental high-energy physics experiments. Muons are commonly produced indirectly through pion decay by…

Accelerator Physics · Physics 2015-04-03 Diktys Stratakis , David V. Neuffer

The MEG II experiment searches for a charged-lepton-flavour-violating $\mu \to e \gamma$ with the target sensitivity of $6 \times 10^{-14}$. A liquid xenon calorimeter with VUV-sensitive photosensors measures photon position, timing, and…

In both particle physics and cosmic ray muon applications, a high-resolution muon momentum measurement capability plays a significant role not only in providing valuable information on the properties of subatomic particles but also in…

Instrumentation and Detectors · Physics 2021-11-25 Junghyun Bae , Stylianos Chatzidakis

Muon Colliders have unique technical and physics advantages and disadvantages when compared with both hadron and electron machines. They should thus be regarded as complementary. Parameters are given of 4 TeV and 0.5 TeV high luminosity…

acc-phys · Physics 2012-08-29 R. B. Palmer , A. Sessler , A. Skrinsky , A. Tollestrup

We present a measurement of the ratio of positive to negative muon fluxes from cosmic ray interactions in the atmosphere, using data collected by the CMS detector both at ground level and in the underground experimental cavern at the CERN…

High Energy Physics - Experiment · Physics 2012-08-27 The CMS Collaboration

A muon collider represents the ideal machine to reach very high center-of-mass energies and luminosities by colliding elementary particles. This is the result of the low level of beamstrahlung and synchrotron radiation compared to linear or…

The performance of muon reconstruction in CMS is evaluated using a large data sample of cosmic-ray muons recorded in 2008. Efficiencies of various high-level trigger, identification, and reconstruction algorithms have been measured for a…

Instrumentation and Detectors · Physics 2012-08-27 CMS Collaboration

In the case of underground experiments for neutrino physics or rare event searches, the background caused by cosmic muons contributes significantly and therefore must be identified and rejected. We proposed and optimized a new detector…

Instrumentation and Detectors · Physics 2017-04-05 Y. P. Zhang , J. L. Xu , H. Q. Lu , P. Zhang , C. C. Zhang , C. G. Yang

The Underground Muon Detector of the Pierre Auger Observatory features a calorimetric detection mode that estimates the number of muons based on signal charge measurements. This contribution provides an overview of the calibration…

Instrumentation and Detectors · Physics 2025-07-25 Marina Scornavacche

The Mu2e experiment at Fermilab aims at measuring the neutrinoless conversion of a negative muon into an electron and reach a single event sensitivity of 2.5x10^{-17} after three years of data taking. The monoenergetic electron produced in…

The Compact Muon Solenoid (CMS) is a general purpose detector, designed to run at the highest luminosity at the CERN Large Hadron Collider (LHC). Its distinctive features include a 4 T superconducting solenoid with 6-m-diameter by…

Instrumentation and Detectors · Physics 2016-08-09 V. I. Klyukhin , N. Amapane , A. Ball , B. Curé , A. Gaddi , H. Gerwig , A. Hervé , M. Mulders , R. Loveless

Muons have a similar latency/energy correlation from pion decay as do the neutrinos, and hence in each time-slice in a stroboscopic analysis measurements of their momentum spectra can reduce systematic uncertainties due to flux. There are,…

High Energy Physics - Experiment · Physics 2022-12-20 Henry J. Frisch

The Compact Muon Solenoid (CMS) is a general purpose detector, designed to run at the highest luminosity at the CERN Large Hadron Collider (LHC). Its distinctive features include a 4 T superconducting solenoid with 6-m-diameter by…

Instrumentation and Detectors · Physics 2017-12-21 B. Curé , N. Amapane , A. Ball , A. Gaddi , H. Gerwig , A. Hervé , V. I. Klyukhin , R. Loveless , M. Mulders

We report the in-situ 3D reconstruction of through-going muons in the CUORE experiment, a cryogenic calorimeter array searching for neutrinoless double beta ($0\nu\beta\beta$) decay, leveraging the segmentation of the detector. Due to the…

Instrumentation and Detectors · Physics 2025-09-09 CUORE Collaboration , D. Q. Adams , C. Alduino , K. Alfonso , A. Armatol , F. T. Avignone , O. Azzolini , G. Bari , F. Bellini , G. Benato , M. Beretta , M. Biassoni , A. Branca , D. Brandani , C. Brofferio , C. Bucci , J. Camilleri , A. Caminata , A. Campani , J. Cao , S. Capelli , L. Cappelli , L. Cardani , P. Carniti , N. Casali , D. Chiesa , Y. Chu , M. Clemenza , S. Copello , O. Cremonesi , R. J. Creswick , A. D'Addabbo , I. Dafinei , S. Dell'Oro , S. Di Domizio , S. Di Lorenzo , T. Dixon , D. Q. Fang , M. Faverzani , E. Ferri , F. Ferroni , E. Fiorini , M. A. Franceschi , S. J. Freedman , S. H. Fu , B. K. Fujikawa , S. Ghislandi , A. Giachero , M. Girola , L. Gironi , A. Giuliani , P. Gorla , C. Gotti , P. V. Guillaumon , T. D. Gutierrez , K. Han , E. V. Hansen , K. M. Heeger , D. L. Helis , H. Z. Huang , M. T. Hurst , G. Keppel , Yu. G. Kolomensky , R. Kowalski , R. Liu , L. Ma , Y. G. Ma , L. Marini , R. H. Maruyama , D. Mayer , M. N. Moore , T. Napolitano , M. Nastasi , C. Nones , E. B. Norman , A. Nucciotti , I. Nutini , T. O'Donnell , M. Olmi , S. Pagan , C. E. Pagliarone , L. Pagnanini , M. Pallavicini , L. Pattavina , M. Pavan , G. Pessina , V. Pettinacci , C. Pira , S. Pirro , E. G. Pottebaum , S. Pozzi , E. Previtali , A. Puiu , S. Puranam , S. Quitadamo , A. Ressa , C. Rosenfeld , B. Schmidt , R. Serino , A. Shaikina , V. Sharma , V. Singh , M. Sisti , D. Speller , P. T. Surukuchi , L. Taffarello , C. Tomei , A. Torres , J. A. Torres , K. J. Vetter , M. Vignati , S. L. Wagaarachchi , R. Wang , B. Welliver , J. Wilson , K. Wilson , L. A. Winslow , F. Xie , T. Zhu , S. Zimmermann , S. Zucchelli

We have developed a track fitting procedure based on Kalman Filter technique for an Iron Calorimeter (ICAL) prototype detector when the detector is flushed with single muon tracks. The relevant track parameters i.e., momentum, direction and…

Nuclear Experiment · Physics 2009-08-07 Tapasi Ghosh , Subhasis Chattopadhyay

We have designed a threshold Cherenkov detector at the Rutherford-Appleton Laboratory to identify muons with momenta between 230 and 350 MeV/c. We investigated the properties of three aerogels for the design. The nominal indexes of…

Instrumentation and Detectors · Physics 2009-09-28 Lucien Cremaldi , David A. Sanders , Peter Sonnek , Donald J. Summers , Jim Reidy