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The reconstruction of charged particle trajectories is one of the most complex and CPU consuming parts of event processing in high energy experiments. At future hadron colliders such as the High-Luminosity Large Hadron Collider (HL-LHC) or…

Instrumentation and Detectors · Physics 2019-10-25 Xiaocong Ai

The reconstruction of the trajectories of charged particles, or track reconstruction, is a key computational challenge for particle and nuclear physics experiments. While the tuning of track reconstruction algorithms can depend strongly on…

The proposed Super Tau-Charm Facility (STCF) is an electron-positron collider designed to operate in a center-of-mass energy range from 2 to 7 GeV. It provides a unique platform for physics research in the tau-charm energy region. To…

High Energy Physics - Experiment · Physics 2024-12-20 Hang Zhou , Kexin Sun , Zhenna Lu , Hao Li , Xiaocong Ai , Jin Zhang , Xingtao Huang , Jianbei Liu

In high energy physics (HEP) experiments, the reconstruction of charged particle trajectories is one of the most fundamental yet computationally expensive parts of event processing. At future hadron colliders such as the High-Luminosity…

Instrumentation and Detectors · Physics 2020-07-03 Xiaocong Ai

The Super $\tau$-Charm facility (STCF) is an electron-positron collider proposed by the Chinese particle physics community. It is designed to operate in a center-of-mass energy range from 2 to 7 GeV with a peak luminosity of $0.5\times…

High Energy Physics - Experiment · Physics 2024-05-24 M. Achasov , X. C. Ai , R. Aliberti , L. P. An , Q. An , X. Z. Bai , Y. Bai , O. Bakina , A. Barnyakov , V. Blinov , V. Bobrovnikov , D. Bodrov , A. Bogomyagkov , A. Bondar , I. Boyko , Z. H. Bu , F. M. Cai , H. Cai , J. J. Cao , Q. H. Cao , Z. Cao , Q. Chang , K. T. Chao , D. Y. Chen , H. Chen , H. X. Chen , J. F. Chen , K. Chen , L. L. Chen , P. Chen , S. L. Chen , S. M. Chen , S. Chen , S. P. Chen , W. Chen , X. F. Chen , X. Chen , Y. Chen , Y. Q. Chen , H. Y. Cheng , J. Cheng , S. Cheng , J. P. Dai , L. Y. Dai , X. C. Dai , D. Dedovich , A. Denig , I. Denisenko , D. Z. Ding , L. Y. Dong , W. H. Dong , V. Druzhinin , D. S. Du , Y. J. Du , Z. G. Du , L. M. Duan , D. Epifanov , Y. L. Fan , S. S. Fang , Z. J. Fang , G. Fedotovich , C. Q. Feng , X. Feng , Y. T. Feng , J. L. Fu , J. Gao , P. S. Ge , C. Q. Geng , L. S. Geng , A. Gilman , L. Gong , T. Gong , W. Gradl , J. L. Gu , A. G. Escalante , L. C. Gui , F. K. Guo , J. C. Guo , J. Guo , Y. P. Guo , Z. H. Guo , A. Guskov , K. L. Han , L. Han , M. Han , X. Q. Hao , J. B. He , S. Q. He , X. G. He , Y. L. He , Z. B. He , Z. X. Heng , B. L. Hou , T. J. Hou , Y. R. Hou , C. Y. Hu , H. M. Hu , K. Hu , R. J. Hu , X. H. Hu , Y. C. Hu , J. Hua , G. S. Huang , J. S. Huang , M. Huang , Q. Y. Huang , W. Q. Huang , X. T. Huang , X. J. Huang , Y. B. Huang , Y. S. Huang , N. Hüsken , V. Ivanov , Q. P. Ji , J. J. Jia , S. Jia , Z. K. Jia , H. B. Jiang , J. Jiang , S. Z. Jiang , J. B. Jiao , Z. Jiao , H. J. Jing , X. L. Kang , X. S. Kang , B. C. Ke , M. Kenzie , A. Khoukaz , I. Koop , E. Kravchenko , A. Kuzmin , Y. Lei , E. Levichev , C. H. Li , C. Li , D. Y. Li , F. Li , G. Li , G. Li , H. B. Li , H. Li , H. N. Li , H. J. Li , H. L. Li , J. M. Li , J. Li , L. Li , L. Li , L. Y. Li , N. Li , P. R. Li , R. H. Li , S. Li , T. Li , W. J. Li , X. H. Li , X. Q. Li , X. H. Li , Y. Li , Y. Y. Li , Z. J. Li , H. Liang , J. H. Liang , G. R. Liao , L. Z. Liao , Y. Liao , C. X. Lin , X. S. Lin , B. J. Liu , C. W. Liu , D. Liu , F. Liu , G. M. Liu , H. B. Liu , J. Liu , J. J. Liu , J. B. Liu , K. Liu , K. Y. Liu , K. Liu , L. Liu , Q. Liu , S. B. Liu , T. Liu , X. Liu , Y. W. Liu , Y. Liu , Y. L. Liu , Z. Q. Liu , Z. Y. Liu , Z. W. Liu , I. Logashenko , Y. Long , C. G. Lu , N. Lu , Q. F. Lü , Y. Lu , Y. Lu , Z. Lv , P. Lukin , F. J. Luo , T. Luo , X. F. Luo , H. J. Lyu , X. R. Lyu , J. P. Ma , P. Ma , Y. Ma , F. Maas , S. Malde , D. Matvienko , Z. X. Meng , R. Mitchell , J. M. Dias , A. Nefediev , Y. Nefedov , S. L. Olsen , Q. Ouyang , P. Pakhlov , G. Pakhlova , X. Pan , Y. Pan , E. Passemar , Y. P. Pei , H. P. Peng , L. Peng , X. Y. Peng , X. J. Peng , K. Peters , S. Pivovarov , E. Pyata , B. B. Qi , Y. Q. Qi , W. B. Qian , Y. Qian , C. F. Qiao , J. J. Qin , J. J. Qin , L. Q. Qin , X. S. Qin , T. L. Qiu , J. Rademacker , C. F. Redmer , H. Y. Sang , M. Saur , W. Shan , X. Y. Shan , L. L. Shang , M. Shao , L. Shekhtman , C. P. Shen , J. M. Shen , Z. T. Shen , H. C. 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Zhou , H. Zhou , S. H. Zhou , X. Zhou , X. K. Zhou , X. R. Zhou , Y. L. Zhou , Y. Zhou , Y. X. Zhou , Z. Y. Zhou , J. Y. Zhu , K. Zhu , R. D. Zhu , R. L. Zhu , S. H. Zhu , Y. C. Zhu , Z. A. Zhu , V. Zhukova , V. Zhulanov , B. S. Zou , Y. B. Zuo

An implementation of A Common Tracking Software (ACTS) toolkit for signal electron reconstruction for the COMET muon to electron conversion experiment is discussed. The COMET experiment in J-PARC, Japan, will search for neutrinoless…

High Energy Physics - Experiment · Physics 2024-01-17 Amaia Razquin , MyeongJae Lee

Reconstruction of tracks of charged particles with high precision is very crucial for HEP experiments to achieve their physics goals. As the tracking detector of BESIII experiment, the BESIII drift chamber has suffered from aging effects…

Electron-positron colliders operating in the GeV region of center-of-mass energies or the Tau-Charm energy region, have been proven to enable competitive frontier research, due to its several unique features. With the progress of high…

A description is provided of the software algorithms developed for the CMS tracker both for reconstructing charged-particle trajectories in proton-proton interactions and for using the resulting tracks to estimate the positions of the LHC…

Instrumentation and Detectors · Physics 2014-10-29 CMS Collaboration

The performance of the missing transverse momentum (E$_{T}^{miss}$) reconstruction with the ATLAS detector is evaluated using data collected in proton-proton collisions at the LHC at a center-of-mass energy of 13 TeV in 2015. To reconstruct…

High Energy Physics - Experiment · Physics 2018-12-14 ATLAS Collaboration

sPHENIX is a high energy nuclear physics experiment under construction at the Relativistic Heavy Ion Collider at Brookhaven National Laboratory (BNL). The primary physics goals of sPHENIX are to study the quark-gluon-plasma, as well as the…

We report on the operation and performance of the ATLAS Semi-Conductor Tracker (SCT), which has been functioning for 3 years in the high luminosity, high radiation environment of the Large Hadron Collider at CERN. We also report on the few…

Instrumentation and Detectors · Physics 2019-08-13 Zhijun Liang

The semiconductor tracker (SCT) is one of the tracking systems for charged particles in the ATLAS detector. It consists of 4088 silicon strip sensor modules. During Run 2 (2015$-$2018) the Large Hadron Collider delivered an integrated…

Instrumentation and Detectors · Physics 2022-01-21 ATLAS Collaboration

With the increase in energy of the Large Hadron Collider to a centre-of-mass energy of 13 TeV for Run 2, events with dense environments, such as in the cores of high-energy jets, became a focus for new physics searches as well as…

High Energy Physics - Experiment · Physics 2017-10-27 ATLAS Collaboration

Reconstructing charged particle tracks is a fundamental task in modern collider experiments. The unprecedented particle multiplicities expected at the High-Luminosity Large Hadron Collider (HL-LHC) pose significant challenges for track…

High Energy Physics - Experiment · Physics 2025-12-16 Samuel Van Stroud , Philippa Duckett , Max Hart , Nikita Pond , Sébastien Rettie , Gabriel Facini , Tim Scanlon

The Super Tau-Charm Facility (STCF) is a future electron-positron collider proposed in China with a peak luminosity of above 0.5$\times$10$^{35}$ cm$^{-2}$s$^{-1}$ and center-of-mass energy ranging from 2 to 7 GeV. An excellent particle…

Instrumentation and Detectors · Physics 2021-09-01 Binbin Qi , Ziwei Li , Ming Shao , Jianbei Liu , Zhujun Fang , Huangchao Shi , Xin Li

Particle tracking is among the most sophisticated and complex part of the full event reconstruction chain. A number of reconstruction algorithms work in a sequence to build these trajectories from detector hits. These algorithms use many…

High Energy Physics - Experiment · Physics 2023-12-11 Rocky Bala Garg , Corentin Allaire , Andreas Salzburger , Hadrien Grasland , Lauren Tompkins , Elyssa Hofgard

The identification and reconstruction of charged particles, such as muons, is a main challenge for the physics program of the ATLAS experiment at the Large Hadron Collider. This task will become increasingly difficult with the start of the…

Data Analysis, Statistics and Probability · Physics 2026-03-30 Jonathan Renusch

The expected performance of track reconstruction with LHC events using the CMS silicon tracker is presented. Track finding and fitting is accomplished with Kalman Filter techniques that achieve efficiencies above 99% on single muons with…

Instrumentation and Detectors · Physics 2010-03-04 Paolo Azzurri

The performance and strategies used in electron reconstruction and selection at CMS are presented based on data corresponding to an integrated luminosity of 19.7 inverse femtobarns, collected in proton-proton collisions at sqrt(s) = 8 TeV…

Instrumentation and Detectors · Physics 2015-07-02 CMS Collaboration
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