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We propose a solution to the CMB component separation problem based on standard parameter estimation techniques. We assume a parametric spectral model for each signal component, and fit the corresponding parameters pixel by pixel in a…

An automatic image segmentation procedure is an inevitable part of many image analyses and computer vision which deeply affect the rest of the system; therefore, a set of interactive segmentation evaluation methods can substantially…

计算机视觉与模式识别 · 计算机科学 2020-11-22 Majid Harouni , Hadi Yazdani Baghmaleki

This study constructs a hybrid module with a multi-material collaborative detection architecture by integrating silicon pixel layers into the longitudinally segmented scintillating fiber sampling calorimeter module and optimizes the…

仪器与探测器 · 物理学 2025-09-30 Jia-Le Fei , Ao Yuan , Chang-Heng Huang , Liu-Pan An , Ji-Ke Wang

CMOS Monolithic Active Pixel Sensors (CPS) are ultra-light and highly granular silicon pixel detectors suited for highly sensitive charged particle tracking. Being manufactured with cost efficient standard CMOS processes, CPS may integrate…

仪器与探测器 · 物理学 2020-01-29 M. Deveaux

We present a unified framework for multipartite entanglement characterization based on the conditional gradient (CG) method, incorporating both fast heuristic detection and rigorous witness construction with numerical error control. Our…

量子物理 · 物理学 2025-08-04 Ye-Chao Liu , Jannis Halbey , Sebastian Pokutta , Sébastien Designolle

Accurate noise characterization is essential for reliable quantum computation. Effective Pauli noise models have emerged as powerful tools, offering detailed description of the error processes with a manageable number of parameters, which…

量子物理 · 物理学 2026-02-03 Alessio Calzona , Miha Papič , Pedro Figueroa-Romero , Adrian Auer

The purpose of this short tutorial paper is to review various criteria that have been used to characterize the quantum character of correlations in optical systems, such as "gemellity", QND correlation, intrication, EPR correlation and Bell…

量子物理 · 物理学 2007-05-23 Nicolas Treps , Claude Fabre

The CMS Beam Conditions and Radiation Monitoring System, BRM, will support beam tuning, protect the CMS detector from adverse beam conditions, and measure the accumulated dose close to or inside all sub-detectors. It is composed of…

CMOS Image Sensors are experiencing significant growth due to their capabilities to be integrated in smartphones with refined image quality. One of the major contributions to the growth of image sensors is the innovation brought about in…

信号处理 · 电气工程与系统科学 2023-06-09 Kirthika Nahalingam , Linda P. B. Katehi

This paper draws a proposal of a set of parameters and methods for accuracy evaluation of visual inspection systems. The case of a monochrome board is treated, but practically all conclusions and methods may be extended for colour…

计算机视觉与模式识别 · 计算机科学 2008-03-04 Radu Arsinte , Costin Miron

Channel polarization is a method of constructing capacity achieving codes for symmetric binary-input discrete memoryless channels (B-DMCs) [1]. In the original paper, the construction complexity is exponential in the blocklength. In this…

信息论 · 计算机科学 2009-05-23 Ryuhei Mori , Toshiyuki Tanaka

The Electron-Muon Ranger (EMR) is a fully-active tracking-calorimeter in charge of the electron background rejection downstream of the cooling channel at the international Muon Ionization Cooling Experiment. It consists of 2832 plastic…

仪器与探测器 · 物理学 2017-10-20 Francois Drielsma

We introduce a pixel space method to detect dipole modulation or hemispherical power asymmetry in the cosmic microwave background (CMB) polarization. The method relies on the use of squared total polarized flux whose ensemble average picks…

宇宙学与河外天体物理 · 物理学 2020-07-15 Shamik Ghosh , Pankaj Jain

Collider detectors have taken advantage of the resolution and accuracy of silicon detectors for at least four decades. Future colliders will need large areas of silicon sensors for low mass trackers and sampling calorimetry. Monolithic…

Muon tomography is a non-destructive imaging technique that uses cosmic-ray muons to probe dense materials. Bar scintillator and scintillating fiber detectors equipped with one-dimensional SiPM arrays offer compact, high-resolution…

仪器与探测器 · 物理学 2026-04-06 Chenghan Lv , Kun Hu , Huiling Li , Hui Liang , Cong Liu , Hongbo Wang , Zibing Wu , Weiwei Xu

We present a new instrument composed of a large number of sub-electron noise Skipper-CCDs operated with a two stage analog multiplexed readout scheme suitable for scaling to thousands of channels. New, thick, $1.35$ Mpix sensors, from a new…

The CMS pixel detector is the innermost component of the CMS tracker occupying the region around the centre of CMS, where the LHC beams are crossed, between 4.3 cm and 30 cm in radius and 46.5 cm along the beam axis. It operates in a…

仪器与探测器 · 物理学 2019-08-13 Viktor Veszpremi

We prove and demonstrate here for the example of the large scale pixel detector of ATLAS that Serial Powering of pixel modules is a viable alternative and that has been devised and implemented for ATLAS pixel modules using dedicated on-chip…

仪器与探测器 · 物理学 2009-11-11 D. B. Ta , T. Stockmanns , F. Huegging , P. Fischer , J. Grosse-Knetter Oe. Runolfsson , N. Wermes

The MIP Timing Detector will provide additional timing capabilities for detection of minimum ionizing particles (MIPs) at CMS during the High Luminosity LHC era, improving event reconstruction and pileup rejection. The central portion of…

仪器与探测器 · 物理学 2021-07-19 R. Abbott , A. Abreu , F. Addesa , M. Alhusseini , T. Anderson , Y. Andreev , A. Apresyan , R. Arcidiacono , M. Arenton , E. Auffray , D. Bastos , L. A. T. Bauerdick , R. Bellan , M. Bellato , A. Benaglia , M. Benettoni , R. Bertoni , M. Besancon , S. Bharthuar , A. Bornheim , E. Brücken , J. N. Butler , C. Campagnari , M. Campana , R. Carlin , P. Carniti , N. Cartiglia , M. Casarsa , O. Cerri , P. Checchia , H. Chen , S. Chidzik , F. Chlebana , F. Cossutti , M. Costa , B. Cox , I. Dafinei , F. De Guio , P. Debbins , D. del Re , A. Dermenev , E. Di Marco , K. Dilsiz , K. F. Di Petrillo , G. Dissertori , S. Dogra , U. Dosselli , I. Dutta , F. Caleb , C. Fernandez Madrazo , M. Fernandez , M. Ferrero , Z. Flowers , W. Funk , M. Gallinaro , S. Ganjour , M. Gardner , F. Geurts , A. Ghezzi , S. Gninenko , F. Golf , J. Gonzalez , C. Gotti , L. Gray , F. Guilloux , S. Gundacker , E. Hazen , S. Hedia , A. Heering , R. Heller , T. Isidori , R. Isocrate , R. Jaramillo , M. Joyce , K. Kaadze , A. Karneyeu , H. Kim , J. King , G. Kopp , M. Korjik , O. K. Koseyan , A. Kozyrev , N. Kratochwil , M. Lazarovits , A. Ledovskoy , H. Lee , J. Lee , A. Li , S. Li , W. Li , T. Liu , N. Lu , M. Lucchini , W. Lustermann , C. Madrid , M. Malberti , I. Mandjavize , J. Mao , Y. Maravin , D. Marlow , B. Marsh , P. Martinez del Arbol , B. Marzocchi , R. Mazza , C. McMahon , V. Mechinsky , P. Meridiani , A. Mestvirishvili , N. Minafra , A. Mohammadi , F. Monti , C. S. Moon , R. Mulargia , M. Murray , Y. Musienko , J. Nachtman , S. Nargelas , L. Narvaez , O. Neogi , C. Neu , T. Niknejad , M. Obertino , H. Ogul , G. Oh , I. Ojalvo , Y. Onel , G. Organtini , T. Orimoto , J. Ott , I. Ovtin , M. Paganoni , F. Pandolfi , R. Paramatti , A. Peck , C. Perez , G. Pessina , C. Pena , S. Pigazzini , O. Radchenko , N. Redaelli , D. Rigoni , E. Robutti , C. Rogan , R. Rossin , C. Rovelli , C. Royon , M. Ö. Sahin , W. Sands , F. Santanastasio , U. Sarica , I. Schmidt , R. Schmitz , J. Sheplock , J. C. Silva , F. Siviero , L. Soffi , V. Sola , G. Sorrentino , M. Spiropulu , D. Spitzbart , A. G. Stahl Leiton , A. Staiano , D. Stuart , I. Suarez , T. Tabarelli de Fatis , G. Tamulaitis , Y. Tang , B. Tannenwald , R. Taylor , E. Tiras , M. Titov , S. Tkaczyk , D. Tlisov , I. Tlisova , M. Tornago , M. Tosi , R. Tramontano , J. Trevor , C. G. Tully , B. Ujvari , J. Varela , S. Ventura , I. Vila , T. Wamorkar , C. Wang , X. Wang , M. Wayne , J. Wetzel , S. White , D. Winn , S. Wu , S. Xie , Z. Ye , G. B. Yu , G. Zhang , L. Zhang , Y. Zhang , Z. Zhang , R. Zhu

The barrel region of the CMS pixel detector will be equipped with ``n-in-n'' type silicon sensors. They are processed on DOFZ material, use the moderated p-spray technique and feature a bias grid. The latter leads to a small fraction of the…