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The heaviest known Fermion particle -- the top quark -- was discovered at Fermilab in the first run of the Tevatron in 1995. However, besides its mere existence one needs to study its properties precisely in order to verify or falsify the…

High Energy Physics - Experiment · Physics 2008-11-26 Daniel Wicke

In 1995, the top quark was discovered at the Fermilab Tevatron Collider by the CDF and D0 collaborations in the ppbar collisions at sqrt(s)=1.8 TeV using about 50pb^-1 of data per experiment. We present the studies of the top quark…

High Energy Physics - Experiment · Physics 2017-08-23 Y. Peters

The physics that can be done with 30 fb$^{-1}$ of data at the Tevatron (TeV33) will significantly advance our understanding of particle physics. In this document we consider the potential of the DO detector for running with the TeV33…

High Energy Physics - Experiment · Physics 2012-08-27 The D0 Collaboration

Online reconstruction is key for monitoring purposes and real time analysis in High Energy and Nuclear Physics experiments. A necessary component of reconstruction algorithms is particle identification that combines information left by a…

Instrumentation and Detectors · Physics 2026-01-13 Richard Tyson , Gagik Gavalian

This paper describes an algorithm for reconstructing and identifying a highly collimated hadronically decaying $\tau$-lepton pair with low transverse momentum. When two $\tau$-leptons are highly collimated, their visible decay products…

High Energy Physics - Experiment · Physics 2025-05-29 ATLAS Collaboration

The MicroBooNE liquid argon time projection chamber (LArTPC) has been taking data at Fermilab since 2015 collecting, in addition to neutrino beam, cosmic-ray muons. Results are presented on the reconstruction of Michel electrons produced by…

Instrumentation and Detectors · Physics 2023-02-17 MicroBooNE collaboration , R. Acciarri , C. Adams , R. An , J. Anthony , J. Asaadi , M. Auger , L. Bagby , S. Balasubramanian , B. Baller , C. Barnes , G. Barr , M. Bass , F. Bay , M. Bishai , A. Blake , T. Bolton , L. Bugel , L. Camilleri , D. Caratelli , B. Carls , R. Castillo Fernandez , F. Cavanna , H. Chen , E. Church , D. Cianci , E. Cohen , G. H. Collin , J. M. Conrad , M. Convery , J. I. Crespo-Anadon , M. Del Tutto , D. Devitt , S. Dytman , B. Eberly , A. Ereditato , L. Escudero Sanchez , J. Esquivel , B. T. Fleming , W. Foreman , A. P. Furmanski , D. Garcia-Gamez , G. T. Garvey , V. Genty , D. Goeldi , S. Gollapinni , N. Graf , E. Gramellini , H. Greenlee , R. Grosso , R. Guenette , A. Hackenburg , P. Hamilton , O. Hen , V Hewes , C. Hill , J. Ho , G. Horton-Smith , E. -C. Huang , C. James , J. Jan de Vries , C. -M. Jen , L. Jiang , R. A. Johnson , J. Joshi , H. Jostlein , D. Kaleko , G. Karagiorgi , W. Ketchum , B. Kirby , M. Kirby , T. Kobilarcik , I. Kreslo , A. Laube , Y. Li , A. Lister , B. R. Littlejohn , S. Lockwitz , D. Lorca , W. C. Louis , M. Luethi , B. Lundberg , X. Luo , A. Marchionni , C. Mariani , J. Marshall , D. A. Martinez Caicedo , V. Meddage , T. Miceli , G. B. Mills , J. Moon , M. Mooney , C. D. Moore , J. Mousseau , R. Murrells , D. Naples , P. Nienaber , J. Nowak , O. Palamara , V. Paolone , V. Papavassiliou , S. F. Pate , Z. Pavlovic , E. Piasetzky , D. Porzio , G. Pulliam , X. Qian , J. L. Raaf , A. Rafique , L. Rochester , C. Rudolf von Rohr , B. Russell , D. W. Schmitz , A. Schukraft , W. Seligman , M. H. Shaevitz , J. Sinclair , E. L. Snider , M. Soderberg , S. Soldner-Rembold , S. R. Soleti , P. Spentzouris , J. Spitz , J. St. John , T. Strauss , K. A. Sutton , A. M. Szelc , N. Tagg , K. Terao , M. Thomson , M. Toups , Y. -T. Tsai , S. Tufanli , T. Usher , R. G. Van de Water , B. Viren , M. Weber , D. A. Wickremasinghe , S. Wolbers , T. Wongjirad , K. Woodruff , T. Yang , L. Yates , G. P. Zeller , J. Zennamo , C. Zhang

This paper describes the mechanical design, the readout chain, the production, testing and the installation of the Silicon Microstrip Tracker of the D0 experiment at the Fermilab Tevatron collider. In addition, description of the…

Instrumentation and Detectors · Physics 2011-03-02 S. N. Ahmed , R. Angstadt , M. Aoki , B. Åsman , S. Austin , L. Bagby , E. Barberis , P. Baringer , A. Bean , A. Bischoff , F. Blekman , T. A. Bolton , C. Boswell , M. Bowden , F. Browning , D. Buchholz , S. Burdin , D. Butler , H. Cease , S. Choi , A. R. Clark , J. Clutter , A. Cooper , W. E. Cooper , M. Corcoran , S. J. de Jong , M. Demarteau , R. Demina , S. Desai , G. Derylo , J. Ellison , P. Ermolov , J. Fagan , J. Fast , F. Filthaut , J. Foglesong , H. Fox , C. F. Galea , J. Gardner , R. J. Genik , C. E. Gerber , Y. Gershtein , K. Gounder , S. Grinstein , W. Gu , P. Gutierrez , H. Haggerty , R. E. Hall , S. Hagopian , R. Hance , K. Harder , P. Heger , A. P. Heinson , U. Heintz , G. Hesketh , D. Hover , J. Howell , M. Hrycyk , I. Iashvili , M. Johnson , H. Jöstlein , A. Juste , W. Kahl , E. Kajfasz , D. Karmanov , S. Kesisoglou , A. Khanov , J. King , S. Kleinfelder , J. Kowalski , K. Krempetz , M. Kubantsev , Y. Kulik , G. Landsberg , A. Leflat , F. Lehner , R. Lipton , H. S. Mao , M. Martin , J. Mateski , M. Matulik , M. McKenna , A. Melnitchouk , M. Merkin , D. Mihalcea , O. Milgrome , H. E. Montgomery , S. Moua , N. A. Naumann , A. Nomerotski , D. Olis , D. C. O'Neil , G. J. Otero y Garzón , N. Parua , J. Pawlak , M. Petteni , B. Quinn , P. A. Rapidis , P. Ratzmann , F. Rizatdinova , M. Roco , R. Rucinski , V. Rykalin , H. Schellman , W. Schmitt , G. Sellberg , C. Serritella , E. Shabalina , R. A. Sidwell , V. Simak , E. Smith , B. Squires , N. R. Stanton , G. Steinbrück , J. Strandberg , S. Strandberg , M. Strauss , S. Stredde , A. Toukhtarov , S. M. Tripathi , T. G. Trippe , D. Tsybychev , M. Utes , P. van Gemmeren , M. Vaz , M. Weber , D. A. Wijngaarden , J. Wish , J. Womersley , R. Yarema , Z. Ye , A. Zieminski , T. Zimmerman , E. G. Zverev

The standard model is a successful but limited theory. There is significant theoretical motivation to believe that new physics may appear at the energy scale of a few TeV, the lower end of which is currently probed by the Fermilab Tevatron…

High Energy Physics - Experiment · Physics 2009-06-22 Joel Piper

The collisions of high energy photons produced at an electron-positron collider provide a comprehensive laboratory for testing QCD, electroweak interactions, and extensions of the Standard Model. The luminosity and energy of the colliding…

High Energy Physics - Phenomenology · Physics 2009-09-25 Stanley J. Brodsky , SLAC , Peter M. Zerwas , DESY

We present the results of searches for non-standard model phenomena in photon and jet final states. These searches use data from integrated luminosities of 0.7--2.7/fb of p-pbar collisions at sqrt(s)=1.96 TeV, collected with the CDF and D0…

High Energy Physics - Experiment · Physics 2009-05-15 Shin-Shan Yu

This review discusses how low-energy, valence excitations created by swift electrons can render information on the optical response of structured materials with unmatched spatial resolution. Electron microscopes are capable of focusing…

Materials Science · Physics 2012-11-13 F. J. Garcia de Abajo

We have measured the W boson mass using the D0 detector and a data sample of 82 pb^-1 from the Tevatron collider. This measurement used W -> e nu decays, where the electron is close to a boundary of a central electromagnetic calorimeter…

High Energy Physics - Experiment · Physics 2008-11-26 The D0 Collaboration , V. M. Abazov

High intensity back-scattered laser beams will allow the efficient conversion of a substantial fraction of the incident lepton energy into high energy photons, thus significantly extending the physics capabilities of an electron-electron or…

High Energy Physics - Phenomenology · Physics 2009-09-11 S. J. Brodsky

The D0 experiment was designed in the mid 1980s and ran at the Fermilab pp collider from 1992 through 2011. I describe the uranium-liquid argon calorimeter and its readout electronic which was upgraded in the late 1990s to handle the higher…

Instrumentation and Detectors · Physics 2014-03-19 Dean Schamberger

Results on diffraction from the Fermilab Tevatron collider obtained by the CDF II Collaboration using data from proton-antiproton collisions at a c.m.s. energy of 1.96 TeV are reviewed and compared with theoretical expectations.…

High Energy Physics - Experiment · Physics 2010-05-12 Konstantin Goulianos

Electron tomography is becoming an increasingly important tool in materials science for studying the three-dimensional morphologies and chemical compositions of nanostructures. The image quality obtained by many current algorithms is…

Electron tomography is a technique used in both materials science and structural biology to image features well below optical resolution limit. In this work, we present a new algorithm for reconstructing the three-dimensional(3D)…

Signal Processing · Electrical Eng. & Systems 2018-07-12 David Ren , Michael Chen , Laura Waller , Colin Ophus

Results on soft and hard diffraction obtained by the CDF Collaboration at the Fermilab Tevatron proton-antiproton Collider are reviewed with emphasis on aspects of the data that point to the underlying QCD mechanism for diffraction. The…

High Energy Physics - Phenomenology · Physics 2014-11-17 Konstantin Goulianos

Detailed measurements of the electron performance of the ATLAS detector at the LHC are reported, using decays of the Z, W and J/psi particles. Data collected in 2010 at sqrt(s)=7 TeV are used, corresponding to an integrated luminosity of…

High Energy Physics - Experiment · Physics 2012-08-27 ATLAS Collaboration

In the last decades electroweak processes were studied at hadron and lepton colliders. By exploiting the large statistics and the c.o.m. energy available, hadron colliders played a significant role in performing precision measurements of…

High Energy Physics - Experiment · Physics 2009-10-02 Giorgio Chiarelli