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The occurrence of vacuum arcs or radio frequency (rf) breakdowns is one of the most prevalent factors limiting the high-gradient performance of normal conducting rf cavities in particle accelerators. In this paper, we search for the…

The Wake Field Monitor (WFM) system installed on the CLIC prototype accelerating structure in CERN Linear Accelerator for Research (CLEAR) has two channels for each horizontal/vertical plane, operating at different frequencies. When moving…

Aspects of ICHEP 2004 are summarized from a theoretical point of view. QCD works, new NNLO calculations are becoming available and new string calculational tools are emerging, but no conclusions can yet be drawn about the discovery of the…

High Energy Physics - Phenomenology · Physics 2010-11-05 John Ellis

We discuss implementation of the LHC experimental data sets in the new CT18 global analysis of quantum chromodynamics (QCD) at the next-to-next-leading order of the QCD coupling strength. New methodological developments in the fitting…

This part of the conference proceeding provides a detailed overview of cutting-edge advancements in detector technologies, focusing on their optimization, characterization, and applications in particle physics experiments. Building on the…

We report on suppression of long-range wakefields in CLIC accelerating structures. Strong detuning and moderate damping is employed. In these initial design studies we focus on the CLIC_G structure and enforce a moderate Q of 300 and 500.…

Accelerator Physics · Physics 2009-06-22 V. F. Khan , R. M. Jones

Nitrogen seeded detachment has been achieved in the Tokamak a Configuration Variable (TCV) in advanced divertor configurations (ADCs), namely X-divertor and X-point target, with and without baffles in H-mode plasmas with high core…

The Compact Linear Collider (CLIC) is a high-energy high-luminosity linear electron-positron collider under development. It is foreseen to be built and operated in three stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV,…

Instrumentation and Detectors · Physics 2019-05-08 A. C. Abusleme Hoffman , G. Parès , T. Fritzsch , M. Rothermund , H. Jansen , K. Krüger , F. Sefkow , A. Velyka , J. Schwandt , I. Perić , L. Emberger , C. Graf , A. Macchiolo , F. Simon , M. Szalay , N. van der Kolk , H. Abramowicz , Y. Benhammou , O. Borysov , M. Borysova , A. Joffe , S. Kananov , A. Levy , I. Levy , G. Eigen , R. Bugiel , S. Bugiel , M. Firlej , T. A. Fiutowski , M. Idzik , J. Moroń , K. P. Świentek , P. Terlecki , P. Brückman de Renstrom , B. Turbiarz , T. Wojtoń , L. K. Zawiejski , E. Firu , V. Ghenescu , A. T. Neagu , T. Preda , I. Boyko , Yu. Nefedov , A. Rymbekova , A. Sapronov , G. Shelkov , A. Zhemchugov , A. Ruiz-Jimeno , I. Vila , E. Fullana , J. Fuster , P. Gomis Lopez , M. Perelló , M. A. Villarejo , M. Vos , J. Alozy , N. Alipour Tehrani , D. Arominski , R. Ballabriga Sune , F. Boyer , E. Brondolin , M. Buckland , M. Campbell , D. Dannheim , K. Dette , F. Duarte Ramos , N. Egidos Plaja , K. Elsener , A. Fiergolski , C. Fuentes Rojas , C. Grefe , D. Hynds , W. Klempt , I. Kremastiotis , J. Kröger , S. Kulis , E. Leogrande , L. Linssen , X. Llopart Cudie , A. Lucaci-Timoce , M. Munker , L. Musa , A. Nürnberg , F. -X. Nuiry , E. Perez Codina , H. Pernegger , M. Petrič , F. Pitters , T. Quast , S. Redford , P. Riedler , P. Roloff , A. Sailer , E. Santin , U. Schnoor , E. Sicking , K. Sielewicz , R. Simoniello , W. Snoeys , S. Spannagel , S. Sroka , R. Ström , P. Valerio , S. van Dam , E. van der Kraaij , T. Vǎnát , O. Viazlo , M. Vicente Barreto Pinto , M. A. Weber , M. Williams , K. Wolters , M. Benoit , G. Iacobucci , D M S Sultan , R. R. Bosley , T. Price , M. F. Watson , N. K. Watson , A. G. Winter , J. Goldstein , S. Green , J. S. Marshall , M. A. Thomson , B. Xu , G. Casse , J. Vossebeld , T. Coates , F. Salvatore , J. Repond , L. Xia , C. Kenney , A. Tomada

In the NLC (Next Linear Collider) small misalignments in each of the individual accelerator structures (or the accelerator cells) will give rise to wakefields which kick the beam from its electrical axis. This wakefield can cause BBU (Beam…

Accelerator Physics · Physics 2009-03-12 R. M. Jones , N. M. Kroll , R. H. Miller , T. O. Raubenheimer , G. V. Stupakov

A large Time Projection Chamber is the main device for tracking and charged-particle identification in the ALICE experiment at the CERN LHC. After the second long shutdown in 2019/20, the LHC will deliver Pb beams colliding at an…

Instrumentation and Detectors · Physics 2018-07-16 M. M. Aggarwal , Z. Ahammed , S. Aiola , J. Alme , T. Alt , W. Amend , A. Andronic , V. Anguelov , H. Appelshäuser , M. Arslandok , R. Averbeck , M. Ball , G. G. Barnaföldi , E. Bartsch , R. Bellwied , G. Bencedi , M. Berger , N. Bialas , P. Bialas , L. Bianchi , S. Biswas , L. Boldizsár , L. Bratrud , P. Braun-Munzinger , M. Bregant , C. L. Britton , E. J. Brucken , H. Caines , A. J. Castro , S. Chattopadhyay , P. Christiansen , L. G. Clonts , T. M. Cormier , S. Das , S. Dash , A. Deisting , S. Dittrich , A. K. Dubey , R. Ehlers , M. Engel , F. Erhardt , N. B. Ezell , L. Fabbietti , U. Frankenfeld , J. J. Gaardhøje , C. Garabatos , P. Gasik , Á. Gera , P. Ghosh , S. K. Ghosh , P. Glässel , O. Grachov , A. Grein , T. Gunji , H. Hamagaki , G. Hamar , J. W. Harris , P. Hauer , J. Hehner , E. Hellbär , H. Helstrup , T. E. Hilden , B. Hohlweger , M. Ivanov , M. Jung , D. Just , E. Kangasaho , R. Keidel , B. Ketzer , S. A. Khan , S. Kirsch , T. Klemenz , S. Klewin , A. G. Knospe , M. Kowalski , L. Kumar , R. Lang , R. Langoy , L. Lautner , F. Liebske , J. Lien , C. Lippmann , H. M. Ljunggren , W. J. Llope , S. Mahmood , T. Mahmoud , R. Majka , P. Malzacher , A. Marín , C. Markert , S. Masciocchi , A. Mathis , A. Matyja , M. Meres , D. L. Mihaylov , D. Miskowiec , J. Mitra , T. Mittelstaedt , T. Morhardt , J. Mulligan , R. H. Munzer , K. Münning , M. G. Munhoz , S. Muhuri , H. Murakami , B. K. Nandi , H. Natal da Luz , C. Nattrass , T. K. Nayak , R. A. Negrao De Oliveira , M. Nicassio , B. S. Nielsen , L. Oláh , A. Oskarsson , J. Otwinowski , K. Oyama , G. Paić , R. N. Patra , V. Peskov , M. Pikna , L. Pinsky , M. Planinic , M. G. Poghosyan , N. Poljak , F. Pompei , S. K. Prasad , C. A. Pruneau , J. Putschke , S. Raha , J. Rak , J. Rasson , V. Ratza , K. F. Read , A. Rehman , R. Renfordt , T. Richert , K. Røed , D. Röhrich , T. Rudzki , R. Sahoo , S. Sahoo , P. K. Sahu , J. Saini , B. Schaefer , J. Schambach , S. Scheid , C. Schmidt , H. R. Schmidt , N. V Schmidt , H. Schulte , K. Schweda , I. Selyuzhenkov , N. Sharma , D. Silvermyr , R. N. Singaraju , B. Sitar , N. Smirnov , S. P. Sorensen , F. Sozzi , J. Stachel , E. Stenlund , P. Strmen , I. Szarka , G. Tambave , K. Terasaki , A. Timmins , K. Ullaland , A. Utrobicic , D. Varga , R. Varma , A. Velure , V. Vislavicius , S. Voloshin , B. Voss , D. Vranic , J. Wiechula , S. Winkler , J. Wikne , B. Windelband , C. Zhao

Recent experiments at SLAC [1,2] and CERN [3] have revealed evidence of significant deformation in the form of "pitting" of the cells of the 1.8m series of structures DDS/RDDS (Damped Detuned Structure/Rounded Damped Detuned Structure).…

Accelerator Physics · Physics 2008-11-26 R. M. Jones , N. M. Kroll , T. Higo , Z. Li , R. H. Miller , T. O. Raubenheimer , J. W. Wang

The Inert Doublet Model (IDM) is a simple extension of the Standard Model, introducing an additional Higgs doublet that brings in four new scalar particles. The lightest of the IDM scalars is stable and is a good candidate for a dark matter…

High Energy Physics - Phenomenology · Physics 2022-11-01 Jan Klamka , Aleksander Filip Zarnecki

In this paper, we summarize the high power testing results of the X-band mixed-mode RF windows at KEK and SLAC for linear colliders. The main feature of these windows is that the combination of modes on the surface of the ceramic…

High Energy Physics - Experiment · Physics 2007-05-23 S. Tokumoto , Y. H. Chin , H. Mizuno , K. Ohya , S. Yamaguchi , KEK , Tsukuba , Japan S. Kazakov , BINP , Protvino , Moscow , Russia R. Loewen , R. Fowkes , A. Menegat , A. Vlieks , SLAC , Stanford , CA , USA

Next-generation dual-phase time projection chambers (TPCs) for rare event searches will require large-scale, high-precision electrodes. To meet the stringent requirements for high-voltage performance of such an experiment, we have developed…

Instrumentation and Detectors · Physics 2026-02-04 Shumit A. Mitra , Alexander Deisting , Jan Lommler , Uwe Oberlack , Fabian Piermaier , Quirin Weitzel , Daniel Wenz

Dielectric layers are gradually being down-scaled in different electronic devices like MOSFETs and Magnetic Tunnel Junctions (MTJ) with shrinking device sizes. As a result, time dependent dielectric breakdown (TDDB) has become a major issue…

Mesoscale and Nanoscale Physics · Physics 2017-02-28 Ahmed Kamal Reza , Mohammad Khaled Hassan , Kaushik Roy

The ALICE (A Large Ion Collider Experiment) Time Projection Chamber (TPC) at CERN LHC is presently equipped with Multi Wire Proportional Chambers (MWPCs). A gating grid prevents ions produced during the gas amplification from moving into…

Instrumentation and Detectors · Physics 2017-06-28 Alexander Deisting , Chilo Garabatos

This review consolidates experimental, theoretical, and simulation work examining the behavior of high-field devices and the fundamental process of vacuum arc initiation, commonly referred to as breakdown. Detailed experimental observations…

The layered transition metal trihalide $\alpha$-RuCl$_3$ has been studied extensively in recent years as a promising candidate for a proximate Kitaev quantum spin liquid state. In high quality samples, a complete structural transition from…

Materials Science · Physics 2026-01-05 Paige Harford , Ezekiel Horsley , Subin Kim , Young-June Kim