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We report on a search for the process $p\bar{p}\to \gamma+W/Z$ with $W/Z\to q\bar{q}$ in events containing two jets and a photon at the center-of-mass energy $\sqrt{s}=1.96$ TeV, using 184 pb$^{-1}$ of data collected by the CDF II detector.…

High Energy Physics - Experiment · Physics 2010-05-12 CDF Collaboration , T. Aaltonen

We present proof-of-operation for a new method of electron thermometry using microwave impedance of a hafnium micro-absorber. The new method leads to an ultimate THz-range detector suitable for microwave readout and frequency division…

Instrumentation and Detectors · Physics 2019-11-27 A. V. Merenkov , V. I. Chichkov , A. B. Ermakov , A. V. Ustinov , S. V. Shitov

The HARP system of resistive plate chambers (RPCs) was designed to perform particle identification by the measurement of the difference in the time-of-flight of different particles. In previous papers an apparent discrepancy was shown…

First measurements are presented from a newly commissioned two-photon absorption (TPA) setup at Nikhef. The characterisation of the various components of the system is discussed. Two planar silicon sensors, one being electron collecting and…

Instrumentation and Detectors · Physics 2022-02-23 R. Geertsema , K. Akiba , M. van Beuzekom , T. Bischoff , K. Heijhoff , H. Snoek

Accurate identification of charged pions and kaons is essential for precision measurements in relativistic heavy-ion collisions, but becomes increasingly challenging at intermediate and high transverse momentum due to the overlap between…

Instrumentation and Detectors · Physics 2026-03-05 Shaowei Lan , Bijun Fan , Like Liu

We analyze the performance of graphene microstructures as thermal photon detectors and deduce the range of parameters that define a linear response. The saturation effects of a graphene thermal detector that operates beyond the linear range…

Mesoscale and Nanoscale Physics · Physics 2014-01-22 Chris B. McKitterick , Daniel E. Prober , Boris S. Karasik

We consider the free carrier dispersion effect in a semiconductor nanocavity in the limit of discrete photoexcited electron-hole pairs. This analysis reveals the possibility of ultrafast, incoherent transduction and gain from a single…

A unique feature of gas xenon electroluminescent time projection chambers (GXeEL TPCs) in $0\nu\beta\beta$ searches is their ability to reconstruct event topology, in particular to distinguish "single-electron" from "double-electron"…

Instrumentation and Detectors · Physics 2026-04-03 J. J. Gómez-Cadenas , L. Arazi , M. Elorza , Z. Freixa , F. Monrabal , A. Pazos , J. Renner , S. R. Soleti , S. Torelli

We show that the sensitivity of antenna-coupled field-effect transistors (FETs) to terahertz (THz) radiation improves continuously with decreasing temperature. The noise-equivalent power (NEP) of 540 GHz patch-antenna-coupled FETs decreases…

Direct photons provide a insightful tool to study the different stages of a heavy ion collision, especially the formation of a quark-gluon plasma, without being influenced by the strong interaction and hadronization processes. The yield of…

Nuclear Experiment · Physics 2007-05-23 Haijiang Gong

Dual-phase liquid-xenon time projection chambers (LXe TPCs) deploying a few tonnes of liquid are presently leading the search for WIMP dark matter. Scaling these detectors to 10-fold larger fiducial masses, while improving their sensitivity…

Instrumentation and Detectors · Physics 2024-09-17 G. Martínez-Lema , A. Roy , A. Breskin , L. Arazi

Single photon detectors (SPDs) are essential technology in quantum science, quantum network, biology, and advanced imaging. To detect the small quantum of energy carried in a photon, conventional SPDs rely on energy excitation across either…

Novel high efficiency fast-neutron detectors were suggested for fan-beam tomography applications. They combine multi-layer polymer converters in gas medium, coupled to thick gaseous electron multipliers (THGEM). In this work we discuss the…

Instrumentation and Detectors · Physics 2015-06-11 M. Cortesi , R. Zboray , R. Adams , V. Dangendorf , A. Breskin , S. Mayer , H. Hoedlmoser , H. -M. Prasser

The capabilities of liquid argon time projection chambers (LArTPCs) to reconstruct the spatial and calorimetric information of neutrino events have made them the detectors of choice in a number of experiments, specifically those looking to…

We have developed a dedicated front-end-electronics board for a high-pressure xenon gas time projection chamber for a neutrinoless double-beta decay search. The ionization signal is readout by detecting electroluminescence photons with…

Instrumentation and Detectors · Physics 2020-09-17 K. Z. Nakamura , S. Ban , A. K. Ichikawa , M. Ikeno , K. D. Nakamura , T. Nakaya , S. Obara , S. Tanaka , T. Uchida , M. Yoshida

Spurious-electron signals in dual-phase noble-liquid time projection chambers have been observed in both xenon and argon Time Projection Chambers (TPCs). This paper presents the first comprehensive study of spurious electrons in argon,…

High Energy Physics - Experiment · Physics 2025-08-01 50 Collaboration , P. Agnes , I. F. Albuquerque , T. Alexander , A. K. Alton , M. Ave , H. O. Back , G. Batignani , E. Berzin , K. Biery , V. Bocci , W. M. Bonivento , B. Bottino , S. Bussino , M. Cadeddu , M. Cadoni , F. Calaprice , A. Caminata , M. D. Campos , N. Canci , M. Caravati , N. Cargioli , M. Cariello , M. Carlini , V. Cataudella , P. Cavalcante , S. Cavuoti , S. Chashin , A. Chepurnov , C. Cicalò , G. Covone , D. D'Angelo , S. Davini , A. De Candia , S. De Cecco , G. De Filippis , G. De Rosa , A. V. Derbin , A. Devoto , M. D'Incecco , C. Dionisi , F. Dordei , M. Downing , D. D'Urso , M. Fairbairn , G. Fiorillo , D. Franco , F. Gabriele , C. Galbiati , C. Ghiano , C. Giganti , G. K. Giovanetti , A. M. Goretti , G. Grilli di Cortona , A. Grobov , M. Gromov , M. Guam , M. Gulino , B. R. Hackett , K. Herner , T. Hessel , B. Hosseini , F. Hubaut , T. Hugues , E. V. Hungerford , A. Ianni , V. Ippolito , K. Keeter , C. L. Kendziora , M. Kimura , I. Kochanek , D. Korablev , G. Korga , A. Kubankin , M. Kuss , M. Kuźniak , M. La Commara , M. Lai , X. Li , M. Lissia , G. Longo , O. Lychagina , I. N. Machulin , L. P. Mapelli , S. M. Mari , J. Maricic , A. Messina , R. Milincic , J. Monroe , M. Morrocchi , V. N. Muratova , P. Musico , A. O. Nozdrina , A. Oleinik , F. Ortica , L. Pagani , M. Pallavicini , L. Pandola , E. Pantic , E. Paoloni , K. Pelczar , N. Pelliccia , S. Piacentini , A. Pocar , M. Poehlmann , S. Pordes , S. S. Poudel , P. Pralavorio , D. Price , F. Ragusa , M. Razeti , A. Razeto , A. L. Renshaw , M. Rescigno , J. Rode , A. Romani , D. Sablone , O. Samoylov , E. Sandford , W. Sands , S. Sanfilippo , C. Savarese , B. Schlitzer , D. A. Semenov , A. Shchagin , A. Sheshukov , M. D. Skorokhvatov , O. Smirnov , A. Sotnikov , R. Stefanizzi , S. Stracka , C. Sunny , Y. Suvorov , R. Tartaglia , G. Testera , A. Tonazzo , E. V. Unzhakov , A. Vishneva , R. B. Vogelaar , M. Wada , H. Wang , Y. Wang , S. Westerdale , M. M. Wojcik , X. Xiao , C. Yang , G. Zuzel

We analyze the operation of a resonant detector of terahertz (THz) radiation based on a two-dimensional electron gas (2DEG) channel with split gates. The side gates are used for the excitation of plasma oscillations by incoming THz…

Other Condensed Matter · Physics 2009-11-13 V. Ryzhii , A. Satou , T. Otsuji , M. S. Shur

The investigation of the energy frontier in physics requires novel concepts for future colliders. The idea of a muon collider is very appealing since it would allow to study particle collisions at up to tens of TeV energy, while offering a…

Rare event searches such as neutrinoless double beta decay and Weakly Interacting Massive Particle detection require ultra-low background detectors. Radon contamination is a significant challenge for these experiments, which employ highly…

Instrumentation and Detectors · Physics 2025-08-11 nEXO Collaboration , A. Anker , P. A. Breur , B. Mong , P. Acharya , A. Amy , E. Angelico , I. J. Arnquist , A. Atencio , J. Bane , V. Belov , E. P. Bernard , T. Bhatta , A. Bolotnikov , J. Breslin , J. P. Brodsky , S. Bron , E. Brown , T. Brunner , B. Burnell , E. Caden , L. Q. Cao , G. F. Cao , D. Cesmecioglu , D. Chernyak , M. Chiu , R. Collister , T. Daniels , L. Darroch , R. DeVoe , M. L. di Vacri , Y. Y. Ding , M. J. Dolinski , A. Dragone , B. Eckert , M. Elbeltagi , A. Emara , W. Fairbank , N. Fatemighomi , B. Foust , Y. S. Fu , D. Gallacher , N. Gallice , G. Giacomini , W. Gillis , A. Gorham , R. Gornea , G. Gratta , Y. D. Guan , C. A. Hardy , S. Hedges , M. Heffner , E. Hein , J. D. Holt , A. Iverson , X. S. Jiang , A. Karelin , D. Keblbeck , I. Kotov , A. Kuchenkov , K. S. Kumar , A. Larson , M. B. Latif , K. G. Leach , B. G. Lenardo , A. Lennarz , D. S. Leonard , K. Leung , H. Lewis , G. Li , X. Li , Z. Li , C. Licciardi , R. Lindsay , R. MacLellan , S. Majidi , C. Malbrunot , M. Marquis , J. Masbou , M. Medina-Peregrina , S. Mngonyama , D. C. Moore , X. E. Ngwadla , K. Ni , A. Nolan , S. C. Nowicki , J. C. Nzobadila Ondze , A. Odian , J. L. Orrell , G. S. Ortega , C. T. Overman , L. Pagani , H. Peltz Smalley , A. Perna , A. Piepke , A. Pocar , V. Radeka , E. Raguzin , R. Rai , H. Rasiwala , D. Ray , S. Rescia , F. Retiére , G. Richardson , N. Rocco , R. Ross , P. C. Rowson , R. Saldanha , S. Sangiorgio , S. Sekula , T. Shetty , L. Si , F. Spadoni , V. Stekhanov , X. L. Sun , S. Thibado , T. Totev , S. Triambak , R. H. M. Tsang , O. A. Tyuka , E. van Bruggen , M. Vidal , S. Viel , M. Walent , H. Wang , Q. D. Wang , Y. G. Wang , M. Watts , M. Wehrfritz , W. Wei , L. J. Wen , U. Wichoski , S. Wilde , M. Worcester , X. M. Wu , H. Xu , H. B. Yang , L. Yang , M. Yu , O. Zeldovich , J. Zhao
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