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The idea of using fixed-target annihilations of a high-energy positron beam on a target for producing a new, very feebly interacting particle has been exploited by the PADME experiment at LNF using the extracted beam from the LINAC in the…

We study coherent synchrotron radiation (CSR) in a perfectly conducting vacuum chamber of rectangular cross section, in a formalism allowing an arbitrary sequence of bends and straight sections. We apply the paraxial method in the frequency…

Accelerator Physics · Physics 2016-06-09 Robert L. Warnock , David A. Bizzozero

Long-term beamforming substantially reduces the channel estimation and inversion overhead of conventional massive MU-MIMO receivers; yet, its construction still hinges on the inversion of a large Hermitian matrix, whose condition number…

Signal Processing · Electrical Eng. & Systems 2026-05-05 Amirreza Kiani , Ali Rasteh , Marco Mezzavilla , Sundeep Rangan

A storage ring-based light source, Beijing Advanced Photon Source (BAPS) is proposed to store 5-GeV low-emittance electron beam and to provide high-brilliance coherent radiation. In this paper, we report our efforts of pushing down the…

Accelerator Physics · Physics 2015-10-15 Xu Gang , Jiao Yi

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 ICARUS-T600 detector is a 760-ton Liquid Argon Time Projection Chamber (LArTPC) currently operating at Fermilab as the Far Detector in the Short Baseline Neutrino (SBN) program. The SBN program is composed of three LArTPCs with a…

High Energy Physics - Experiment · Physics 2023-12-12 Anna Heggestuen

Exciting high-power resonators pose challenges such as managing power reflections, which can cause energy losses and damage system components. This is crucial for applications like Lower Hybrid Current Drive (LHCD) systems in tokamaks,…

A longitudinal beam properties, data acquisition system has been commissioned to operate in the Fermilab booster ring. This system captures real time information including beam synchronous phase, bunch length, and coupled bunch instability…

Accelerator Physics · Physics 2012-08-20 J. Steimel , C. Y. Tan

The SIS100 synchrotron as a part of the new FAIR accelerator facility at GSI should be operated at the "space charge limit" for light and heavy ion beams. Beam losses due to space charge induced resonance crossing should not exceed a few…

This paper introduces the protection of circular particle accelerators from accidental beam losses. Already the energy stored in the beams for accelerators such as the TEVATRON at Fermilab and Super Proton Synchrotron (SPS) at CERN could…

Accelerator Physics · Physics 2016-08-11 R. Schmidt

In the Rapid Cycling Synchrotron(RCS) of China Spallation Neutron Source(CSNS), transverse painting injection is employed to suppress the space-charge effects. The beta-beating caused by edge focusing of the injection bump magnets leads to…

Accelerator Physics · Physics 2018-03-16 Xiaohan Lu , Shouyan Xu , Sheng Wang

In the frame of a R\&D effort conducted by CEA toward the design and the qualification of a 5 GHz LHCD system for the ITER tokamak, two 5 GHz 500 kW/5 s windows have been designed, manufactured and tested at high power in collaboration with…

Plasma Physics · Physics 2015-03-18 Julien Hillairet , J Kim , N Faure , J Achard , L Delpech , M Goniche , S Larroque , R Magne , L Marfisi , S Park , S Poli , N Dechambre , K Vulliez

We report on fast tunability of an electromagnetic environment coupled to a superconducting coplanar waveguide resonator. Namely, we utilize a recently-developed quantum-circuit refrigerator (QCR) to experimentally demonstrate a dynamic…

The reduction of the average charge per count in the gas along with the capability to discriminate very small signals from noise can allow an efficient and long-term Resistive Plate Chamber detector operation in high radiation background…

Instrumentation and Detectors · Physics 2020-12-30 Luca Pizzimento

In order to meet the needs of Fermilabs planned post-collider experimental program, the total proton throughput of the 8 GeV Booster accelerator must be nearly doubled within the next two years. A system of 48 ramped corrector magnets has…

Accelerator Physics · Physics 2012-03-09 M. McAteer , S. Kopp , E. Prebys

The Fermilab Booster uses multi-turn beam injection with all its cavities phased such that beam sees a net zero RF voltage even when each station is at the same maxi-mum voltage. During beam capture the RF voltage is increased slowly by…

Many modern and future particle accelerators employ high gradient superconducting RF (SRF) to generate beams of high energy, high intensity and high brightness for research in high energy and nuclear physics, basic energy sciences, etc. In…

We review the recent developments which had taken place in the domain of quasi one dimensional BECs from the viewpoint of integrability. To start with, we consider the dynamics of scalar BECs in a time independent harmonic trap and observe…

Quantum Gases · Physics 2015-01-21 R. Radha , P. S. Vinayagam

The Fermilab Linac delivers 400 MeV H- beam to the rest of the accelerator chain. Providing stable intensity, energy, and emittance is key since it directly affects downstream machines. To operate high current beam, accelerators must…

Accelerator Physics · Physics 2023-07-11 R. Sharankova , M. Mwaniki , K. Seiya , M. Wesley

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