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Related papers: Modeling of the positron sources: an experiment-ba…

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The high design luminosity of the SuperKEKB electron-positron collider will result in challenging levels of beam-induced backgro\ unds in the interaction region. Understanding and mitigating these backgrounds is critical to the success of…

Several designs for high-energy Lepton Colliders serving as Higgs factories but extendable to higher energies up to the TeV range are under discussion. The most mature design is the International Linear Collider (ILC), but also the Compact…

High Energy Physics - Phenomenology · Physics 2023-09-28 Gudrid Moortgat-Pick , Sabine Riemann , Peter Sievers , Carmen Tenholt

We report the instrumentation of a new positron diffractometer that is connected to the high-intensity positron source NEPOMUC. Crucial elements for the adaption of the positron beam are presented, which include the magnetic field…

Instrumentation and Detectors · Physics 2021-11-05 Matthias Dodenhöft , Sebastian Vohburger , Christoph Hugenschmidt

The generation and capture of polarized positrons at a source with a superconducting helical undulator having 4.3 cm period and 500 GeV electron drive beam have been simulated. The positron polarization has been calculated for the different…

Accelerator Physics · Physics 2013-01-09 Andriy Ushakov , Gudrid Moortgat-Pick , Sabine Riemann , Wanming Liu , Wei Gai

A hybrid positron source, consisting of a crystal as electron to photon converter and a amorphous target, is a candidate to relax heat load problem for high intensity positron sources. In this article we report status of experimental study…

Accelerator Physics · Physics 2012-03-07 Tohru Takahashi

We describe a novel design for an intense source of slow positrons based on pair production with a beam of electrons from a 10 MeV accelerator hitting a thin target at a low incidence angle. The positrons are collected with a set of coils…

High Energy Physics - Experiment · Physics 2009-11-10 P. Perez , A. Rosowsky

The International Linear Collider is a planned electron-positron linear collider with its positron source producing positrons by aiming undulator radiation onto a rotating target. The resulting, highly divergent positron beam requires…

Accelerator Physics · Physics 2023-09-06 M. Formela , N. Hamann , G. Moortgat-Pick , G. Loisch , M. Mewes , M. Thévenet , J. Osterhoff , G. Boyle

Monte Carlo simulations of slow positron production via energetic electron interaction with a solid target have been performed. The aim of the simulations was to determine the expected slow positron beam intensity from a low energy, high…

Accelerator Physics · Physics 2015-05-27 B. E. O'Rourke , N. Hayashizaki , A. Kinomura , R. Kuroda , E. Minehara , T. Ohdaira , N. Oshima , R. Suzuki

The full exploitation of the physics potential of a future Linear Collider requires the development of polarised positron beams. A very promising scheme for the technical realisation is the use of helical undulators, generating circular…

High Energy Physics - Phenomenology · Physics 2011-09-13 Gudrid Moortgat-Pick

Positron beams, both polarized and unpolarized, are identified as essential ingredients for the experimental programs at the next generation of lepton accelerators. In the context of the hadronic physics program at Jefferson Lab (JLab),…

Nuclear Experiment · Physics 2021-09-15 A. Accardi , A. Afanasev , I. Albayrak , S. F. Ali , M. Amaryan , J. R. M. Annand , J. Arrington , A. Asaturyan , H. Atac , H. Avakian , T. Averett , C. Ayerbe Gayoso , X. Bai , L. Barion , M. Battaglieri , V. Bellini , R. Beminiwattha , F. Benmokhtar , V. V. Berdnikov , J. C. Bernauer , V. Bertone , A. Bianconi , A. Biselli , P. Bisio , P. Blunden , M. Boer , M. Bondì , K. -T. Brinkmann , W. J. Briscoe , V. Burkert , T. Cao , A. Camsonne , R. Capobianco , L. Cardman , M. Carmignotto , M. Caudron , L. Causse , A. Celentano , P. Chatagnon , J. -P. Chen , T. Chetry , G. Ciullo , E. Cline , P. L. Cole , M. Contalbrigo , G. Costantini , A. D'Angelo , L. Darmé , D. Day , M. Defurne , M. De Napoli , A. Deur , R. De Vita , N. D'Hose , S. Diehl , M. Diefenthaler , B. Dongwi , R. Dupré , H. Dutrieux , D. Dutta , M. Ehrhart , L. El Fassi , L. Elouadrhiri , R. Ent , J. Erler , I. P. Fernando , A. Filippi , D. Flay , T. Forest , E. Fuchey , S. Fucini , Y. Furletova , H. Gao , D. Gaskell , A. Gasparian , T. Gautam , F. -X. Girod , K. Gnanvo , J. Grames , G. N. Grauvoge , P. Gueye , M. Guidal , S. Habet , T. J. Hague , D. J. Hamilton , O. Hansen , D. Hasell , M. Hattawy , D. W. Higinbotham , A. Hobart , T. Horn , C. E. Hyde , H. Ibrahim , A. Ilyichev , A. Italiano , K. Joo , S. J. Joosten , V. Khachatryan , N. Kalantarians , G. Kalicy , B. Karky , D. Keller , C. Keppel , M. Kerver , M. Khandaker , A. Kim , J. Kim , P. M. King , E. Kinney , V. Klimenko , H. -S. Ko , M. Kohl , V. Kozhuharov , B. T. Kriesten , G. Krnjaic , V. Kubarovsky , T. Kutz , L. Lanza , M. Leali , P. Lenisa , N. Liyanage , Q. Liu , S. Liuti , J. Mammei , S. Mantry , D. Marchand , P. Markowitz , L. Marsicano , V. Mascagna , M. Mazouz , M. McCaughan , B. McKinnon , D. McNulty , W. Melnitchouk , A. Metz , Z. -E. Meziani , S. Migliorati , M. Mihovilovic , R. Milner , A. Mkrtchyan , H. Mkrtchyan , A. Movsisyan , H. Moutarde , M. Muhoza , C. Muñoz Camacho , J. Murphy , P. Nadel-Turonski , E. Nardi , J. Nazeer , S. Niccolai , G. Niculescu , R. Novotny , J. F. Owens , M. Paolone , L. Pappalardo , R. Paremuzyan , B. Pasquini , E. Pasyuk , T. Patel , I. Pegg , C. Peng , D. Perera , M. Poelker , K. Price , A. J. R. Puckett , M. Raggi , N. Randazzo , M. N. H. Rashad , M. Rathnayake , B. Raue , P. E. Reimer , M. Rinaldi , A. Rizzo , Y. Roblin , J. Roche , O. Rondon-Aramayo , F. Sabatié , G. Salmè , E. Santopinto , R. Santos Estrada , B. Sawatzky , A. Schmidt , P. Schweitzer , S. Scopetta , V. Sergeyeva , M. Shabestari , A. Shahinyan , Y. Sharabian , S. Širca , E. S. Smith , D. Sokhan , A. Somov , N. Sparveris , M. Spata , H. Spiesberger , M. Spreafico , S. Stepanyan , P. Stoler , I. Strakovsky , R. Suleiman , M. Suresh , P. Sznajder , H. Szumila-Vance , V. Tadevosyan , A. S. Tadepalli , A. W. Thomas , M. Tiefenback , R. Trotta , M. Ungaro , P. Valente , M. Vanderhaeghen , L. Venturelli , H. Voskanyan , E. Voutier , B. Wojtsekhowski , M. H. Wood , S. Wood , J. Xie , W. Xiong , Z. Ye , M. Yurov , H. -G. Zaunick , S. Zhamkochyan , J. Zhang , S. Zhang , S. Zhao , Z. W. Zhao , X. Zheng , J. Zhou , C. Zorn

We report on an indirect and non-invasive method to simultaneously characterise the energy-dependent emittance and source size of ultra-relativistic positron beams generated during the propagation of a laser-wakefield accelerated electron…

Relativistic positron sources with high spin polarization have important applications in nuclear and particle physics and many frontier fields. However, it is challenging to produce dense polarized positrons. Here we present a simple and…

Plasma Physics · Physics 2024-05-22 Xing-Long Zhu , Wei-Yuan Liu , Tong-Pu Yu , Min Chen , Su-Ming Weng , Wei-Min Wang , Zheng-Ming Sheng

Electron microscopy is a powerful tool for studying the properties of materials down to their atomic structure. In many cases, the quantitative interpretation of images requires simulations based on atomistic structure models. These…

Fast simulation tools are highly appreciated in particle physics phenomenology studies, especially in the exploration of the physics potential of future experimental facilities. The Circular Electron Positron Collider is a proposed Higgs…

High Energy Physics - Experiment · Physics 2017-12-29 Cheng Chen , Xin Mo , Michele Selvaggi , Qiang Li , Gang Li , Manqi Ruan , Xinchou Lou

Protons and heavy-ion beams at unprecedented energies are brought into collisions in the CERN Large Hadron Collider for high-energy experiments. The LHC multi-stage collimation system is designed to provide protection against regular and…

Accelerator Physics · Physics 2020-11-11 N. Fuster-Martínez

A photon-positron conversion target of the undulator or laser based polarized positron source is optimized using a modified GEANT-3 program adapted to count the spin transfer. High intensity positron beam with around 0.75 polarisation could…

Instrumentation and Detectors · Physics 2009-02-16 V. Gharibyan

Spallation source dedicated for neutron scattering experiments, as well as multi-purpose facilities serving several applications call for pulsed mode operation of a high intensity proton linac. There is general agreement on the…

Accelerator Physics · Physics 2007-05-23 Alban Mosnier

In the baseline design of the International Linear Collider (ILC) an undulator-based source is foreseen for the positron source in order to match the physics requirements. The recently chosen first energy stage with sqrt(s)=250 GeV requires…

The PSI Positron Production (P$^3$ or P-cubed) experiment is a demonstrator for a e+ source and capture system with potential to improve the state-of-the-art e+ yield by an order of magnitude. The experiment is driven by the FCC-ee injector…

The ILC baseline design for the positron source is based on radiation from a helical undulator to produce positrons in a thin target. Since the photon beam created in the helical undulator is circularly polarized, the generated positron…

Accelerator Physics · Physics 2017-08-23 F. Staufenbiel , O. S. Adeyemi , V. Kovalenko , G. Moortgat-Pick , L. Malysheva , S. Riemann , A. Ushakov