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Related papers: Seeding of proton bunch self-modulation by an elec…

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Ultrashort electron bunches are crucial for an increasing number of applications, however, diagnosing their longitudinal phase space remains a challenge. We propose a new method that harnesses the strong electric fields present in a laser…

Accelerator Physics · Physics 2016-07-21 I. Dornmair , C. B. Schroeder , K. Floettmann , B. Marchetti , A. R. Maier

The generation of very high quality electron bunches (high brightness and low energy spread) from a plasma-based accelerator in the three-dimensional blowout regime using self-injection in tailored plasma density profiles is analyzed…

Accelerator Physics · Physics 2017-11-29 X. L. Xu , F. Li , W. An , P. Yu , W. Lu , C. Joshi , W. B. Mori

Recent simulation shows that a self-modulated high energy proton bunch can excite a large amplitude plasma wakefield and accelerate an externally injected electron bunch to the energy frontier in a single stage acceleration through a long…

Accelerator Physics · Physics 2012-06-01 Guoxing Xia , Allen Caldwell , Patric Muggli

The production of ultra-bright electron bunches using ionization injection triggered by two transversely colliding laser pulses inside a beam-driven plasma wake is examined via three-dimensional (3D) particle-in-cell (PIC) simulations. The…

Accelerator Physics · Physics 2015-06-12 F. Li , J. F. Hua , X. L. Xu , C. J. Zhang , L. X. Yan , Y. C. Du , W. H. Huang , H. B. Cheng , C. X. Tang , W. Lu , C. Joshi , W. B. Mori , Y. Q. Gu

Using a periodic electron beam bunch train to resonantly excite plasma wakefields in the quasi-nonlinear (QNL) regime has distinct advantages over employing a single, higher charge bunch. Resonant excitation in the QNL regime can produce…

Accelerator Physics · Physics 2021-05-31 P. Manwani , N. Majernik , J. B. Rosenzweig

The FLASHForward experimental facility is a high-performance test-bed for precision plasma-wakefield research, aiming to accelerate high-quality electron beams to GeV-levels in a few centimetres of ionised gas. The plasma is created by…

Next-generation plasma-based accelerators can push electron bunches to gigaelectronvolt energies within centimetre distances. The plasma, excited by a driver pulse, generates large electric fields that can efficiently accelerate a trailing…

A stationary wave solution is obtained for the proton driven plasma wake field accelerator (PDPWFA). The wake field excitation by trains of equidistant proton microbunches produced due to self modulational instability has been discussed.…

Plasma Physics · Physics 2020-04-09 Mithun Karmakar , Sudip Sengupta , Nikhil Chakrabarti

We investigate beam loading and emittance preservation for a high-charge electron beam being accelerated in quasi-linear plasma wakefields driven by a short proton beam. The structure of the studied wakefields are similar to those of a…

Accelerator Physics · Physics 2018-09-14 Veronica K. Berglyd Olsen , Erik Adli , Patric Muggli

The "Advanced Proton Driven Plasma Wakefield Acceleration Experiment" (AWAKE) aims to accelerate leptons via proton-beam-driven wakefield acceleration. It comprises extensive numerical studies as well as experiments at the CERN laboratory.…

Computational Physics · Physics 2019-09-19 N. Moschüring , K. V. Lotov , K. Bamberg , F. Deutschmann , H. Ruhl

AWAKE project, a proton driven plasma wakefield acceleration (PDPWA) experiment is approved by CERN. The PDPWA scheme consists of a seeding laser, a drive beam to establish the accelerating wakefields within the plasma cell; and a witness…

Accelerator Physics · Physics 2014-06-06 Oznur Mete , Guoxing Xia , Graeme Burt , Swapan Chattopadhyay

It is shown that co-linear injection of electrons or positrons into the wakefield of the self-modulating particle beam is possible and ensures high energy gain. The witness beam must co-propagate with the tail part of the driver, since the…

We use numerical simulations to determine whether the saturation length of the self-modulation (SM) instability of a long proton bunch in plasma could be determined by measuring the radius of the bunch halo SM produces. Results show that…

Plasma Physics · Physics 2024-12-18 Arthur Clairembaud , Marlene Turner , Patric Muggli

Synchronized, independently tunable and focused $\mu$J-class laser pulses are used to release multiple electron populations via photo-ionization inside an electron-beam driven plasma wave. By varying the laser foci in the laboratory frame…

Ionization injection is attractive as a controllable injection scheme for generating high quality electron beams using plasma-based wakefield acceleration. Due to the phase dependent tunneling ionization rate and the trapping dynamics…

Plasma Physics · Physics 2016-07-20 X. L. Xu , C. J. Zhang , F. Li , Y. Wan , Y. P. Wu , J. F. Hua , C. -H. Pai , W. Lu , W. An , P. Yu , W. B. Mori , C. Joshi

Plasma accelerators driven by intense laser or particle beams provide gigavolt-per-meter accelerating fields, promising to drastically shrink particle accelerators for high-energy physics and photon science. Applications such as linear…

Accelerator Physics · Physics 2021-04-30 Carl A. Lindstrøm

Laser wakefield accelerators are on the way to provide GeV scale high-brightness electron beams for multidisciplinary applications. In the present work, electron bunches are studied in the framework of a Free-Electron Laser driven by an…

Accelerator Physics · Physics 2025-09-23 Federico Nguyen , Paolo Tomassini , Leonida A. Gizzi , Luca Giannessi , Anna Giribono

In an electron wakefield accelerator, an intense laser pulse or charged particle beam excites plasma waves. Under proper conditions, electrons from the background plasma are trapped in the plasma wave and accelerated to ultra-relativistic…

This report describes the conceptual steps in reaching the design of the AWAKE experiment currently under construction at CERN. We start with an introduction to plasma wakefield acceleration and the motivation for using proton drivers. We…

Plasma Physics · Physics 2016-08-03 A. Caldwell , E. Adli , L. Amorim , R. Apsimon , T. Argyropoulos , R. Assmann , A. -M. Bachmann , F. Batsch , J. Bauche , V. K. Berglyd Olsen , M. Bernardini , R. Bingham , B. Biskup , T. Bohl , C. Bracco , P. N. Burrows , G. Burt , B. Buttenschon , A. Butterworth , M. Cascella , S. Chattopadhyay , E. Chevallay , S. Cipiccia , H. Damerau , L. Deacon , P. Dirksen , S. Doebert , U. Dorda , E. Elsen , J. Farmer , S. Fartoukh , V. Fedosseev , E. Feldbaumer , R. Fiorito , R. Fonseca , F. Friebel , G. Geschonke , B. Goddard , A. A. Gorn , O. Grulke , E. Gschwendtner , J. Hansen , C. Hessler , S. Hillenbrand , W. Hofle , J. Holloway , C. Huang , M. Huther , D. Jaroszynski , L. Jensen , S. Jolly , A. Joulaei , M. Kasim , F. Keeble , R. Kersevan , N. Kumar , Y. Li , S. Liu , N. Lopes , K. V. Lotov , W. Lu , J. Machacek , S. Mandry , I. Martin , R. Martorelli , M. Martyanov , S. Mazzoni , M. Meddahi , L. Merminga , O. Mete , V. A. Minakov , J. Mitchell , J. Moody , A. -S. Muller , Z. Najmudin , T. C. Q. Noakes , P. Norreys , J. Osterhoff , E. Oz , A. Pardons , K. Pepitone , A. Petrenko , G. Plyushchev , J. Pozimski , A. Pukhov , O. Reimann , K. Rieger , S. Roesler , H. Ruhl , T. Rusnak , F. Salveter , N. Savard , J. Schmidt , H. von der Schmitt , A. Seryi , E. Shaposhnikova , Z. M. Sheng , P. Sherwood , L. Silva , F. Simon , L. Soby , A. P. Sosedkin , R. I. Spitsyn , T. Tajima , R. Tarkeshian , H. Timko , R. Trines , T. Tueckmantel , P. V. Tuev , M. Turner , F. Velotti , V. Verzilov , J. Vieira , H. Vincke , Y. Wei , C. P. Welsch , M. Wing , G. Xia , V. Yakimenko , H. Zhang , F. Zimmermann

An electron injector concept for laser-plasma accelerator was developed in ref [1] and [2] ; it relies on the use of counter-propagating ultrashort laser pulses. In [2], the scheme is as follows: the pump laser pulse generates a large…

Plasma Physics · Physics 2009-11-13 C. Rechatin , J. Faure , A. Lifschitz , V. Malka , E. Lefebvre
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