PPT-potential CERN facilities to study proton-driven plasma acceleration

potential CERN facilities to study protondriven plasma acceleration Frank Zimmermann Munich MPI 9 December 2008 CTF3 e xisting accelerator chain LHC beam PS booster PS SPS LHC final momentum . Outline. Introduction. AWAKE in CNGS. Planning. Ongoing Work. Summary. Edda Gschwendtner, CERN. 2. Introduction. AWAKE . – A Proton Driven Plasma Wakefield Acceleration Experiment at . CERN. Proof-of-principle R&D experiment proposed at CERN. . Edda . Gschwendtner, CERN. Outline. Motivation. AWAKE at CERN. AWAKE Experimental Layout: 1. st. Phase . AWAKE . Experimental Layout: . 2. nd. . Phase. Experimental Facility at CERN. Electron Source. I. nstability. Long proton beam. Neutral plasma. Affects long drive beams.. +. +. +. +. +. +. -. -. -. Microbunches are spaced . λ. p. . . . apart. .. Charge density increased.. Micro bunch lengths are much . Erik Adli (University of Oslo). For the FACET E200 collaboration. CLIC Beam Dynamics meeting. CERN, Sep 5 2012. Introduction. 2. Beam-driven plasma-wake field acceleration. Principle of beam-driven plasma-. A.S. 5.1.1 – 5.1.4 due Monday. Reading reference: chapter 16. Question 16.1a. . Electric Potential Energy I . a). . proton. b). . electron. c). . both feel the same force. d) neither – there is no force. 21. Al with resonance elastic and inelastic scattering using an active target. B. . Fernández-Domínguez. (Univ. Santiago de . Compostela. , Spain). Olof. . Tengblad. (CSIC-Madrid, Spain). M. . Caamaño. Robert L. Merlino and Su-Hyun Kim . University of Iowa. Guru . Ganguli. U. S. Naval Research Laboratory. 1. APS DPP Mini-Conference on Nonlinear Effects in . Geospace. Plasmas November 9, 2015. Introduction. 21. Al with resonance elastic and inelastic scattering using an active target. B. . Fernández-Domínguez. (Univ. Santiago de . Compostela. , Spain). Olof. . Tengblad. (CSIC-Madrid, Spain). M. . Caamaño. SuperDARN. Mark Lester. 1. , Adrian Grocott. 1,2. , Suzie Imber. 3. , Steve Milan. 1. , Mick Denton. 4. and Joe Borovsky. 5. . 1. Physics and Astronomy, University of Leicester, Leicester, United Kingdom. . Long-range c orrelations in driven systems David Mukamel Outline Will discuss two examples where long-range correlations show up a nd consider some consequences Example I : Effect of a local drive on the Edda Gschwendtner, CERN. w. ith input from A. Caldwell, P. . . Crivelli. , A. Pardons, A. Petrenko, S. . Gninenko. , . M. . Wing . 1. Outline. Introduction to AWAKE. Physics case for a fixed target experiment a la NA64 with AWAKE-like electron beam.. 1. Françoise BEZERRA, CNES, France (WP Leader), . Arto JAVANAINEN. , JYU, Finland (WP Deputy Leader). G-RAD(NEXT), May 4th 2022. https://indico.cern.ch/event/1095485/. . WP10 Heavy-ion and proton facilities – beam allocation. What is the future?. Is it useful for HEP?. Nicolas . Delerue. LAL. How it works (for electrons)? (1/2). A gas volume (at low density/pressure: ~mbar) will be used to create the plasma.. This volume is ionised by a beam (laser, particles) at high power and ultra-short (duration: . Dave Einolf, Managing Director, Endeavour EHS. Nick Ashley, Ph.D., P.E. Global Director, Process Safety, W. R. Grace & Co.. Lu Menghini, CPSA, Senior Audit Manager, Operations, Internal Audit, bp.