'Beam current' diaporamas de présentation

5 MeV Mott Polarimeter Progress

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USPAS Course on Recirculating Linear Accelerators

USPAS Course on Recirculating Linear Accelerators. G. A. Krafft and L. Merminga Jefferson Lab Lecture 8. Outline. Introduction Cavity Fundamental Parameters RF Cavity as a Parallel LCR Circuit Coupling of Cavity to an rf Generator Equivalent Circuit for a Cavity with Beam Loading

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eRHIC Overview

eRHIC Overview. JLEIC Collaboration Meeting April 3 , 2017 Ferdinand Willeke. Outline. eRHIC Requirements eRHIC Concept Accelerator Layout Luminosity IR Design Storage Ring Lattice Beam-Dynamics Issues Cooling Polarization Injectors Timeline. Requirements on an EIC.

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The ESS Linac

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Nuovo nucleare - Reattori sottocritici descrizione ADS

Nuovo nucleare - Reattori sottocritici descrizione ADS. Nuovo nucleare - Reattori sottocritici descrizione ADT. ACCELERATORE. beam line. RAFFINAZIONE/FABBRICAZIONE. Turbina/alternatore. BOP. TARGET. SOTTOCRITICO.

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Power requirementS for the LHC harmonic cavities with the full-detuning scheme

P. Baudrenghien , T. Mastoridis, CERN BE-RF 2nd LHC Harmonic Cavity meeting, May 27 th ,2013. Power requirementS for the LHC harmonic cavities with the full-detuning scheme. Content. Beam-Cavity-TX interaction formula

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Basic BPM Hardware Theory

Basic BPM Hardware Theory. Jim Steimel. Wall Current. Charge in a cylindrical perfectly conducting pipe produces an equal and opposite image charge at the edge of the conductor. This image charge follows a moving packet of charge through the cylinder. -. -. -. -. -. +. +. +. +. +. +.

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A Circular Higgs Factory

A Circular Higgs Factory. H.P. Geng , Y.Y. Guo , Q. Qin , Y.W. An, D. Wang, Y.S. Xu , C. Zhang Institute of High Energy Physics, CAS. Outline. Physics motivation Parameters determination and limits Preliminary design of accelerator Further studies Conclusion.

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Experience with High Power Operation at PSI M.Seidel, PSI HB2008, Nashville

Experience with High Power Operation at PSI M.Seidel, PSI HB2008, Nashville. PSI High Power - Outline. overview of the facility comments on CW acceleration with cyclotrons [CW vs. pulsed operation, resonators, electrostatic elements, interruption and recovery statistics]

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Focal Plane Scanner

Focal Plane Scanner. Jeff Martin University of Winnipeg with: Jie Pan, Peiqing Wang, David Harrison. Motivation. Q 2 determination, background studies, all done at 10 nA using tracking system. Region III operable up to 100 nA. Qweak production running 180 ?A.

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Luminosity Limitations of e-p Colliders

Luminosity Limitations of e-p Colliders. Extrapolation from HERA Experience Examples for IR Layout LINAC-Ring Limitations HERA Limitations. HERA Luminosity. 2001 PARAMETERS N p number of protons per bunch = 1 x 10 11 N e number of leptons per bunch = 3 x 10 10

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The High Intensity Proton Accelerator of the Paul Scherrer Institute

The High Intensity Proton Accelerator of the Paul Scherrer Institute. nuclear research. nano / micro technology. PSI west. Energy research. PSI east. Protons: cyclotron. Muons Pions. UCN:spallation. neutrons: spallation. Proton therapy. Elektrons: SLS. Aare. Seite 2. PSI,.

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Long-Pulse Modulator for the Superconducting RF Test Facility

Accelerator Laboratory. Long-Pulse Modulator for the Superconducting RF Test Facility. M. Akemoto, H. Honma, H. Nakajima, T. Shidara, S. Fukuda High Energy Accelerator Research Organization(KEK) RPIA 2006, March, 7. Table of Contents. Accelerator Laboratory. STF plan

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Measuring the Attenuation Coefficient of Biological Materials

Measuring the Attenuation Coefficient of Biological Materials. Sarah DeLeo Kyle Gautreaux Shreya Purohit Eric Richard. Introductions. Many uses for medical physics Radiation therapy, x-ray imaging, etc. Attenuation occurs when photons pass through a material.

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Linac 4 Diagnostics

Linac 4 Diagnostics. L4: K. Hanke, M.Pasini (requirements, specifications, integration) AB/BI: U.Raich et al. (technical responsibility). General Remarks. We divide the diagnostics in two main categories: commissioning and day-to-day operation.

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Motivation for a H - Charge Exchange Injection Lattice Perturbations and their Compensation

Beam Optics and Painting Schemes C. Bracco , C. Carli, B. Goddard, J.-B. Lallement , M.Martini , W. Weterings. Motivation for a H - Charge Exchange Injection Lattice Perturbations and their Compensation Injection Painting Apertures Typical Simulation Results

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High Energy Plume Impingement on Spacecraft Systems AFOSR Telecon

High Energy Plume Impingement on Spacecraft Systems AFOSR Telecon. Jarred Alexander Young October 22, 2012. Electrical Issues. All components biased relative to ground May prevent beam generation Beam Diagnostics thrown off by Decel Grid Bias

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