LCLS Conceptual Design Report - Stanford Synchrotron Radiation ...

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This document, and the material and data contained therein, was developed under sponsorship of the United States Government. Neither the United States nor the Department of Energy, nor the Leland Stanford Junior University, nor their employees, nor their respective contractors, subcontractors, or their employees, makes any warranty, express or implied, or assumes any liability of responsibility for accuracy, completeness or usefulness of any information, apparatus, product or process disclosed, or represents that its use will not infringe privately owned rights. Mention of any product, its manufacturer, or suppliers shall not, nor is intended to imply approval, disapproval, or fitness for any particular use. A royalty-free, nonexclusive right to use and disseminate same for any purpose whatsoever, is expressly reserved to the United States and the University.
L C L S C O N C E P T U A L D E S I G N R E P O R T List of Authors and Contributors J. Arthur, Stanford Synchrotron Radiation Laboratory, Stanford, CA, USA P. Anfinrud, National Institutes of Health, Bethesda, MD, USA P. Audebert, Laboratoire pour l'Utilisation des Lasers, Paris, France K. Bane, Stanford Linear Accelerator Center, Stanford, CA, USA I. Ben-Zvi, Brookhaven National Laboratory, Upton, NY, USA V. Bharadwaj, Stanford Linear Accelerator Center, Stanford, CA, USA R. Bionta, Lawrence Livermore National Laboratory, Livermore, CA, USA P. Bolton, Stanford Linear Accelerator Center, Stanford, CA, USA M. Borland, Argonne National Laboratory, Argonne, IL, USA P. H. Bucksbaum, University of Michigan, Ann Arbor, MI, USA R. C. Cauble, Lawrence Livermore National Laboratory, Livermore, CA, USA J. Clendenin, Stanford Linear Accelerator Center, Stanford, CA, USA M. Cornacchia, Stanford Synchrotron Radiation Laboratory, Stanford, CA, USA G. Decker, Argonne National Laboratory, Argonne, IL, USA P. Den Hartog, Argonne National Laboratory, Argonne, IL, USA S. Dierker, University of Michigan, Ann Arbor, MI, USA D. Dowell, Stanford Linear Accelerator Center, Stanford, CA, USA D. Dungan, Stanford Synchrotron Radiation Laboratory, Stanford, CA, USA P. Emma, Stanford Linear Accelerator Center, Stanford, CA, USA I. Evans, Stanford Synchrotron Radiation Laboratory, Stanford, CA, USA G. Faigel, Research Institute for Solid State Physics, Budapest, Hungary R. Falcone, University of California, Berkeley, CA, USA W.M. Fawley, Lawrence Berkeley National Laboratory, Berkeley, CA, USA M. Ferrario, Istituto Nazionale di Fisica Nucleare - Lab. Naz. di Frascati, Frascati, Italy A.S. Fisher, Stanford Linear Accelerator Center, Stanford, CA, USA R. R. Freeman, University of California, Davis, CA, USA J. Frisch, Stanford Linear Accelerator Center, Stanford, CA, USA L I S T O F A U T H O R S A N D C O N T R I B U T O R S
Page 1: Linac Coherent Light Source (LCLS)
Page 5 and 6: L C L S C O N C E P T U A L D E S I
Page 7 and 8: Preface This Conceptual Design Repo
Page 11 and 12: Table of Contents 1 Executive Summa
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Page 28 and 29: 6. Two experiment halls L C L S C O
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L C L S C O N C E P T U A L D E S I
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5 TECHNICAL SYNOPSIS FEL Parameters
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and the total peak beam power L C L
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5.4.2.2 Case II - High Charge Limit
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∆P ∆I sat pl / P / I sat pk L C
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5.9 Summary L C L S C O N C E P T U
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6 Injector TECHNICAL SYNOPSIS The i
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εn,x (µm) 4 3 2 1 4-2001 8560A95
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Quantum Yield (electrons/photon) 10
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Bz (T) 0.3 0.2 0.1 1-2002 8560A92 L
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Master Clock 9.917 MHz x8 x6 x6 Df
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1-2002 8560A198 Linac Center Line L
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B z (kG) 3 2 1 4-2001 8560A91 L C L
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γε x,y (µm) 3 2 1 0 3-2001 8560A
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γεx,y (µm) yn 10 0 -10 -10 0 10
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σ γ /γ 0 (percent) ∆N/N 0.02 0
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5 0 -5 5 0 -5 5 0 -5 L C L S C O N
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Table 6.5 PARMELA Output Parameters
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gama x (micro.m) 3 2 1 0 0 L C L S
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∆E/E 0 (%) ∆N/N 0 -1 -2 0.02 0
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〈∆E/E 0 〉 /% I pk /I pk0 0.1
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β (m) 35 30 25 20 15 10 5 0 K21_1B
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β (m) 60 50 40 30 20 10 0 L C L S
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economic reasons. L C L S C O N C E
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Phase [deg. S-band] L C L S C O N C
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New Solid-State Sub-Booster and Ele
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7.8.2 Bunch Length Diagnostics L C
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Magnet String Location Existing, Ne
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8.1 Overview 8.1.1 Introduction L C
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Mu in the pole, for mu
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Gasload (Torr-l/sec-cm) (x10 -12 )
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8.10.4 Conclusion L C L S C O N C E
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x θ j > 0 L C L S C O N C E P T U
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Quad ∆X/µm Quad ∆Y/µm −500
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∆X/µm ∆Y/µm L C L S C O N C E
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8.13.2 Undulator Cell Structure L C
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9.2 Layout and Optics 9.2.1 Experim
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Fast Valve L C L S C O N C E P T U
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0.01 10 -4 10 -6 10 -8 10 -10 10 -1
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Table 9.5 Mirror requirements L C L
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Refractive Focusing System L C L S
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Pulse Split/Delay L C L S C O N C E
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Figure 9.20 LCLS Ion Chamber L C L
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9.4.3.2 Pulse Length L C L S C O N
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9.4.3.6 Divergence L C L S C O N C
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10 Conventional Facilities TECHNICA
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1-2002 8560A198 Linac Center Line L
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Figure 10.6 Near hall floor plan 10
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11 Controls TECHNICAL SYNOPSIS The
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11.5.3 Motion Controls L C L S C O
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12.1 Procedural Overview L C L S C
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13 Environment, Safety and Health a
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Table 13-1 Hazard Identification an
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13.1 Ionizing Radiation The design
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Table 13-2 Minimum Training Require
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13.10 SLAC References L C L S C O N
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L C L S D E S I G N S T U D Y R E P
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15 TECHNICAL SYNOPSIS Work Breakdow
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A A.1 FEL-Physics A.1.1 Performance
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A.2 Photo-Injector A.2.1 Gun-Laser
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A.2.3.2 Electron Beam L C L S C O N
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A.2.4.7 Vacuum L C L S C O N C E P
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A.3.8 DL-2 A.3.8.1 Subsystem L C L
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A.4 Undulator A.4.1 Undulator A.4.1
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B Control Points B.1 Injector Contr
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C Glossary ACO Anneaux Collisions O
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