LCLS Conceptual Design Report - Stanford Synchrotron Radiation ...

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∆X/µm ∆Y/µm 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 〈∆X 100 2 〉 1/2 2 1/2 2 1/2 = 7.0 µm, 〈∆X 〉 = 2.6 µm, 〈∆XQUAD 〉 =24.5 µm, 〈∆φx 〉 = 318.1° BPM 50 0 −50 −100 0 20 40 60 80 100 120 〈∆Y 100 2 〉 1/2 2 1/2 2 1/2 = 7.8 µm, 〈∆Y 〉 = 1.5 µm, 〈∆YQUAD 〉 =14.2 µm, 〈∆φy 〉 = 82.0° BPM 50 0 −50 −100 0 20 40 60 80 100 120 S/m Figure 8.50 After two iterations of steps 3-7 (x rms = 7.0 µm, y rms = 7.8 µm and peak values of x pk = 17 µm, y pk = 18 µm). A new scale is used here. ∆X/µm ∆Y/µm 〈∆X 100 2 〉 1/2 2 1/2 2 1/2 = 1.7 µm, 〈∆X 〉 = 1.2 µm, 〈∆XQUAD 〉 =10.6 µm, 〈∆φx 〉 = 81.9° BPM 50 0 −50 −100 0 20 40 60 80 100 120 〈∆Y 100 2 〉 1/2 2 1/2 2 1/2 = 2.7 µm, 〈∆Y 〉 = 1.1 µm, 〈∆YQUAD 〉 = 6.9 µm, 〈∆φy 〉 = 21.1° BPM 50 0 −50 −100 0 20 40 60 80 100 120 S/m Figure 8.51 After three iterations of steps 3-7 (x rms = 1.7 µm, y rms = 2.7 µm and peak values of x pk = 5.3 µm, y pk = 6.8 µm). The raw BPM readbacks also give a clear indication as to whether the procedure is converging and when to terminate the process. As the alignment is improved, the BPM readbacks will respond less and less to energy variations. With the energy lowered to 5 GeV the BPM readings should change, with respect to the readbacks at 14.3 GeV, by
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 readings change by
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Linac Coherent Light Source (LCLS)
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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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Preface This Conceptual Design Repo
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Table of Contents 1 Executive Summa
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6. Two experiment halls L C L S C O
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2.7.1.7 Conventional Facilities L C
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3 TECHNICAL SYNOPSIS Scientific Bas
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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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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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