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Chapter 3: Front Ends and Insertion Devices
Advanced Photon Source Upgrade Project Final Design Report May 2019 Chapter 3: Front Ends and Insertion Devices Document Number : APSU-2.01-RPT-003 ICMS Content ID : APSU_2032071 Advanced Photon Source Upgrade Project 3–ii • Table of Contents Table of Contents 3 Front Ends and Insertion Devices 1 3-1 Introduction . 1 3-2 Front Ends . 2 3-2.1 High Heat Load Front End . 6 3-2.2 Canted Undulator Front End . 11 3-2.3 Bending Magnet Front End . 16 3-3 Insertion Devices . 20 3-3.1 Storage Ring Requirements . 22 3-3.2 Overview of Insertion Device Straight Sections . 23 3-3.3 Permanent Magnet Undulators . 24 3-3.4 Superconducting Undulators . 30 3-3.5 Insertion Device Vacuum Chamber . 33 3-4 Bending Magnet Sources . 36 References 39 Advanced Photon Source Upgrade Project List of Figures • 3–iii List of Figures Figure 3.1: Overview of ID and BM front ends in relation to the storage ring components. 2 Figure 3.2: Layout of High Heat Load Front End for APS-U. 6 Figure 3.3: Model of the GRID XBPM for the HHL front end. 8 Figure 3.4: Layout of Canted Undulator Front End for APS-U. 11 Figure 3.5: Model of the GRID XBPM for the CU front end. 13 Figure 3.6: Horizontal fan of radiation from different dipoles for bending magnet beamlines. 16 Figure 3.7: Layout of Original APS Bending Magnet Front End in current APS. 17 Figure 3.8: Layout of modified APSU Bending Magnet Front End to be installed in APSU. -
Insertion Devices Lecture 4 Undulator Magnet Designs
Insertion Devices Lecture 4 Undulator Magnet Designs Jim Clarke ASTeC Daresbury Laboratory Hybrid Insertion Devices – Inclusion of Iron Simple hybrid example Top Array e- Bottom Array 2 Lines of Magnetic Flux Including a non-linear material like iron means that simple analytical formulae can no longer be derived – linear superposition no longer works! Accurate predictions for particular designs can only be made using special magnetostatic software in either 2D (fast) or 3D (slow) e- 3 Field Levels for Hybrid and PPM Insertion Devices Assuming Br = 1.1T and gap of 20 mm When g/u is small the impact of the iron is very significant 4 Introduction We now have an understanding for how we can use Permanent Magnets to create the sinusoidal fields required by Insertion Devices Next we will look at creating more complex field shapes, such as those required for variable polarisation Later we will look at other technical issues such as the challenge of in-vacuum undulators, dealing with the large magnetic forces involved, correcting field errors, and also how and why we might cool undulators to ~150K Finally, electromagnetic alternatives will be considered 5 Helical (or Elliptical) Undulators for Variable Polarisation We need to include a finite horizontal field of the same period so the electron takes an elliptical path when it is viewed head on We want two orthogonal fields of equal period but of different amplitude and phase 3 independent variables Three independent variables are required for the arbitrary selection of any polarisation state -
A Review of High-Gain Free-Electron Laser Theory
atoms Review A Review of High-Gain Free-Electron Laser Theory Nicola Piovella 1,* and Luca Volpe 2 1 Dipartimento di Fisica “Aldo Pontremoli”, Università degli Studi di Milano, Via Celoria 16, 20133 Milano, Italy 2 Centro de Laseres Pulsados (CLPU), Parque Cientifico, 37185 Salamanca, Spain; [email protected] * Correspondence: [email protected] Abstract: High-gain free-electron lasers, conceived in the 1980s, are nowadays the only bright sources of coherent X-ray radiation available. In this article, we review the theory developed by R. Bonifacio and coworkers, who have been some of the first scientists envisaging its operation as a single-pass amplifier starting from incoherent undulator radiation, in the so called self-amplified spontaneous emission (SASE) regime. We review the FEL theory, discussing how the FEL parameters emerge from it, which are fundamental for describing, designing and understanding all FEL experiments in the high-gain, single-pass operation. Keywords: free-electron laser; X-ray emission; collective effects 1. Basic Concepts The free-electron laser is essentially a device that transforms the kinetic energy of a relativistic electron beam (e-beam) into e.m. radiation [1–4]. The e-beam passing through a transverse periodic magnetic field oscillates in a direction perpendicular to the magnetic Citation: Piovella, N.; Volpe, L. field and the propagation axis, and emits radiation confined in a narrow cone along the A Review of High-Gain Free-Electron propagation direction. The periodic magnetic field is provided by the so-called undulator, an Laser Theory. Atoms 2021, 9, 28. insertion device usually realized with two arrays of permanent magnets with alternating https://doi.org/10.3390/atoms9020028 polarities (see Figure1) or with two helical coils with current circulating in opposite directions. -
Third-Generation Synchrotron X-Ray Diffraction of 6- M Crystal of Raite, Na
Proc. Natl. Acad. Sci. USA Vol. 94, pp. 12263–12267, November 1997 Geology Third-generation synchrotron x-ray diffraction of 6-mm crystal of raite, 'Na3Mn3Ti0.25Si8O20(OH)2z10H2O, opens up new chemistry and physics of low-temperature minerals (crystal structureymicrocrystalyphyllosilicate) JOSEPH J. PLUTH*, JOSEPH V. SMITH*†,DMITRY Y. PUSHCHAROVSKY‡,EUGENII I. SEMENOV§,ANDREAS BRAM¶, CHRISTIAN RIEKEL¶,HANS-PETER WEBER¶, AND ROBERT W. BROACHi *Department of Geophysical Sciences, Center for Advanced Radiation Sources, GeologicalySoilyEnvironmental, and Materials Research Science and Engineering Center, 5734 South Ellis Avenue, University of Chicago, Chicago, IL 60637; ‡Department of Geology, Moscow State University, Moscow, 119899, Russia; §Fersman Mineralogical Museum, Russian Academy of Sciences, Moscow, 117071, Russia; ¶European Synchrotron Radiation Facility, BP 220, 38043, Grenoble, France; and UOP Research Center, Des Plaines, IL 60017 Contributed by Joseph V. Smith, September 3, 1997 ABSTRACT The crystal structure of raite was solved and the energy and metal industries, hydrology, and geobiology. refined from data collected at Beamline Insertion Device 13 at Raite lies in the chemical cooling sequence of exotic hyperal- the European Synchrotron Radiation Facility, using a 3 3 3 3 kaline rocks of the Kola Peninsula, Russia, and the 65 mm single crystal. The refined lattice constants of the Monteregian Hills, Canada (2). This hydrated sodium- monoclinic unit cell are a 5 15.1(1) Å; b 5 17.6(1) Å; c 5 manganese silicate extends the already wide range of manga- 5.290(4) Å; b 5 100.5(2)°; space group C2ym. The structure, nese crystal chemistry (3), which includes various complex including all reflections, refined to a final R 5 0.07. -
The U.S. Department of Energy's Ten-Year-Plans for the Office Of
U.S. DEPARTMENT OF ENERGY The U.S. Department of Energy’s Ten-Year-Plans for the Office of Science National Laboratories FY 2019 FY 2019 Annual Laboratory Plans for the Office of Science National Laboratories i Table of Contents Introduction ................................................................................................................................................................1 Ames Laboratory ........................................................................................................................................................3 Lab-at-a-Glance ......................................................................................................................................................3 Mission and Overview ............................................................................................................................................3 Core Capabilities .....................................................................................................................................................4 Science Strategy for the Future ..............................................................................................................................8 Infrastructure .........................................................................................................................................................8 Argonne National Laboratory ................................................................................................................................. -
Insertion Devices at Diamond Light Source: a Retrospective Plus Future Developments
TUPAB116 Proceedings of IPAC2017, Copenhagen, Denmark INSERTION DEVICES AT DIAMOND LIGHT SOURCE: A RETROSPECTIVE PLUS FUTURE DEVELOPMENTS Z. Patel, E. C. M. Rial, A. George, S. Milward, A. J. Rose, R. P. Walker, and J. H. Williams Diamond Light Source, Didcot, UK Abstract Table 1: Installed IDs for Phase I of DLS. Peak field is given for IVU devices at 5 mm gap and I06 at 15 mm gap. 2017 marks the tenth year of Diamond operation, during which time all insertion device straights have been filled. Di- Beam ID type Period No. of Peak Field amond Light Source is a third generation, 3 GeV facility that -line [mm] Periods [T] boasts 29 installed insertion devices. Most room temperature devices have been designed, manufactured and measured I02 IVU 23 85 0.92 in-house, and progress has been made in structure design I03 IVU 21 94 0.86 and control systems to ensure new devices continue to meet I04 IVU 23 85 0.92 stringent requirements placed upon them. The ‘completion’ I06a APPLE-II 64 33 1.10 of the storage ring is not, however, the end of activity for I15 SCW 60 22.5 3.5 the ID group at Diamond, as beamlines map out potential I16 IVU 27 73 0.98 upgrade paths to Cryogenic Permanent Magnet Undulators I18 IVU 27 73 0.98 (CPMUs) and SuperConducting Undulators (SCUs). This paper traces the progress of ID design at Diamond, and maps Diamond were IVUs of periods 21 mm - 25 mm, and were out future projects such as the upgrade to CPMUs and the a continuation of the design of the Phase I devices, extra challenges of designing a fixed-gap mini-wiggler to replace constraints were being placed on future IDs that meant that a sextupole in the main storage ring lattice. -
Argonne National Laboratory
AT A GLANCE: ARGONNE NATIONAL LABORATORY Argonne National Laboratory accelerates science and technology (S&T) to drive U.S. prosperity and security. The laboratory is recognized for seminal discoveries in fundamental science, innovations in energy technologies, leadership in scientific computing and analysis, and excellence in stewardship of national scientific user facilities. Argonne’s basic research drives advances in materials science, chemistry, physics, biology, and environmental science. In applied science and engineering, the laboratory overcomes critical technological challenges in energy and national security. The laboratory’s user facilities propel breakthroughs in fields ranging from supercomputing and AI applications for science, to materials characterization and nuclear physics, and climate science. The laboratory also leads nationwide collaborations spanning the research spectrum from discovery to application, including the Q-NEXT quantum information science center, Joint Center for Energy Storage Research, and ReCell advanced ba!ery recycling center. To take laboratory discoveries to market, Argonne collaborates actively with regional universities and companies and expands the impact of its research through innovative partnerships. FUNDING BY SOURCE HUMAN CAPITAL 3,448 FTE employees FY 2019 Costs (in $M) HEP $20 379 joint faculty Total Laboratory Operating NE $38 317 postdoctoral researchers Costs: $837* NP $30 297 undergraduate students DOE/NNSA Costs: $727 ASCR $97 224 graduate students SPP (Non-DOE/Non-DHS) 8,035 facility users Costs: $87 BES $274 FACTS NNSA 809 visiting scientists SPP as % of Total Laboratory $57 Operating Costs: 13% DHS $24 CORE CAPABILITIES DHS Costs: $24 BER $31 Accelerator S&T SPP $87 *Excludes expenditures of Advanced Computer Science, Visualization, and Data Other SC monies received from other Other DOE $23 Applied Materials Science and Engineering $65 DOE contractors and through EERE $91 Applied Mathematics joint appointments of research Biological and Bioprocess Engineering sta!. -
Advanced Photon Source: Lighting the Way to a Better Tomorrow
www.anl.gov www.aps.anl.gov ADVANCED PHOTON SOURCE — LIGHTING THE WAY TO A BETTER TOMORROW Frontier science serving the national interest and positively impacting nearly every aspect of our lives THE APS ENABLES RESEARCH IN NEARLY EVERY SCIENTIFIC DISCIPLINE ☐ Materials science ☐ Chemical science ☐ Environmental, geological, and planetary science ☐ Physics ☐ Polymer science ☐ Biological and life science ☐ Pharmaceutical research ☐ Nanoscale research The U.S. Department of Energy Office of Science’s (DOE-SC’s) Advanced The APS Upgrade will provide Photon Source (APS) gives scientists access to high-energy, high-brightness, researchers with a next-generation highly-penetrating x-ray beams that are ideal for studying the arrangements tool to probe structure and function of molecules and atoms, probing the interfaces where materials meet, across length, time, and energy determining the interdependent form and function of biological proteins, scales, extending the U.S. global and watching chemical processes that happen on the nanoscale. leadership in hard x-ray science for This remarkable scientific tool helps of these institutions and companies decades to come. researchers illuminate answers to invest millions of dollars to equip NOBEL PRIZE-WINNING the challenges of our world, from APS x-ray beamlines. The APS facility RESEARCH developing new forms of energy to houses x-ray-producing technologies The recipients of the 2009 Nobel sustaining our nation’s technological that comprise one of the most Prize in Chemistry published papers and economic competitiveness to complex machines in the world, on their award-worthy work based on pushing back against the ravages of the result of innovative research data collected at DOE x-ray disease. -
Chapter 1: Executive Summary
Advanced Photon Source Upgrade Project Preliminary Design Report September 2017 Chapter 1: Executive Summary Document Number : APSU-2.01-RPT-002 ICMS Content ID : APSU_1705610 Advanced Photon Source Upgrade Project 1ii Table of Contents Table of Contents 1 Executive Summary1 1-1 Introduction . .1 1-2 Project Capabilities . .2 1-3 Project Scope . .2 1-4 Cost and Schedule . .3 1-5 Alternatives Analysis . .4 1-6 Acquisition Strategy . .5 References 6 Advanced Photon Source Upgrade Project List of Tables 1iii List of Tables Table 1.1: APS Upgrade Performance Parameters . .3 Table 1.2: APS Upgrade proposed Critical Decision milestones . .4 Advanced Photon Source Upgrade Project 1iv Acronyms Acronyms and Abbreviations APS Advanced Photon Source APS-U Advanced Photon Source Upgrade Argonne Argonne National Laboratory BESAC Basic Energy Sciences Advisory Committee CD-n DOE Critical Decision (n = 0, 1, 2, 3, 4) DOE U.S. Department of Energy ID Insertion Device MBA Multi-Bend Achromat PDR Preliminary Design Report PME Project Management Executive SC Oce of Science TPC Total Project Cost UChicago UChicago Argonne LLC Advanced Photon Source Upgrade Project Executive Summary Page 11 1 Executive Summary 1-1 Introduction The tremendous scientic impacts of U.S. world leadership in accelerator-based x-ray light source user facilities over the last 40 years were underscored in the July 2013 Report of the Basic Energy Sciences Advisory Committee (BESAC) Subcommittee on Future X-ray Light Sources [1]. The report noted that recent technological advances are driving widespread international interest in developing the next generation of synchrotron light sources, which will enable transformational advances across a wide range of scientic disciplines. -
Advanced Photon Source Upgrade Project Final Design Report May
Advanced Photon Source Upgrade Project Final Design Report May 2019 Chapter 1: Executive Summary and Project Overview Document Number : APSU-2.01-RPT-003 ICMS Content ID : APSU_2032071 Advanced Photon Source Upgrade Project 1–ii • Table of Contents Table of Contents 1 Executive Summary and Project Overview1 1-1 Introduction . .1 1-2 Project Capabilities . .2 1-3 Project Scope . .2 1-4 Work Breakdown Structure . .3 1-5 Cost and Schedule . .5 1-6 Risk Assessment and Management . .8 References 10 Advanced Photon Source Upgrade Project List of Figures • 1–iii List of Figures Figure 1.1: Organization of the WBS . .5 Advanced Photon Source Upgrade Project 1–iv • List of Tables List of Tables Table 1.1: APS Upgrade Performance Parameters . .3 Table 1.2: APS-U Key Performance Parameter . .4 Table 1.3: Cost Summary for the APS Upgrade at CD-2. .6 Table 1.4: Funding Profile . .6 Table 1.5: APS Upgrade Critical Decision milestones . .6 Table 1.6: APS Upgrade Production Level 2 Milestones . .7 Advanced Photon Source Upgrade Project Acronyms • 1–v Acronyms and Abbreviations APS Advanced Photon Source APS-U Advanced Photon Source Upgrade Argonne Argonne National Laboratory BESAC Basic Energy Sciences Advisory Committee BOE Basis of Estimate CD-n DOE Critical Decision (n = 0, 1, 2, 3, 4) DOE U.S. Department of Energy ID Insertion Device MBA Multi-Bend Achromat PME Project Management Executive SC Office of Science TPC Total Project Cost WBS Work Breakdown Structure Advanced Photon Source Upgrade Project Executive Summary and Project Overview • Page 1–1 1 Executive Summary and Project Overview 1-1 Introduction The Advanced Photon Source (APS) at Argonne National Laboratory is a world leading synchrotron source of high energy x-rays, one of five light sources operated under the stewardship of the Depart- ment of Energy Office of Science / Office of Basic Energy Science. -
Free Electron Lasers Lecture 2.: Insertion Devices
„Preparation of the concerned sectors for educational and R&D activities related to the Hungarian ELI project ” Free electron lasers Lecture 2.: Insertion devices Zoltán Tibai János Hebling TÁMOP-4.1.1.C-12/1/KONV-2012-0005 projekt 1 Outline Introduction and history of insertion devices Dipole magnet Quadropole magnet Chicane Undulators . Pure Permanent magnet . Hybrid design . Helical undulator . Electromagnet Planar undulator . Electromagnet Helical undulator Examples TÁMOP-4.1.1.C -12/1/KONV-2012-0005 projekt 2 Introduction Whenever an electron beam changes direction it emits radiation in a continuous frequency band. The most conspicuous example is the intense radiation produced by electron in a synchrotron orbit. It is sometimes concentrated in a certain frequency range by ‘wiggling‘ the beam as it leaves the machine with the help of a few magnets so as to follow a shape like the outline of a camel’s back. Such a device is called wiggler. Many wiggler in succession, say 50 or more, serve to concentrate the radiation spatially into a narrow cone, and spectrally into a narrow frequency interval. The beam is made wavy and waves are produced, and for this reason a multi-period wiggler is called an undulator. TÁMOP-4.1.1.C-12/1/KONV-2012-0005 projekt 3 History of insertion devices 1947 Vitaly Ginzburg showed theoretically that undulators could be built. 1951/1953 The first undulator was built by Hans Motz. 1976 Free electron laser radiation from a superconducting helical undulator. 1979/1980 First operation of insertion devices in storage rings. 1980 First operation of wavelength shifters in storage rings Today few tens of 3rd generation synchrotron radiation light sources (SASE FEL) TÁMOP-4.1.1.C-12/1/KONV-2012-0005 projekt 4 Dipole magnet A dipole magnet provides us a constant field, B. -
Advanced Photon Source
ADVANCED PHOTON SOURCE I VOLUME 1 • NUMBER 1 • APRIL 1998 • ANL/APS/TB-31 ARGONNE NATIONAL LABORATORY IS OPERATED BY THE UNIVERSITY OF CHICAGO FOR THE U.S. DEPARTMENT OF ENERGY UNDER CONTRACT W-31-109-ENG-38 MASTER or THIS DOCUMWT IS IN THIS ISSUE LETTER FROM THE DIRECTOR DAVID E. MONCTON PG. 1 THE ADVANCED PHOTON SOURCE: A BRIEF OVERVIEW PG. 2 MAD ANALYSIS OF FHIT AT THE STRUCTURAL BIOLOGY CENTER PG. 6 CHRISTOPHER D. LIMA, KEVIN L. D'AMICO, ISTVAN NADAY, GEROLD ROSENBAUM, EDWIN M. WESTBROOK, & WAYNE A. HENDRICKSON ADVANCES IN HIGH-ENERGY-RESOLUTION X-RAY SCATTERING AT BEAMLINE 3-ID PG. 9 ESEN ERCAN ALP, WOLFGANG STURHAHN, THOMAS TOELLNER, PETER LEE, MARKUS SCHWOERER-BOHNING, MICHAEL HU, PHILIP HESSION, JOHN SUTTER, & PETER ABBAMONTE X-RAY IMAGING & MICROSPECTROSCOPY OF THE MYCORRHIZAL PG. 15 FUNGUS-PLANT SYMBIOSIS ZHONGHOU CM, WENBING YUN, STEPHEN T. PRATT, RAYMOND M. MILLER, EFIM GLUSKIN, DOUGLAS B. HUNTER, AMIEL G. JARSTFER, KENNETH M. KEMNER, BARRY LAI, HEUNG-RAE LEE, DANIEL G. LEGNINI, WILLIAM RODRIGUES, & CHRISTOPHER I. SMITH MEASUREMENT & CONTROL OF PARTICLE-BEAM TRAJECTORIES IN THE PG. 21 ADVANCED PHOTON SOURCE STORAGE RING GLENN DECKER BEAM ACCELERATION & STORAGE AT THE ADVANCED PHOTON SOURCE OPERATIONS REPORT ROD GERIG PG. 26 EXPERIMENTAL FACILITIES OPERATIONS & CURRENT STATUS ANTANAS RAUCHAS PG. 28 RECENT PUBLICATIONS PG. 30 ON THE FRONT COVER: The colored segments superimposed on an aerial photograph of the Advanced Photon Source facility indicate experiment hall sectors currently occupied by Collaborative Access Teams. See the back cover of this issue for a description of each team's proposed research initiatives.