NSF Light Source Report
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FEL Physics Summary
VUV and X-Ray Free Electron Lasers: The Technology and Its Scientific Promise William Barletta and Carlo Rizzuto Sections I & III – Motivations & FEL Physics List of symbols fine structure constant dimensionless vector potential aw horizontal Twiss x bunching parameter b mean resolution error of BPMs BPMres position error of BPMs BPMpos remanent field BR undulator magnetic field strength Bw horizontal Twiss x speed of light c mean phase error in undulator penetration depth δp horizontal dispersion Dx derivative of Dx D´x FEL beam diameter on optic Dw energy chirp from CSR E/E beam emittance electron charge e beam energy E peak electric field in gun Eo normalized emittance n energy in the FEL pulse EPulse longitudinal space charge force Fsc angle of incidence j i 1 2 relativistic factor (E/ me c ) optical function in transport H magnetic coercivity HC Alfven current at =1 IAo beam current Ib BBU threshold current IBBU undulator parameter K mean undulator strength Krms undulator spatial frequency kw gain length LG th m harmonic wavelength m plasma wavelength P radiation wavelength r undulator wavelength w root of gain equation harmonic number m electron mass me number of electrons Ne electron density ne number of undulator periods Nu radiation power P input laser power Plaser noise power Pn pole roll angle error BNP (or Pierce) parameter quantum FEL parameter ´ atom density A quality factor Q dipole quality factor Qdipole FEL energy constraint ratio r1 FEL emittance constraint ratio r2 FEL diffraction constraint ratio r3 classical radius of electron re bend angle in undulator bend angle in achromat 2 th phase of i electron i kick relative to each pole error j mean energy spread of electrons e bunch length z relativistic plasma frequency p distance along undulator z mean longitudinal velocity <vz> impedance of free space Zo Rayleigh range ZR 3 I. -
Bilateral NIST-PTB Comparison of Spectral Responsivity in the VUV
Bilateral NIST-PTB Comparison of Spectral Responsivity in the VUV A Gottwald 1, M Richter 1, P-S Shaw 2, Z Li 2 and U Arp 2 1Physikalisch-Technische Bundesanstalt, Abbestraße 2-12, 10587 Berlin, Germany 2National Institute for Standards and Technology, 100 Bureau Dr., Gaithersburg, MD 20899-8410, U.S.A. E-mail: [email protected] Abstract. To compare the calibration capabilities for the spectral responsivity in the vacuum-ultraviolet spectral region between 135 nm and 250 nm, PTB and NIST agreed on a bilateral comparison. Calibrations of semiconductor photodiodes as transfer detectors were performed using monochromatized synchrotron radiation and cryogenic electrical substitution radiometers as primary detector standards. Great importance was attached to the selection of suitable transfer detector standards due to their critical issues in that wavelength regime. The uncertainty budgets were evaluated in detail. The comparison showed a reasonable agreement between the participants. However, it got obvious that the uncertainty level for this comparison cannot easily be further reduced due to the lack of sufficiently radiation-hard and long-term stable transfer standard detectors. Keywords: PACS: 07.60.Dq, 07.85.Qe, 85.60.Dw, 06.20.fb Bilateral NIST-PTB Comparison of Spectral Responsivity in the VUV 2 1. Introduction The last decade has seen numerous key comparisons in the field of photometry and radiometry between different national metrology institutes (NMIs) in the context of the Mutual Recognition Arrangement. At first, these comparisons were restricted to wavelengths longer than 200 nm, with just the exception of a recent pilot comparison from 10 nm to 20 nm [1]. -
Collimation System for the Bessy Fel∗
T. Kamps / Proceedings of the 2004 FEL Conference, 381-384 381 COLLIMATION SYSTEM FOR THE BESSY FEL∗ T. Kamps Berliner Elektronenspeicherring-Gesellschaft fur¨ Synchrotronstrahlung BESSY, D-12489 Berlin, Germany Abstract magnet undulators. Each undulator is composed of mod- ules with length ranging from 1.6 m to 3.9 m, the total Beam collimation is an essential element for the success- length of the high energy FEL line is 70 m. A FODO lat- ful running of a linear accelerator based free electron laser. tice is superimposed onto the undulator structure with the The task of the collimation system is to protect the undu- quadrupole magnets located at the intersections between lator modules against mis-steered beam and dark-current. the undulator modules. For the present analysis in total 14 This is achieved by a set of apertures limiting the succeed- undulator modules are taken into account for the simulation ing transverse phase space volume and magnetic dogleg studies. The gap between the undulator poles is 10 mm, the structure for the longitudinal phase space. In the follow- beampipe radius is 4 mm. The undulator magnets are made ing the design of the BESSY FEL collimation system is of NdFeB in order to obtain large undulator K parameters. described together with detailed simulation studies. This material is very sensitive to irradiation, especially to the reduced dose deposited by high-energy electrons (> MOTIVATION 20 MeV). From studies with NdFeB under electron irra- Experiences from linac driven FEL operation (for exam- diation [4] the limit for acceptable beam loss in the undula- ple at TTF1 [1]) indicate that beam collimation is essential tor chamber has been derived. -
Synchrotron Light Source
Synchrotron Light Source The evolution of light sources echoes the progress of civilization in technology, and carries with it mankind's hopes to make life's dreams come true. The synchrotron light source is one of the most influential light sources in scientific research in our times. Bright light generated by ultra-rapidly orbiting electrons leads human beings to explore the microscopic world. Located in Hsinchu Science Park, the NSRRC operates a high-performance synchrotron, providing X-rays of great brightness that is unattainable in conventional laboratories and that draws NSRRC users from academic and technological communities worldwide. Each year, scientists and students have been paying over ten thousand visits to the NSRRC to perform experiments day and night in various scientific fields, using cutting-edge technologies and apparatus. These endeavors aim to explore the vast universe, scrutinize the complicated structures of life, discover novel nanomaterials, create a sustainable environment of green energy, unveil living things in the distant past, and deliver better and richer material and spiritual lives to mankind. Synchrotron Light Source Light, also known as electromagnetic waves, has always been an important means for humans to observe and study the natural world. The electromagnetic spectrum includes not only visible light, which can be seen with a naked human eye, but also radiowaves, microwaves, infrared light, ultraviolet light, X-rays, and gamma rays, classified according to their wave lengths. Light of Trajectory of the electron beam varied kind, based on its varied energetic characteristics, plays varied roles in the daily lives of human beings. The synchrotron light source, accidentally discovered at the synchrotron accelerator of General Electric Company in the U.S. -
The Diamond Light Source
The Diamond Light Source ... a bright future for UK and World science Richard P. Walker, Technical Director What is Diamond ? • The largest scientific investment in the UK for 30 years • A synchrotron light source producing pinpoint UV and X-ray light beams of exceptional brightness • A ‘super microscope’ for new research opportunities into the structure and properties of matter What is Diamond ? • A Power Converter ! 15 MW of electrical power from the grid … 300-500 kW of X-rays … … but most of which only produces unwanted heat; only a fraction is selected for use in experiments. What is Synchrotron Radiation ? SR is electromagnetic radiation emitted when a high energy beam of charged particles (electrons) is deflected by a magnetic field. What’s so special about Synchrotron Radiation ? SR SR is emitted over a wide range of the electromagnetic spectrum, from Infra-red to hard X-rays Any desired radiation wavelength can be produced - enabling a very wide range of scientific and technological applications What’s so special about Synchrotron Radiation ? SR is very intense, and has extremely high brightness (emitted from a small area, with small angular divergence, determined by the properties of the electron beam) High brightness means: - it can be focused to sub-micron spot sizes: possibility of examining extremely small samples or investigating the structure and properties of objects with very fine spatial resolution - experiments can be carried out much more quickly: high through-put of samples or ability to follow chemical and biological reactions in real-time Diamond is a “third-generation” synchrotron radiation source • 1st generation: machines originally built for other purposes e.g. -
National Laboratories Subcommittee (Pdf)
The Regents of the University of California NATIONAL LABORATORIES SUBCOMMITTEE January 24, 2018 The National Laboratories Subcommittee met on the above date at Mission Bay Conference Center, San Francisco. Members present: Regents De Le Peña, Mancia, Napolitano, Ortiz Oakley, Pérez, and Tauscher; Chancellor Block In attendance: Secretary and Chief of Staff Shaw, Vice Presidents Budil and Ellis, Deputy General Counsel Woodall, and Recording Secretary McCarthy The meeting convened at 3:15 p.m. with Subcommittee Vice Chair De La Peña presiding. He acknowledged the dedicated service of Committee Chair Pattiz, who for ten years was chair of the Boards of Directors of the Los Alamos National Security LLC and the Lawrence Livermore National Security LLC. He had served in these roles with passion and distinction, affirming the importance of UC’s work with the National Laboratories. 1. APPROVAL OF MINUTES OF PREVIOUS MEETING Upon motion duly made and seconded, the minutes of the meeting of November 15, 2017 were approved. 2. PRESENTATION ON THE STATE OF THE LAWRENCE BERKELEY NATIONAL LABORATORY [Background material was provided to Regents in advance of the meeting, and a copy is on file in the Office of the Secretary and Chief of Staff.] Vice President Budil expressed appreciation for Committee Chair Pattiz’ leadership and tireless advocacy over the past decade for the National Laboratories and the University’s role in the Los Alamos National Security LLC and the Lawrence Livermore National Security LLC. Ms. Budil introduced Lawrence Berkeley National Laboratory (LBNL) Director Michael Witherell, who said he had been privileged to lead LBNL for two years. -
The Tesla Free Electron Laser J
THE TESLA FREE ELECTRON LASER J. Rossbach, for the TESLA FEL collaboration DESY, Notkestrasse 85, D22603 Hamburg, Germany Abstract occupied many scientists, a practical solution to this prob- lem has not yet been realized. To be an efficient research The TESLA Free Electron Laser (FEL) makes use of the tool, such a source would have to provide stable intensities high electron beam quality that can be provided by the su- with short pulses and repetition frequencies similar to what perconducting TESLA linac to drive a single pass FEL at is found in optical lasers. Exactly this seems to be possible wavelengths far below the visible. To reach a wavelength by using the so-called self amplified spontaneous emission of 6 nanometers, the TESLA Test Facility (TTF) currently process SASE. under construction at DESY will be extended to 1 GeV The basic principle [1] makes use of the fact that an elec- beam energy. Because there are no mirrors and seed-lasers tron beam of sufficient quality, passing a long undulator in this wavelength regime, the principle of Self-Amplified- magnet, exponentially amplifies an initially existing radi- Spontaneous-Emission (SASE) will be employed. A first ation field, if the photon wavelength λph matches a reso- test of both the principle and technical components is fore- nance condition determined by undulator parameters and seen at a photon wavelength larger than 42 nanometers. the beam energy: With respect to linac technology, the key prerequisite for such single-pass, high-gain FELs is a high intensity, λu 2 λph = (1 + K ) (1) diffraction limited, electron beam to be generated and ac- 2γ2 celerated without degradation. -
X-Ray Photoelectron Spectroscopy of Hydrogen and Helium 12 February 2019
X-ray photoelectron spectroscopy of hydrogen and helium 12 February 2019 This work demonstrated that ambient pressure X- ray photoelectron spectra of hydrogen and helium can be obtained when a bright-enough X-ray source is used, such as at the National Synchrotron Light Source II. In the case of helium gas, the spectrum shows a symmetric peak from its only orbital. In the case of hydrogen gas molecules, an asymmetric peak is observed, which is related to the different possible vibrational modes of the final state. The hydrogen X-ray beam induces photo-ejection of an electron from 2 (left) hydrogen and (right) helium . Credit: US molecule vibrational structure is evident in the H 1s Department of Energy spectrum. More information: Jian-Qiang Zhong et al. Synchrotron-based ambient pressure X-ray For the first time scientists measured the photoelectron spectroscopy of hydrogen and vibrational structure of hydrogen and helium atoms helium, Applied Physics Letters (2018). DOI: by X-rays. The results disprove the misconception 10.1063/1.5022479 that it's impossible to obtain X-ray photoelectron spectroscopy (XPS) spectra of hydrogen and helium, the two lightest elements of the Periodic Table. This was thought to be the case due to low Provided by US Department of Energy probabilities of electron ejection from these elements induced by X-rays. Unparalleled beam brightness at the National Synchrotron Light Source-II significantly increases the probability of a photon colliding with a gas atom at ambient pressures. The beamline makes it possible to use XPS to directly study the two most abundant elements in the universe. -
Biomaterials
BIOMATERIALS Research in the Department of Biomaterials The Department of Biomaterials focuses on interdisci- New Methods for Analysis of Biomaterials plinary research in the field of biological and bio- Studying hierarchical biomaterials requires state-of-the-art mimetic materials. The emphasis is on under- experimental equipment, but there is also some need for the standing how the mechanical or other physical development of new approaches. Scanning methods based properties are governed by structure and compo- on the diffraction of synchrotron radiation, as well as the sition (see Fig. 1). Furthermore, research on nat- technique of small-angle x-ray scattering (SAXS) are continu- ural materials (such as bone or wood) has poten- ously developed to improve the characterization of hierarchi- tial applications in many fields. First, design con- cal biomaterials. Further technical improvement is expected cepts for new materials may be improved by from a dedicated scanning set-up which is currently being learning from Nature. Second, the understanding installed at the synchrotron BESSY in Berlin. of basic mechanisms by which the structure of bone or connective tissue is optimised opens the way for Plant Biomechanics Biotemplating studying diseases and, thus, for contributing to diagnosis (Ingo Burgert) (Oskar Paris) and development of treatment strategies. A third option is to use structures grown by Nature and transform them by phys- Mechanobiology Biomimetic Materials ical or chemical treatment into technically relevant materials (Richard Weinkamer) (Peter Fratzl) (biotemplating). Given the complexity of natural materials, new approaches for structural characterisation are needed. Mineralized Tissues Bone Research Some of these are further developed in the Department, in (Himadri S. -
10 Bessy Ventilation Concept
XFEL Tunnel Ventilation and Air Conditioning BESSY ventilation concept www.helmholtz-berlin.de BESSY I - History • 1979 BESSY GmbH was founded • 1982 BESSY operated until 1999 the electron storage ring facility BESSY I in Berlin-Wilmersdorf • 1999 BESSY I was cut back and 30 Beamlines were reconstructed at BESSY II www.helmholtz-berlin.de BESSY II - History • March 1993 the project team BESSY II starts work in Adlershof • 4. July 1994 Groundbreaking ceremony on the construction site for BESSY II • 13. Dec. 1995 Topping-out ceremony for the new building • 07. April 1997 Commencement of operation of the synchrotron www.helmholtz-berlin.de BESSY II - Commisioning • 23. June 1997 First acceleration of an electron beam in the synchrotron up to 1.9 GeV • 22. April 1998 First storage of an elctron beam in the storage ring and detection of synchrotron radiation • 16. July 1998 First production of „undulator“ –light • 4. Sept. 1998 Inauguration ceremony for the high brilliance synchrotron radiation source BESSY II www.helmholtz-berlin.de BESSY II - Operation • Oct. 1998 First scientific experiment • Jan. 1999 Official start of user-dedicated operation • Jan. 2000 Admission to the Leibnitz- Association • Dec. 2001 Inauguration of the BESSY extension office www.helmholtz-berlin.de BESSY II – Helmholtz-Zentrum Berlin • Jan. 2009 the Helmholtz-Zentrum Berlin (HZB) was foundet by merging the former Hahn- Meitner Institut (HMI) and BESSY • the Helmholtz-Zentrum Berlin now operates two scientific large scale facilities for investigating the structure -
National Synchrotron Light Source II
National Synchrotron Light Source II J.P. Hill, NSLS-II Director National Lab Day October 10th 2019 User Facilities at the National Labs • One of the primary missions of the National Labs is to provide large scale user facilities that are beyond the reach of individual institutions • Principal among these are the 5 light sources, the 2 neutron sources and the 5 nanocenters. DOE-BES stewards these facilities for the Nation • Each provides world-leading characterization facilities that are free to use through a transparent, peer-reviewed proposal process • Our scientists are leaders in their fields and are there to help you answer your science questions • In structural biology, synchrotrons in particular have revolutionized the field and continue to push state-of-the-art with diffraction and imaging capabilities of extraordinary sensitivity and resolution 2 NSLS-II: The Nation’s brightest synchrotron 28 “beamlines” for experiments from scattering, to imaging to spectroscopy • State-of-the-art beamlines in structural biology and imaging: Protein crystallography Solution scattering Spectroscopic imaging • Growing emphasis on “multi-modal” i.e. combining more than one technique to obtain a more complete picture of a given biological problem 3 4 Biological “Imaging” at NSLS-II atomic resolution structures Complexes cellular context and function MX MX, S/WAXS Imaging cryoEM 4 Multi-modal, multi-length scale 5 Ultra bright beams enable new methods: Serial crystallography Jets of micro-crystals Raster data collection 1 µm step raster scans. Total shutter open time for dataset = 18 s These new approaches greatly ease the need to grow large crystals – perhaps the biggest bottleneck in structure determination. -
A Brilliant Light for Science
A BRILLIANT LIGHT FOR SCIENCE Located in Grenoble, THE MOST INTENSE A benchmark for science and innovation France, the European SYNCHROTRON Synchrotron Supported by 21 partner countries, the ESRF Radiation Facility LIGHT SOURCE IN THE is the most intense source of synchrotron (ESRF) is a WORLD light. Inaugurated in 1994, the ESRF shining light on is an international centre of excellence for fundamental research with a strong the international A unique research facility commitment to applied and industrial research scene. Imagine a source that produces X-rays 100 research. Every year, the ultra- billion times brighter than the X-rays used With its 43 highly specialised experimental intense X-ray beams in hospitals, X-rays that allow us to fathom stations, known as “beamlines”, produced at the ESRF the structure of matter down to the minutest each equipped with state-of-the-art attract thousands of detail, at the atomic level. Imagine no further! instrumentation, the ESRF offers scientists X-rays with these outstanding properties research scientists an extremely powerful research tool that is really do exist. They can be found at the ESRF, constantly being upgraded. from both academic where they are produced by the high-energy institutions and electrons that race around the institute’s Its strength also lies in bringing together in industry. emblematic “storage ring”, an accelerator of one facility multidisciplinary teams involving impressive proportions. some of the world’s best scientists, engineers and technicians. Working like a giant microscope, the ESRF offers unparalleled opportunities to explore Every year, thousands of scientists come to materials and living matter.