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NSLS-II | |
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General information | |
Type | Research and Development Facility |
Town or city | Upton, New York |
Country | United States |
Coordinates | 40°51′55.38″N72°52′19.71″W / 40.8653833°N 72.8721417°W |
Construction started | 2009 |
Completed | 2015 [1] |
Cost | US$912 million |
Owner | United States Department of Energy |
Technical details | |
Floor area | 400,000 sq ft (37,000 m2) [2] |
Design and construction | |
Architecture firm | HDR, Inc. |
Main contractor | Torcon, Inc. [3] |
Website | |
BNL: National Synchrotron Light Source II (NSLS-II) |
The National Synchrotron Light Source II (NSLS-II) at Brookhaven National Laboratory (BNL) in Upton, New York is a national user research facility funded primarily by the U.S. Department of Energy's (DOE) Office of Science. NSLS-II is one of the world's most advanced synchrotron light sources, designed to produce x-rays 10,000 times brighter than BNL's original light source, the National Synchrotron Light Source (NSLS). NSLS-II supports basic and applied research in energy security, advanced materials synthesis and manufacturing, environment, and human health.
NSLS-II fuels major advances in new energy technologies such as nanocatalyst-based fuel cells, economical use of solar energy, high-temperature superconductors in a high capacity and high reliability electric grid, and advanced electrical storage systems for transportation and harnessing intermittent renewable energy sources. [4]
In the first five months of 2023, NSLS-II served over 1,200 researchers ("users") from academic, industrial, and government laboratories worldwide [5] . Any qualified researcher can submit a peer-reviewed proposal to use NSLS-II [6] .
NSLS-II partners with public and private institutions have joined effort to fund the construction and operation of some of its beamlines. Its partnerships include BNL's Center for Functional Nanomaterials and the National Institute of Standards and Technology, among many others. NSLS-II is always open for new partnerships.
NSLS-II currently has 29 beamlines (experimental stations) open for user operations. [7] When the facility is complete, NSLS-II will have at least 58 beamlines in operation.
The beamlines at NSLS-II are grouped into five science programs: hard x-ray scattering & spectroscopy, imaging & microscopy, structural biology, soft x-ray scattering & spectroscopy, and complex scattering. These programs group beamlines together that offer similar types of research techniques for studying the behavior and structure of matter.
NSLS-II is a medium energy (3.0 GeV) electron storage ring designed to deliver photons with high average spectral brightness exceeding 1021 ph/s in the 2 – 10 keV energy range and a flux density exceeding 1015 ph/s in all spectral ranges. This performance requires the storage ring to support a very high-current electron beam (up to 500 mA) with a very small horizontal (down to 0.5 nm-rad) and vertical (8 pm-rad) emittance. The electron beam is stable in its position (<10% of its size), angle (<10% of its divergence), dimensions (<10%), and intensity (±0.5% variation).
The NSLS-II storage ring lattice consists of 30 double-bend achromat (DBA) cells that can accommodate at least 58 beamlines for user experiments, distributed by type of source as follows:
Continuing the tradition established by the NSLS, NSLS-II radiation sources span a very wide spectral range, from the far infrared (down to 0.1 eV) to the very hard x-ray region (>300 keV). This is achieved by a combination of bending magnets, three-pole wigglers, and insertion device (ID) sources. [8]
Construction of NSLS-II began in 2009 and was completed on-time and under budget in 2014. NSLS-II saw first light in October 2014. The facility cost US$912 million to build, and the project received the DOE's Secretary's Award of Excellence. Torcon Inc., headquartered in New Jersey, was the general contractor selected by the DOE for the project. [9]
A synchrotron light source is a source of electromagnetic radiation (EM) usually produced by a storage ring, for scientific and technical purposes. First observed in synchrotrons, synchrotron light is now produced by storage rings and other specialized particle accelerators, typically accelerating electrons. Once the high-energy electron beam has been generated, it is directed into auxiliary components such as bending magnets and insertion devices in storage rings and free electron lasers. These supply the strong magnetic fields perpendicular to the beam that are needed to stimulate the high energy electrons to emit photons.
Photoemission spectroscopy (PES), also known as photoelectron spectroscopy, refers to energy measurement of electrons emitted from solids, gases or liquids by the photoelectric effect, in order to determine the binding energies of electrons in the substance. The term refers to various techniques, depending on whether the ionization energy is provided by X-ray, XUV or UV photons. Regardless of the incident photon beam, however, all photoelectron spectroscopy revolves around the general theme of surface analysis by measuring the ejected electrons.
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The National Synchrotron Light Source (NSLS) at Brookhaven National Laboratory (BNL) in Upton, New York was a national user research facility funded by the U.S. Department of Energy (DOE). Built from 1978 through 1984, and officially shut down on September 30, 2014, the NSLS was considered a second-generation synchrotron.
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Laser-based angle-resolved photoemission spectroscopy is a form of angle-resolved photoemission spectroscopy that uses a laser as the light source. Photoemission spectroscopy is a powerful and sensitive experimental technique to study surface physics. It is based on the photoelectric effect originally observed by Heinrich Hertz in 1887 and later explained by Albert Einstein in 1905 that when a material is shone by light, the electrons can absorb photons and escape from the material with the kinetic energy: , where is the incident photon energy, the work function of the material. Since the kinetic energy of ejected electrons are highly associated with the internal electronic structure, by analyzing the photoelectron spectroscopy one can realize the fundamental physical and chemical properties of the material, such as the type and arrangement of local bonding, electronic structure and chemical composition.
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