Beamline Name: BL4-3 Primary Contact: Name: Matthew Latimer: Secondary Contact: Name: Erik Nelson: Owner/Operator: SSRL-SMB-XAS: Status: Operational: Status Details: Open %Time Available (general use) 100: Experiments: XAFS, EXAFS: Experiments Details: Beam line 4-3 is a wiggler side-station beam line for X-ray absorption spectroscopy and EXAFS

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SSRL Beamline 5-4 UV or x-ray photons are directed onto a sample where they interact with the electrons within the sample, ejecting them into the vacuum. By analyzing these emitted electrons, we can learn about the properties of electrons within the sample.

Beam line 4-3 is a wiggler side-station dedicated for x-ray absorption spectroscopy and EXAFS measurements on biological, environmental, catalysis, and materials systems. This station enables tender x-ray measurement (S K-edge and up, i.e. 2.4-5 keV) in addition to hard x-rays ( up to 11 keV). The 20-pole wiggler of Beam Line 4-3 produces high-resolution x-ray spectra in the 2.4-14 keV energy range that makes Beam Line 4-3 especially useful to study the elements sulfur, chlorine, and calcium, which are important to biology, geology and archaeology. Science is the search for the unexpected, and Beam Line 4-3 is a great facilitator.

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Our group helps the maintenance of three beamlines, SSRL beamline 5-4, SSRL beamline 5-2 and ALS beamline 10.0.1, respectively. Following are some of their descriptions. Dimosthenis Sokaras at SSRL Beamline 6-2. (Photo by Brad Plummer.) A new spectroscopy instrument has been installed on Beamline 6-2 at the Stanford Synchrotron Radiation Lightsource, where staff scientists are now working to test its various components before offering beam time to users this spring. A beamline has been constructed at Stanford Synchrotron Radiation Laboratory (SSRL) whose radiation source is a multipole permanent magnet wiggler installed in a straight section of the SPEAR 3-3.5 GeV electron storage ring. The wiggler is a hybrid design that utilizes Nd-Fe alloy magnet material combined with Vanadium Permendur poles.

SSRL Beamline 14 Sees First Light . The first X-ray light from Beamline 14 (white spot) hits a florescence screen in this webcam image. (Image courtesy of Daniel Harrington.) Last week, X-ray light for the first time streamed into the new Beamline 14-1 hutch at the Stanford Synchrotron Radiation Lightsource.

By analyzing these emitted electrons, we can learn about the properties of electrons within the sample. Connecting to SSRL computers using NoMachine (NX) As most experiments are conducted remotely, the way to access the beamline control software, blu-ice, is by establishing a remote desktop session to SSRL.

Beamline 4-3 ssrl

SSRL offers more than 30 experimental stations, supporting a variety of techniques including: macromolecular crystallography, soft and hard x-ray microscopy, microXAS imaging, x-ray scattering and diffraction, photoemission spectroscopy and x-ray absorption and emission spectroscopies.

BL 4 - Closed. BL 4-1. BL 4-2. BL 4-3. 17G-IG-BL04, 1.6e-10, Torr.

(Photo by Brad Plummer.) A new spectroscopy instrument has been installed on Beamline 6-2 at the Stanford Synchrotron Radiation Lightsource, where staff scientists are now working to test its various components before offering beam time to users this spring. A beamline has been constructed at Stanford Synchrotron Radiation Laboratory (SSRL) whose radiation source is a multipole permanent magnet wiggler installed in a straight section of the SPEAR 3-3.5 GeV electron storage ring. The wiggler is a hybrid design that utilizes Nd-Fe alloy magnet material combined with Vanadium Permendur poles. It is approximately 2 m long and has 15 full wiggler Beam line 4-1 is optimized for XAS measurements between ~5.5 and 30 keV, whereas BL 4-3 is optimized for experiments at 2.4 to 7 keV.
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SSRL Beamline Map 20 pole 2T Wiggler Beamline 4-3 Enter through the back door ! Stanford Synchrotron Radiation Lightsource The Experimental Setup Tender Energy(2-5 KeV) I0 I1 I2 Fluorescence detector slits to define the beam Sample double crystal monochromator He flight path High Energy (>5000 eV) I0 I1 I2 Fluorescence detector slits to define Beamline 4-3 was newly reopened as of 4/6/2009 bringing special capabilities for soft-energy (2.4-6 keV) studies in addition to hard x-rays. Beamline 4-3 now replaces 6-2 as the preferred location for Sulfur K-edge experiments at SSRL. Spectra of the reference compounds were collected at beamline 4-3 at SSRL according to the methods described above for S XAS measurements.

Filter Spectra by Edge, Beamline, Measurement Mode, Rating, or Text in Name, Comment, or other Field: Edge: SSRL has recently returned to extended running following the successful commissioning of a dedicated injector, and operation of the SPEAR storage ring exclusively for synchrotron radiation research. During the hiatus, the entire beamline data acquisition systems at the laboratory have been upgraded and extended to provide a more consistent, capable, and flexible interface to synchrotron users.
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The photon beam that directly comes out of the beamline is focused to a 150 x 300 micron spot size on the sample, which would improve the spectrum resolution. Beamline Facilities. Our group helps the maintenance of three beamlines, SSRL beamline 5-4, SSRL beamline 5-2 and ALS beamline 10.0.1, respectively. Following are some of their descriptions.

2010, 53, 3532–3551 DOI: 10.1021/jm901713n Identification of 4,5-Dihydro-1H-pyrazolo[4,3-h]quinazoline Derivatives as a New Class of Orally and Selective Polo-Like Kinase 1 Inhibitors Italo Beria,* Dario Ballinari, Jay Aaron Bertrand, Daniela Borghi, Roberto Tiberio Bossi, Maria Gabriella Brasca, Paolo Cappella, Michele Caruso, Walter Ceccarelli, Antonella Ciavolella

edge X-ray absorption spectra were collected on beamline 4−3 at the SSRL operating at 3.0 GeV and 100−200 mA. Methods are described in the SI. Spectral analysis was performed with the program SIXPAK.31 Background before the edge was subtracted using a linear fit to the pre-edge region and spectra were normalized to the postedge step height. Mercury L

Development of this capability is underway at Stanford Synchrotron Radiation Lightsource, SLAC National Accelerator Laboratory, to establish sub-5 nm resolution ptychographic imaging with spatially resolved near-edge The Stanford Synchrotron Radiation Lightsource (SSRL) provides synchrotron radiation, a name given to X-rays or light produced by electrons circulating in a storage ring at nearly the speed of light. These extremely bright X-rays can be used to investigate various forms of matter ranging from objects of atomic and molecular size to man-made materials with unusual properties. 2020-09-23 · Password change on SSRL Macromolecular Crystallography Group computers.

Beamline Name: BL4-3 Primary Contact: Name: Matthew Latimer: Secondary Contact: Name: Erik Nelson: Owner/Operator: SSRL-SMB-XAS: Status: Operational: Status Details: Open %Time Available (general use) 100: Experiments: XAFS, EXAFS: Experiments Details: Beam line 4-3 is a wiggler side-station beam line for X-ray absorption spectroscopy and EXAFS SSRL offers more than 30 experimental stations, supporting a variety of techniques including: macromolecular crystallography, soft and hard x-ray microscopy, microXAS imaging, x-ray scattering and diffraction, photoemission spectroscopy and x-ray absorption and emission spectroscopies. Beamline 4-3 was newly reopened as of 4/6/2009 bringing special capabilities for soft-energy (2.4-6 keV) studies in addition to hard x-rays. Beamline 4-3 now replaces 6-2 as the preferred location for Sulfur K-edge experiments at SSRL. 2018-02-20 · Beam line 7-3 is a wiggler side-station dedicated for x-ray absorption spectroscopy and EXAFS measurements on dilute biological systems. BL7-3 is equipped with a 30-element Ge solid-state detector in addition to ionization chambers and Lytle/PIPS detectors. SSRL Beamline 5-4 UV or x-ray photons are directed onto a sample where they interact with the electrons within the sample, ejecting them into the vacuum.