IFAE-ALBA | Alba, 13 th December, 2012BL29 - BOREAS 1 of 20 BOREASBORE AS BOREAS, Beamline Of REsonant Absorption and Scattering: status report Javier.

Slides:



Advertisements
Similar presentations
NSLS-II Soft X-ray Undulator Beamlines
Advertisements

X-Ray Astronomy Lab X-rays Why look for X-rays? –High temperatures –Atomic lines –Non-thermal processes X-ray detectors X-ray telescopes The Lab.
User requirements Session chair K.Evans-Lutterodt Speakers: Jorg Maser N. Simos D.Arena P.Northrup C. Sanchez-Hanke.
Synchrotron applications of pixel and strip detectors at Diamond Light Source Julien Marchal, Nicola Tartoni, Colin Nave Diamond Light Source 03/09/2008.
How to explore a system? Photons Electrons Atoms Electrons Photons Atoms.
John Arthur X-ray October 12, 2004 X-Ray Detector Program Status John Arthur.
Spectroscopy. Atoms and Light  Atomic electron energy levels are a source of discrete photon energies.  Change from a high to low energy state produces.
SSRL: A Vision for the Future Joachim Stöhr, SSRL Director SSRL 32 nd Annual Users' Meeting October 17, 2005 Present status Management vision and goals.
Abstract A new ultrahigh-resolution photoemission electron microscope called PEEM3 is being developed at the Advanced Light Source. An electron mirror.
Computed Tomography. Introduced in 70’s Principle: Internal structures of an object can be reconstructed from multiple projections of the object.
David Fritz XPP June 17, The X-ray Pump-Probe Instrument Instrument Scientist: David Fritz Second Scientist:
1 Sébastien Boutet 1 Coherent X-ray Imaging Instrument FAC Meeting, June Coherent X-ray Imaging Instrument Sébastien Boutet.
Photoelectron Spectroscopy Lecture 7 – instrumental details –Photon sources –Experimental resolution and sensitivity –Electron kinetic energy and resolution.
Epics Collaboration Meeting Pohang Oct 2012
USING A MICRO FABRICATED UNDULATOR TO BRIDGE THE FOUR DECADE GAP BETWEEN REGULAR PURE PERMANENT MAGNET UNDULATORS AND INVERSE COMPTON SCATTERING SOURCES.
What Are Some Types of Spectroscopy ?
Science Specification of SOLAR-C payload SOLAR-C Working Group 2012 July 23.
Effective lens aperture Deff
X-rays The electric field E(r,t) is given as a cosine function.
Introduction to Synchrotron Radiation Instrumentation
Main Bullet #1 Main Bullet #2 Main Bullet #3 Canadian Light Source National Synchrotron Light Facility.
A U.S. Department of Energy Office of Science Laboratory Operated by The University of Chicago Argonne National Laboratory Office of Science U.S. Department.
Status of the Beamline Simulation A.Somov Jefferson Lab Collaboration Meeting, May 11, 2010.
Laser-microwave double resonance method in superfluid helium for the measurement of nuclear moments Takeshi Furukawa Department of Physics, Graduate School.
HXMA BL Status CLS AUM 07 June 15, 2007 XAFS: operational; Microprobe: opening for letter of intent; Diffraction: under commissioning.
Understanding typical users for this instrument Graduate studentGraduate student –not an X-ray expert but wants to make a spatially resolved measurement;
Karine CHESNEL ALS WORKSHOP Magnetic Nanostructures, Interfaces, and New Materials: Theory, Experiment, and Applications.
SOFT X-RAY SCATTERING AT ESRF: A BRIEF OVERVIEW Peter Bencok European Synchrotron Radiation Facility Grenoble, France.
Detectors for Light Sources Contribution to the eXtreme Data Workshop of Nicola Tartoni Diamond Light Source.
Soft Coherent Scattering and Imaging Chris Jacobsen, Stony Brook Cecilia Sánchez-Hanke, NSLS.
EPICS-based motion control and data acquisition system on hard x-ray microfocus beamline station Yan Fen Hard X-ray Microfocus beamline, Shanghai Synchrotron.
IFAE-ALBA Meeting, December 13 th 2012BL24 - CIRCE 1 of 13 BL 24 – CIRCE Photoelectron spectroscopy and microscopy.
Stability Requirements for Superconducting Wiggler Beamlines
PC4250 Introduction to Surface Analysis Techniques.
Commissioning of the CMCF 08ID-1 Beamline. Light in the Optical Hutch September 2005 Light at the entrance to the white beam slits (42 m). The rectangular.
Latifa Elouadrhiri Jefferson Lab Hall B 12 GeV Upgrade Drift Chamber Review Jefferson Lab March 6- 8, 2007 CLAS12 Drift Chambers Simulation and Event Reconstruction.
1 BROOKHAVEN SCIENCE ASSOCIATES The use of fast-modulated elliptically polarized soft x-rays in the detection of small polarization signals Cecilia Sánchez-Hanke.
A users viewpoint: absorption spectroscopy at a synchrotron Frithjof Nolting.
Proposed NSLS X13B Microdiffraction Instrument Source & Optics James M. Ablett National Synchrotron Light Source.
X-ray absorption spectroscopy (XAS)
Detection Scheme of Single Shot Time Resolved X-ray Emission Spectroscopy of Chemical Dynamics at LCLS Kathleen R. Geyer August 12, 2010 Mentor: Dennis.
Alba, 13 December 2012Detectors at BL22 – CLÆSS 1 of 8 Detectors at BL 22 - CLÆSS.
Measurements of ultra-low emittances using a vertical undulator K.P. Wootton, G.N. Taylor, R.P. Rassool The University of Melbourne M.J. Boland, B.C.C.
Lecture 3-Building a Detector (cont’d) George K. Parks Space Sciences Laboratory UC Berkeley, Berkeley, CA.
Current status of the BaD-ElPh project at ELETTRA
1.1 What’s electromagnetic radiation
Electron Spectrometer: Status July 14 Simon Jolly, Lawrence Deacon 1 st July 2014.
MPI Semiconductor Laboratory, The XEUS Instrument Working Group, PNSensor The X-ray Evolving-Universe Spectroscopy (XEUS) mission is under study by the.
1 B. C. Stratton, S. von Goeler, and R. Feder PPPL J. Lowrance, V. Mastrocola, and G. Renda Princeton Scientific Instruments NSTX Physics Meeting June.
SAC 2014 BL29 BOREAS beamline BL29 BOREAS Resonant X-ray Absorption and Scattering.
CIRCE beamline at ALBA variable polarization soft x-rays for advanced photoelectron spectroscopy & microscopy.
G. Penn SLAC 25 September 2013 Comments on LCLS-IISC Design.
IDs at ALBA synchrotron ALBA-SSRF workshop – December /30 Josep Campmany – CELLS IDs at ALBA synchrotron: Some notes on strategy, design, Manufacturing,
Vertical Emittance Measurements using a Vertical Undulator K.P. Wootton, G.N. Taylor, R.P. Rassool Uni. Melbourne M.J. Boland, B.C.C. Cowie, R. Dowd, Y.-R.E.
Energy-Filtered Transmission Electron Microscope (EFTEM)
NATIONAL SYNCHROTRON RADIATION CENTRE SOLARIS JAGIELLONIAN UNIVERSITY, KRAKOW, POLAND Piotr Goryl Tango Collaboration Meeting, Elettra,
Polarization Dependence in X-ray Spectroscopy and Scattering
National SYNCHROTRON Radiation Centre SOLARIS Jagiellonian University, Krakow, Poland Piotr Goryl Motion Workshop, Soleil,
Improving & combining the spatiale & temporal resolution
Elettra Sincrotrone Trieste
X-ray photoemission electron microscopy (XPEEM)
Introduction to Synchrotron Radiation
X-ray Correlation Spectroscopy (WBS 1.4) Aymeric Robert
Exploring the limits of hybrid pixel detectors with MÖNCH
Practical Absorbance and Fluorescence Spectroscopy
XAFS Spectroscopy Katarina Norén 23/11/2018.
Coherent X-ray Imaging Instrument WBS 1.3
Scope Setting Meeting MIRACLES
X-Ray Endstation Systems (XES) 2006 Schedule
CLIC luminosity monitoring/re-tuning using beamstrahlung ?
Presentation transcript:

IFAE-ALBA | Alba, 13 th December, 2012BL29 - BOREAS 1 of 20 BOREASBORE AS BOREAS, Beamline Of REsonant Absorption and Scattering: status report Javier Herrero Contributions from M. Valvidares, E. Pellegrin, P. Gargiani “Boreas running”, (460 b.c., Yale Univ.)

IFAE-ALBA | Alba, 13 th December, 2012BL29 - BOREAS 2 of 20 General view

IFAE-ALBA | Alba, 13 th December, 2012BL29 - BOREAS 3 of 20 Full x-ray polarization control (APPLE-II undulator) eV energy range (~soft) Variable x-ray beam size and focal distance (KB system) (ES1) High-field SC vector magnet: 6T, 2T with 1.5K-370K sample temp. (ES2) UHV scattering chamber, 2T magnet, large angular access, 20K-350K Beamline designed for soft x-ray polarization-dependent spectroscopy & scattering highlights optical layout BL overview – scientific case & optical layout

IFAE-ALBA | Alba, 13 th December, 2012BL29 - BOREAS 4 of 20 E resolution with MEG BL optics – photon energy resolution -Instrumental resolution (E/  E) ~ 10,000 -Instrumental resolution (E/  E) ~ 10,000 for typically used 15/15 µm (entrance/exit) slits opening Photon flux with MEG) -Flux varying from to sample (depending on E)

IFAE-ALBA | Alba, 13 th December, 2012BL29 - BOREAS 5 of 20 “HECTOR” 6 Tesla UHV - Running full experiments since May 2012Scope - X-ray absorption measurements with: a) variable polarization incoming light b) variable sample temperature c) variable applied magnetic field Detection systems: - Electron drain sample - working - Si diode (transmission mode) - working - Si diode (total fluorescence yield) - in progress (Si diodes made by IRD, model AXUV100) Detection, planned: - Si drift diode (or other) (partial fluorescence yield) BL endstations – XMCD cryomagnet Requirements: E window selection, E range ca eV

IFAE-ALBA | Alba, 13 th December, 2012BL29 - BOREAS 6 of 20 BL endstations– Scattering chamber “MaReS” endstation concept. Expected  end 2013 In-vacuum CCD by XCAM (CFT awarded) In-vacuum magnet

IFAE-ALBA | Alba, 13 th December, 2012BL29 - BOREAS 7 of 20 “MaReS” endstation concept Expected  end 2013 In-vacuum CCD by XCAM (CFT awarded) 2D detection upgrade project Alternatives for 2D detection - Backthinned CMOS (comercially unavailable for soft x-rays when decission on CCD taken) Requirements: large dynamic range, fast reading time, UHV compatible Foreseen Detection systems: a) Point detection (~“0D”) - Si diode, from “IRD”, model SXUV700 - GaAsP diode, from “Hamamatzu” - Channeltron (for high E, photon counting) a) Spatially resolved detection (2D) - Microchannel plate, from “Hamamatzu” - CCD by “e2v”, 2k x 2k pixel, 20 micron pixel size; “XCAM” mouting (awarded)