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SAXS and SANS facilities and experimental practice Clement Blanchet - PowerPoint PPT Presentation

SAXS and SANS facilities and experimental practice Clement Blanchet EMBL Hamburg Small Angle Scattering experiment Detector Sample X-ray or neutron 2 2 Beam s Buffer The beam hits the sample, X-rays/neutrons interact with the


  1. SAXS and SANS facilities and experimental practice Clement Blanchet – EMBL Hamburg

  2. Small Angle Scattering experiment Detector Sample X-ray or neutron 2 θ 2 θ Beam s Buffer The beam hits the sample, X-rays/neutrons interact with the sample and are scattered, providing structural information on the sample. Same formalism but different scattered particles  Different instrument. 10/15/2019 SAXS and SANS facilities 2 Clement Blanchet

  3. Outline • X-rays / neutrons • SAS instruments • Sample environment • Sample requirements and collection strategy 10/15/2019 SAXS and SANS facilities 3 Clement Blanchet

  4. X-rays and neutrons 10/15/2019 SAXS and SANS facilities 4 Clement Blanchet

  5. X-rays Roengten, 1895 10/15/2019 SAXS and SANS facilities 5 Clement Blanchet

  6. Electromagnetic wave 10/15/2019 SAXS and SANS facilities 6 Clement Blanchet

  7. How are X-ray produced? • Brehmstrahlung – When a charge is accelerated charge, electromagnetic radiation is produced 10/15/2019 SAXS and SANS facilities 7 Clement Blanchet

  8. X-ray sources - Synchrotron • Synchrotrons 10/15/2019 SAXS and SANS facilities 8 Clement Blanchet

  9. X-ray sources - synchrotron • Synchrotron radiation – Insertion devices 10/15/2019 SAXS and SANS facilities 9 Clement Blanchet

  10. Insertion devices Undulator (PetraIII) Dipole bending magnet (APS) 10/15/2019 SAXS and SANS facilities 10 Clement Blanchet

  11. Synchrotrons around the world 10/15/2019 SAXS and SANS facilities 11 Clement Blanchet

  12. X-ray sources - FEL • Free electron laser – Electrons are accelerated and send into a long undulator (several 100s meters) – Self amplified spontaneous emission: electrons group themselves into small bunches. – Production of very short and intense X-ray pulses 10/15/2019 SAXS and SANS facilities 12 Clement Blanchet

  13. X-ray sources - FEL • Free electron laser 10/15/2019 SAXS and SANS facilities 13 Clement Blanchet

  14. Lab sources 10/15/2019 SAXS and SANS facilities 14 Clement Blanchet

  15. Lab sources • Principle : electrons, produced by heating a cathode are accelerated in an electric field and projected on a metallic anode. – Brehmstrahlung – Fluorescence 10/15/2019 SAXS and SANS facilities 15 Clement Blanchet

  16. X-ray sources • Lab source (rotating anode, liquid jet) 10/15/2019 SAXS and SANS facilities 16 Clement Blanchet

  17. 10/15/2019 SAXS and SANS facilities 17 Clement Blanchet

  18. Neutron James Chadwick λ= h/mv 10/15/2019 SAXS and SANS facilities 18 Clement Blanchet

  19. Neutron production • Nuclear reaction 10/15/2019 SAXS and SANS facilities 19 Clement Blanchet

  20. Neutron production • Spallation source – Accelerated protons hit a heavy metal target. 10/15/2019 SAXS and SANS facilities 20 Clement Blanchet

  21. Neutrons Facilities 10/15/2019 SAXS and SANS facilities 21 Clement Blanchet

  22. SAXS and SANS Instruments 10/15/2019 SAXS and SANS facilities 22 Clement Blanchet

  23. Optics Monochromatic Polychromatic focused (parallel) divergent beam beam for SAS from the source 10/15/2019 SAXS and SANS facilities 23 Clement Blanchet

  24. Monochromatic X-ray • Bragg diffraction on a crystal n λ = 2 d sin θ 10/15/2019 SAXS and SANS facilities 24 Clement Blanchet

  25. Monochromator • Before • Polychromatic • After • One wavelength + harmonics 10/15/2019 SAXS and SANS facilities 25 Clement Blanchet

  26. Focusing/low divergence 2 θ 2 θ • Small beam at the detector position • Small beam at the sample position 10/15/2019 SAXS and SANS facilities 26 Clement Blanchet

  27. Focusing X-ray • Compound refractive lenses • X-ray mirrors 10/15/2019 SAXS and SANS facilities 27 Clement Blanchet

  28. Focusing X-ray • Focussing mirror 1,0 • Reflectivity 0,8 Transmission 0,6 0.15 Degree 0.25 Degree 0,4 1 Degree 0,2 0,0 10000 Energy [eV] 10/15/2019 SAXS and SANS facilities 28 Clement Blanchet

  29. Focussing mirror – harmonics filter Monochromatic, focused x-ray beam 10/15/2019 SAXS and SANS facilities 29 Clement Blanchet

  30. Monochromatic neutrons • De Broglie equation: λ=h/mv The wavelength of a neutron is related to its velocity. • Velocity selector ∆λ/λ =5-10% • For pulsed source, TOF 10/15/2019 SAXS and SANS facilities 30 Clement Blanchet

  31. Collimation neutrons • The collimator is used to obtain a parallel beam 10/15/2019 SAXS and SANS facilities 31 Clement Blanchet

  32. Get rid of parasitic scattering: slits Beam defining slits Guard or anti-scatter slits

  33. Hybrid slits • Idea: use a crystal for the tip of the blade:  no scattering but diffraction 10/15/2019 SAXS and SANS facilities 33 Clement Blanchet

  34. Hybrid slits • On the P12 beamline 10/15/2019 SAXS and SANS facilities 34 Clement Blanchet

  35. Sample environment 10/15/2019 SAXS and SANS facilities 35 Clement Blanchet

  36. Flight tube 10/15/2019 SAXS and SANS facilities 36 Clement Blanchet

  37. Beamstop • Prevent the direct beam from hitting the detector – Big enough to stop the direct beam – Small enough to collect the small angle • Measure transmitted beam 10/15/2019 SAXS and SANS facilities 37 Clement Blanchet

  38. Active Beamstop • SAXS images needs to be accurately scaled to allow for proper buffer subtraction and extraction of the solute SAXS pattern 10/15/2019 SAXS and SANS facilities 38 Clement Blanchet

  39. Detectors Gas detector X-ray film X-rays ionize a gas (argon) producing of ions and free X-rays interacts with silver halide crystals, electrons. electrons are produced by photoelectric effect. A voltage applied to the gas chamber, ions and electrons They gather around crystal defects, dragging the are moved in opposite direction and produce a detectable silver atoms that can be revealed during the current. development phase. 10/15/2019 SAXS and SANS facilities 39 Clement Blanchet

  40. Photostimulated luminescence X-rays interacts electrons of a photostimulable phosphore plate. After exposure, the electrons are trapped in a high energy state. They can be untrapped by laser illumination and go back to their initial state. While doing so, they produce light that can be detected

  41. Hybrid pixel detectors • Each pixel is readout individually: – No readout noise – Fast readout – high frame rate – High dynamic range

  42. Pilatus Eiger 10/15/2019 SAXS and SANS facilities 42 Clement Blanchet

  43.  Count rate capability 10 7 photons/s/pixel  High spatial resolution with 75 µm pixel size  Kilohertz frame rate with dead-time-free readout  Two energy discriminating thresholds  Gateable detection for pump & probe experiments  Large active area for wide angular coverage  Single-pixel point-spread function  No readout noise or dark current  Compact housing  Room temperature operation of all components 10/15/2019 SAXS and SANS facilities 43 Clement Blanchet

  44. Up to 2000 Hz for smaller detectors 10/15/2019 SAXS and SANS facilities 44 Clement Blanchet

  45. Neutron detection • He3 detector: n + 3 He → 3 H + 1 H + 0.764 MeV 10/15/2019 SAXS and SANS facilities 45 Clement Blanchet

  46. Sample environment 10/15/2019 SAXS and SANS facilities 46 Clement Blanchet

  47. Samples SAS applicable to many type of samples. Metal alloys Sufactants Tissues Polymers Nanomagnetic materials Bio-macromolecules in solution 10/15/2019 SAXS and SANS facilities 47 Clement Blanchet

  48. Sample environment Heating stages Magnetic field system Rapid mixing device Sample changers Example ID02 (ESRF) multipurpose beamline 10/15/2019 SAXS and SANS facilities 48 Clement Blanchet

  49. Sample environment • Bio-macromolecules in solution are weakly scattering sample. • For biological macromolecules in solution: – fragile – Preferably in vacuum – Thermostated 10/15/2019 SAXS and SANS facilities 49 Clement Blanchet

  50. Sample cell • Cell material: low absorption and scattering – Mica, quartz, polycarbonate • Sample thickness (t): compromise between scattering and absorption – Scattering α t – absorption α exp(-ut) • For neutron, cell are rather thin (<1mm to avoid multiple scattering) 10/15/2019 SAXS and SANS facilities Clement Blanchet 50

  51. Solution SAXS 15 years ago: Manual sample loading  Buffer and sample should be measured in the same cell  Difficult to implement in vacuum  10-15 minutes per measurement  High sample consumption  Non-optimized cleaning procedure  Tedious, energy and attention consuming 10/15/2019 SAXS and SANS facilities 51 Clement Blanchet

  52. SAXS sample changer @EMBL Hamburg 10/15/2019 SAXS and SANS facilities 52 Clement Blanchet

  53. SAXS sample changer 10/15/2019 SAXS and SANS facilities 53 Clement Blanchet

  54. Sample changer performances • Large storage capacity • Full cycle time (loading, exposure, flushing, cleaning, drying) ≈ 1 min • Volume 5-20 microliter • Very efficient cleaning • Flow measurement 10/15/2019 SAXS and SANS facilities 54 Clement Blanchet

  55. Online size exclusion column 10/15/2019 SAXS and SANS facilities 55 Clement Blanchet

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